# pdgfootnote

pdgid: S046SNU
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ALEXANDER 1991F limit is for one species of nutilde and is derived from Gamma(invisible, new)/Gamma(lepton lepton) <0.38.


pdgid: S046SE
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AAD 2023M searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for  leptontilde+- pair production, followed by leptontilde+- --> lepton+- chitilde_1()0 in  events with two leptons. The focus is on models  where mass(leptontilde+-) -  mass(chitilde_{{1}}()0) is close to the W mass. No significant excess above the Standard Model  predictions is observed. Limits were set on the leptontilde mass (assuming  etilde-mutilde and L-R degeneracy), as a function of  mass(chitilde_{{1}}()0), see   Figure 6. Limits were also derived for single etilde or  mutilde, and for L and R  independently, see Figure 7.


pdgid: S046SE
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AAD 2020O reported on a search for electroweak production in models with charginos and  sleptons decaying into final states with exactly two oppositely charged leptons and missing  transverse momentum. A dataset of p p collisions at sqrt(s) = 13 TeV corresponding to an  integrated luminosity of 139 fb^{-1} was used.  Light-flavour sleptons etilde and mutilde  are constrained at 95% C.L. to have masses above 700 GeV for massless lightest neutralino,  see their Fig. 7(c).  Exclusion limits are also set for selectrons and smuons separately,  considering either right- or left-handed components, by including only the di-electron and di-muon  same-flavour signal regions defined in the search, see their Fig. 8.


pdgid: S046SE
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SIRUNYAN 2019AW searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  direct electroweak pair production of selectrons or smuons in events with two leptons (electrons or  muons) of the opposite electric charge and same flavour, no jets and large notET. No  significant excess above the Standard Model expectations is observed. Limits are set on the  selectron mass assuming left-handed, right-handed or both left- and right-handed (mass degenerate)  production, see their Figure 6. Similarly, limits are set on the smuon mass, see their Figure 7.   Limits are also set on slepton masses under the assumption that the selectron and smuon are mass  degenerate, see their Figure 5.


pdgid: S046SE
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AABOUD 2018BT searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  direct electroweak production of charginos, chargino and next-to-lightest neutralinos and sleptons  in events with two or three leptons (electrons or muons), with or without jets, and large missing  transverse energy. No significant excess above the Standard Model expectations is observed. Limits  are set on the slepton mass up to 500 GeV for massless chitilde_{{1}}()0, assuming degeneracy of  etilde, mutilde, and tautilde and exploiting the 2lepton signature, see their  Figure 8(b).


pdgid: S046SE
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AABOUD 2018R searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  electroweak production in scenarios with compressed mass spectra in final states with two  low-momentum leptons and missing transverse momentum. The data are found to be consistent with the  SM prediction. Results are interpreted in slepton pair production models with a fourfold degeneracy  assumed in selectron and smuon masses. The etilde masses are excluded up to 190 GeV for mass(etilde) - mass(chitilde_{{1}}()0) = 5 GeV.  The exclusion limits extend down to mass  splittings of 1 GeV, see their Fig. 11.


pdgid: S046SE
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CHATRCHYAN 2014R searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least three leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the slepton mass in a stau (N)NLSP simplified model (GMSB) where the decay leptontilde --> lepton+- tau+- tau-+ Gtilde takes place with a branching ratio of 100%, see Fig. 8.


pdgid: S046SE
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AAD 2013B searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for sleptons decaying to a final state with two leptons (e and mu) and missing transverse energy. No excess beyond the Standard Model expectation is observed. Limits are derived in a simplified model of direct left-handed slepton pair production, where left-handed slepton masses between 85 and 195 GeV are excluded at 95% C.L. for mass(chitilde_{{1}}()0) = 20 GeV. See also Fig. 2(a). Exclusion limits are also derived in the phenomenological MSSM, see Fig. 3.


pdgid: S046SE
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ABBIENDI 2004 search for etilde_R etilde_R production in acoplanar di-electron final states in the 183 -- 208~GeV data. See Fig.13 for the dependence of the limits on mass(chitilde_{{1}}()0) and for the limit at tan(beta)=35 This limit supersedes ABBIENDI 2000G.


pdgid: S046SE
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ACHARD 2004 search for etilde_{{R}}etilde_{{L}} and  etilde_{{R}}etilde_{{R}} production in single- and acoplanar di-electron final states in the 192 -- 209 GeV data. Absolute limits on mass(etilde_{{R}}) are derived from a scan over the MSSM parameter space with universal GUT scale gaugino and scalar masses  and mass(0), 1<=tan(beta)<=60 and -2<=mu<=2 TeV. See Fig.~4 for the dependence of the limits on mass(chitilde_{{1}}()0). This limit supersedes ACCIARRI 1999W.


pdgid: S046SE
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ABDALLAH 2003M looked for acoplanar dielectron +notE final states at sqrt(s) = 189 -- 208 GeV. The limit assumes mu=-200 GeV and tan(beta)=1.5 in the calculation of the production cross section and B(etilde --> e chitilde_1()0). See Fig.~15 for limits in the (mass(etilde_{{R}}), mass(chitilde_{{1}}()0)) plane. These limits include and update the results of ABREU 2001


pdgid: S046SE
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ABDALLAH 2003M uses data from sqrt(s) = 192 -- 208 GeV to obtain limits in the framework of the MSSM with gaugino and sfermion mass universality at the GUT scale. An indirect limit on the mass is derived by constraining the MSSM parameter space by the results from direct searches for neutralinos (including cascade decays) and for sleptons. These limits are valid for values of M(2)<1 TeV, |mu|<=1TeV with the chitilde_{{1}}()0 as LSP. The quoted limit is obtained when there is no mixing in the third family. See Fig.~43 for the mass limits as a function of tan(beta). These limits update the results of ABREU 2000W.


pdgid: S046SE
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HEISTER 2002E looked for acoplanar dielectron + notET final states from e+ e- interactions between 183 and 209 GeV. The mass limit assumes mu<-200 GeV and tan(beta)=2 for the production cross section and B(etilde --> e chitilde_1()0)=1. See their Fig.4 for the dependence of the limit on Delta(m). These limits include and update the results of BARATE 2001.


pdgid: S046SE
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HEISTER 2002N search for etilde_R etilde_L and etilde_R etilde_R production in single- and acoplanar di-electron final states in the 183 -- 208 GeV data.  Absolute limits on mass(etilde_{{R}}) are derived from a scan over the MSSM parameter space with universal GUT scale gaugino and scalar masses m(1/2) and m(0), 1<=tan(beta)<=50 and -10<=mu<=10 TeV.  The region of small |mu|, where cascade decays are important, is covered by a search for chitilde_1()0 chitilde_3()0 in final states with leptons and possibly photons.  Limits on mass(etilde_{{L}}) are derived by exploiting the mass relation between the etilde_{{L}} and etilde_{{R}}, based on universal m(0) and m(1/2). When the constraint from the mass limit of the lightest Higgs from HEISTER 2002 is included, the bounds improve to mass(etilde_{{R}})>77(75) GeV and mass(etilde_{{L}})>115(115) GeV for a top mass of 175(180) GeV.  In the MSUGRA framework with radiative electroweak symmetry breaking, the limits improve further to mass(etilde_{{R}})>95 GeV and mass(etilde_{{L}})>152 GeV, assuming a trilinear coupling A_{{0}}()=0 at the GUT scale.  See Figs.4, 5, 7 for the dependence of the limits on tan(beta).


pdgid: S046SE
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AAD 2020I reported on ATLAS searches for slepton pair production in models with compressed  mass spectra. A dataset of p p collisions at sqrt(s) = 13 TeV corresponding to an integrated  luminosity of 139 fb^{-1} was used. Events with notET, two same-flavour, opposite-charge,  low-transverse-momentum leptons, and jets from initial-state radiation or characteristic of  vector-boson fusion production are selected. Light-flavour sleptons etilde and mutilde are  constrained at 95% C.L. to have masses above 251 GeV for a mass splitting  slepton-chitilde_{{1}}()0  of 10 GeV,  with constraints extending down to mass splittings of  550 MeV at the LEP slepton limits (73 GeV), see their Fig. 16(a). If only selectrons are  considered, and etilde = etilde_{{R}}, masses below 101 GeV are excluded for mass splitting  etilde_{{R}}, chitilde_{{1}}()0 of 7.5 GeV. See their Fig. 16(b).


pdgid: S046SE
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AAD 2020I reported on ATLAS searches for slepton pair production in models with compressed  mass spectra. A dataset of p p collisions at sqrt(s) = 13 TeV corresponding to an integrated  luminosity of 139 fb^{-1} was used. Events with notET, two same-flavour, opposite-charge,  low-transverse-momentum leptons, and jets from initial-state radiation or characteristic of  vector-boson fusion production are selected.  Light-flavour sleptons etilde and mutilde are  constrained at 95% C.L. to have masses above 251 GeV for a mass splitting  slepton-chitilde_{{1}}()0  of 10 GeV,  with constraints extending down to mass splittings of  550 MeV at the LEP slepton limits (73 GeV). See their Fig. 16(a). If only selectron are considered,  and etilde = etilde_{{L}}, masses below 169 GeV are excluded for mass splitting etilde_{{L}},  chitilde_{{1}}()0 of 7.1 GeV. See their Fig. 16(b).


pdgid: S046SE
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AAD 2014G searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for electroweak production of slepton pairs, decaying to a final sate with two leptons (e and mu) and missing transverse momentum. No excess beyond the Standard Model expectation is observed. Exclusion limits are derived in simplified models of slepton pair production, see Fig. 8. An interpretation in the pMSSM is also given, see Fig. 10.


pdgid: S046SE
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KHACHATRYAN 2014I searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for electroweak production of slepton pairs decaying to a final state with opposite-sign lepton pairs (e or mu) and missing transverse momentum. No excess beyond the Standard Model expectation is observed. Exclusion limits are derived in simplified models, see Fig. 18.


pdgid: S046SEV
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AAD 2014X searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least four leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the slepton mass in an R-parity violating simplified model where the decay leptontilde --> lepton chitilde_1()0, with chitilde_1()0 --> lepton+- lepton-+ nu, takes place with a branching ratio of 100%, see Fig. 9.


pdgid: S046SEV
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ABBIENDI 2004F use data from sqrt(s) = 189 -- 209~GeV. They derive limits on sparticle masses under the assumption of RPV with L L Ebar or L Q Dbar couplings. The results are valid for tan(beta) = 1.5, mu = -200~GeV, with, in addition, Delta(m) > 5~GeV for indirect decays via L Q Dbar. The limit quoted applies to direct decays via L L Ebar or L Q Dbar couplings. For indirect decays, the limits on the etilde_{{R}} mass are respectively 99 and 92~GeV for L L Ebar and L Q Dbar couplings and mass(chitilde()0) = 10~GeV and degrade slightly for larger chitilde_{{1}}()0 mass. Supersedes the results of ABBIENDI 2000.


pdgid: S046SEV
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ABDALLAH 2004M use data from sqrt(s) = 192 -- 208~GeV to derive limits on sparticle masses under the assumption of RPV with L L Ebar or Ubar Dbar Dbar couplings. The results are valid for mu = -200~GeV, tan(beta) = 1.5, Delta(m) > 5~GeV and assuming a BR of 1 for the given decay. The limit quoted is for indirect Ubar Dbar Dbar decays using the neutralino constraint of 39.5 GeV for L L Ebar and of 38.0 GeV for Ubar Dbar Dbar couplings, also derived in ABDALLAH 2004M. For indirect decays via L L Ebar the limit improves to 95 GeV if the constraint from the neutralino is used and to 94 GeV if it is not used. For indirect decays via Ubar Dbar Dbar couplings it remains unchanged when the neutralino constraint is not used. Supersedes the result of ABREU 2000U.


pdgid: S046SMU
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AAD 2023CR searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for RPV SUSY  in final states with multiple leptons and b-tagged jets. No significant excess above the Standard  Model expectations is observed.  Limits are set on the production of electroweakinos (wino or  higgsino) that decay via RPV coupling lambda_{{i33}}^' to a charged lepton or a neutrino, a b  quark, and an additional t or b quark, see their figure 16. A second model addresses direct  mutilde_{{L,R}} production and decay to a muon and a bino-like neutralino, which decays in the same  way as in the first model, see their figure 17.


pdgid: S046SMU
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AAD 2023M searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for    leptontilde+- pair production, followed by leptontilde+- --> lepton+- chitilde_1()0 in    events with two leptons. The focus is on models  where mass(leptontilde+-) -  mass(chitilde_{{1}}()0) is close to the W mass. No significant excess above the Standard Model    predictions is observed. Limits were set on the leptontilde mass (assuming     etilde-mutilde and L-R degeneracy), as a function of  mass(chitilde_{{1}}()0), see    Figure 6. Limits were also derived for single etilde or  mutilde, and for L and R independently, see Figure 7.


pdgid: S046SMU
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AAD 2020I reported on ATLAS searches for slepton pair production in models with compressed  mass spectra. A dataset of p p collisions at sqrt(s) = 13 TeV corresponding to an integrated  luminosity of 139 fb^{-1} was used. Events with notET, two same-flavour, opposite-charge,  low-transverse-momentum leptons, and jets from initial-state radiation or characteristic of  vector-boson fusion production are selected. Light-flavour sleptons etilde and mutilde are  constrained at 95% C.L. to have masses above 251 GeV for a mass splitting  slepton-chitilde_{{1}}()0 of 10 GeV, with constraints extending down to mass splittings of  550 MeV at the LEP slepton limits (73 GeV). See their Fig. 16(a). If only smuon are considered, and  mutilde = mutilde_{{R}}, masses below 150 GeV are excluded for mass splitting mutilde_{{R}},  chitilde_{{1}}()0 of 8.2 GeV. See their Fig. 16(b).


pdgid: S046SMU
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AAD 2020I reported on ATLAS searches for slepton pair production in models with compressed  mass spectra. A dataset of p p collisions at sqrt(s) = 13 TeV corresponding to an integrated  luminosity of 139 fb^{-1} was used. Events with notET, two same-flavour, opposite-charge,  low-transverse-momentum leptons, and jets from initial-state radiation or characteristic of  vector-boson fusion production are selected.  Light-flavour sleptons etilde and mutilde are  constrained at 95% C.L. to have masses above 251 GeV for a mass splitting  slepton-chitilde_{{1}}()0  of 10 GeV,  with constraints extending down to mass splittings of  550 MeV at the LEP slepton limits (73 GeV). See their Fig. 16(a). If only smuon are considered, and  mutilde = mutilde_{{L}}, masses below 216 GeV are excluded for mass splitting mutilde_{{L}},  chitilde_{{1}}()0 of 10 GeV. See their Fig. 16(b).


pdgid: S046SMU
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AABOUD 2018R searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  electroweak production in scenarios with compressed mass spectra in final states with two  low-momentum leptons and missing transverse momentum. The data are found to be consistent with the  SM prediction. Results are interpreted in slepton pair production models with a fourfold degeneracy  assumed in selectron and smuon masses. The mutilde masses are excluded up to 190 GeV for mass(mutilde) - mass(chitilde_{{1}}()0) = 5 GeV.  The exclusion limits extend down to mass  splittings of 1 GeV, see their Fig. 11.


pdgid: S046SMU
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ABBIENDI 2004 search for mutilde_R mutilde_R production in acoplanar di-muon final states in the 183 -- 208~GeV data. See Fig.14 for the dependence of the limits on mass(chitilde_{{1}}^0()) and for the limit at tan(beta)=35. Under the assumption of 100% branching ratio for mutilde_R --> mu~chitilde_{{1}}()0, the limit improves to 94.0 GeV for Delta(m)> 4GeV. See Fig.~11 for the dependence of the limits on m(chitilde_{{1}}()0) at several values of the branching ratio. This limit supersedes ABBIENDI 2000G.


pdgid: S046SMU
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ACHARD 2004 search for mutilde_{{R}}mutilde_{{R}} production in acoplanar di-muon final states in the 192 -- 209 GeV data. Limits on mass(mutilde_{{R}}) are derived from a scan over the MSSM parameter space with universal GUT scale gaugino and scalar masses  and mass(0), 1<=tan(beta)<=60 and -2<=mu<=2 TeV. See Fig.~4 for the dependence of the limits on mass(chitilde_{{1}}()0). This limit supersedes ACCIARRI 1999W.


pdgid: S046SMU
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ABDALLAH 2003M looked for acoplanar dimuon +notE final states at sqrt(s) = 189 -- 208 GeV. The limit assumes B(mutilde --> mu chitilde_1()0) = 100%. See Fig.~16 for limits on the (mass(mutilde_{{R}}), mass(chitilde_{{1}}()0)) plane. These limits include and update the results of ABREU 2001.


pdgid: S046SMU
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HEISTER 2002E looked for acoplanar dimuon + notET final states from e+ e- interactions between 183 and 209 GeV. The mass limit assumes  B(mutilde --> mu chitilde_1()0)=1. See their Fig.4 for the dependence of the limit on Delta(m). These limits include and update the results of BARATE 2001.


pdgid: S046SMU
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ABREU 2000V use data from sqrt(s)= 130 -- 189 GeV to search for tracks with large impact parameter or visible decay vertices. Limits are obtained as function of mass(Gtilde), after combining these results with the search for slepton pair production in the SUGRA framework from ABREU 2001 to cover prompt decays and on stable particle searches from ABREU 2000Q.  For limits at different mass(Gtilde), see their Fig.12.


pdgid: S046SMV
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AAD 2022E searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for   supersymmetry by measuring the yield asymmetry between events containing e- mu+ and those   containing e+ mu-. This was found in agreement with the standard model prediction of 1.  Limits  are set on the RPV production of t mutilde_L events with mutilde_L --> mu chitilde_1()0 for   various values of   lambda_{{231}}^', see their figures 6 and 7.


pdgid: S046SMV
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ABDALLAH 2004M use data from sqrt(s) = 192 -- 208~GeV to derive limits on sparticle masses under the assumption of RPV with L L Ebar or Ubar Dbar Dbar couplings. The results are valid for mu = -200~GeV, tan(beta) = 1.5, Delta(m) > 5~GeV and assuming a BR of 1 for the given decay. The limit quoted is for indirect Ubar Dbar Dbar decays using the neutralino constraint of 39.5 GeV for L L Ebar and of 38.0 GeV for Ubar Dbar Dbar couplings, also derived in ABDALLAH 2004M. For indirect decays via L L Ebar the limit improves to 90 GeV if the constraint from the neutralino is used and remains at 87 GeV if it is not used. For indirect decays via Ubar Dbar Dbar couplings it degrades to 85 GeV when the neutralino constraint is not used. Supersedes the result of ABREU 2000U.


pdgid: S046SMV
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HEISTER 2003G searches for the production of smuons in the case of RPV prompt decays with LLEbar, LQDbar or UbarDbarDbar couplings at sqrt(s) = 189 -- 209GeV. The search is performed for direct and indirect decays, assuming one coupling at a time to be non-zero. The limit holds for direct decays mediated by RPV LQDbar couplings and improves to 90 GeV for indirect decays (for Delta(m)> 10 GeV). Limits are also given for LLEbar direct (mass(mutildeR) > 87~GeV) and indirect decays (mass(mutildeR) > 96 GeV for m(chitilde_{{1}}()0) > 23 GeV from BARATE 1998S) and for UbarDbarDbar indirect decays (mass(mutildeR) > 85 GeV for Delta(m)> 10 GeV). Supersedes the results from BARATE 2001B.


pdgid: S046STA
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TUMASYAN 2023AG searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  or direct pair production of tau sleptons in events with two hadronically decaying tau leptons. No  significant excess above the Standard Model expectations is observed. Limits are set on the mass of  the tau slepton in models with tautilde --> tau chitilde_1()0 for mass-degenerate, pure  left-handed and pure right-handed tau sleptons, see their figures 4 -- 7. Limits are also  set for the maximally mixed scenario with long-lived tau sleptons and tautilde lifetimes of  0.01 mm to 2.5 mm, see their figure 8.


pdgid: S046STA
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AAD 2020H presented ATLAS searches for direct production for tautilde in final states  with two hadronically decaying leptons and notET. The analysis uses a dataset of p p  collisions at sqrt(s) = 13 TeV corresponding to an integrated luminosity of 139 fb^{-1}.  Exclusion limits at 95% C.L. are derived in scenarios of direct production of tautilde  pairs with each tautilde decaying into a tau and the lightest neutralino chitilde_{{1}}()0  in simplified models where the tautilde_{{R}} and tautilde_{{L}} mass eigenstates are degenerate.  Stau masses from 120GeV to 390GeV are excluded for a massless lightest neutralino, see their Fig.  7(a).  If tautilde_{{L}}-only pair production is considered, the exclusion region extends between  155 GeV to 310 GeV, see their Fig. 7(b).


pdgid: S046STA
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SIRUNYAN 2020P searched in 77.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  direct pair production of  tau sleptons in events with a tau lepton pair and significant missing  transverse momentum. Final states with two double hadronic decay of the tau leptons are considered,  as well as where one of the tau leptons decays into an electron or a muon.  No significant excess  above the Standard Model expectations is observed.  Limits are set on the stau mass in a simplified  models where two tau sleptons are pair produced and decay to a tau lepton and the lightest  neutralino, assuming either only left-handed stau production,  see Figure 8, or assuming degenerate  left- and right-handed stau production, see Figure 9.


pdgid: S046STA
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ABBIENDI 2004 search for tautilde tautilde production in acoplanar di-tau final states in the 183 -- 208~GeV data. See Fig.15 for the dependence of the limits on mass(chitilde_{{1}}^0()) and for the limit at tan(beta)=35. Under the assumption of 100% branching ratio for tautilde_R --> tau~chitilde_{{1}}()0, the limit improves to 89.8~GeV for Delta(m)> 8GeV. See Fig.~12 for the dependence of the limits on m(chitilde_{{1}}()0) at several values of the branching ratio and for their dependence on theta(tau). This limit supersedes ABBIENDI 2000G.


pdgid: S046STA
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ACHARD 2004 search for tautildetautilde production in acoplanar di-tau final states in the 192 -- 209 GeV data. Limits on mass(tautilde_{{R}}) are derived from a scan over the MSSM parameter space with universal GUT scale gaugino and scalar masses  and mass(0), 1 <=tan(beta)<=60 and -2<=mu<= 2 TeV. See Fig.~4 for the dependence of the limits on mass(chitilde_{{1}}()0).


pdgid: S046STA
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ABDALLAH 2003M looked for acoplanar ditaus +notE final states at sqrt(s) = 130 -- 208 GeV. A dedicated search was made for low mass tautildes decoupling from the Z0. The limit assumes B(tautilde --> tau chitilde_1()0) = 100%. See Fig.~20 for limits on the (mass(tautilde),mass(chitilde_{{1}}()0)) plane and as function of the chitilde_{{1}}()0 mass and of the branching ratio. The limit in the low-mass region improves to 29.6 and 31.1 GeV for tautilde_{{R}} and tautilde_{{L}}, respectively, at Delta(m)> mass(tau). The limit in the high-mass region improves to 84.7GeV for tautilde_{{R}}  and Delta(m)> 15GeV. These limits include and update the results of ABREU 2001.


pdgid: S046STA
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HEISTER 2002E looked for acoplanar ditau + notET final states from e+ e- interactions between 183 and 209 GeV. The mass limit assumes  B(tautilde --> tau chitilde_1()0)=1. See their Fig.4 for the dependence of the limit on Delta(m). These limits include and update the results of BARATE 2001.


pdgid: S046STA
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KHACHATRYAN 2017L searched in about 19 fb^{-1} of p p collisions at sqrt(s) = 8 TeV  for events with two tau (at least one decaying hadronically) and notET. Results were  interpreted to set constraints on the cross section for  production of tautilde_{{L}} pairs for   mass(chitilde_{{1}}()0)=1 GeV. No mass constraints are set, see their Fig. 7.


pdgid: S046STA
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AAD 2016AA summarized and extended ATLAS searches for electroweak supersymmetry in final  states containing several charged leptons, notET, with or without hadronic jets, in 20  fb^{-1} of p p collisions at sqrt(s) = 8 TeV. The paper reports 95% C.L. exclusion  limits on the cross-section for production  of tautilde_{{R}} and tautilde_{{L}} pairs for various  mass(chitilde_{{1}}()0), using the 2 hadronic tau + notET analysis.  The mass(tautilde_{{R/L}})  = 109 GeV is excluded for mass(chitilde_{{1}}()0) = 0 GeV, with the constraints being stronger for  tautilde_{{R}}. See their Fig. 12.


pdgid: S046STA
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AAD 2012AF searched in 2 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events  with two tau leptons, jets and  large notET in a GMSB framework. No significant excess above the expected background was found and an upper limit on the  visible cross section for new phenomena is set. A 95% C.L. lower limit of 32 TeV on the mGMSB breaking scale Lambda is set for M_{{mess}}() = 250 TeV, N_{{S}}() = 3, mu > 0 and C_{{grav}}() = 1, independent of tan(beta).


pdgid: S046STA
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AAD 2012AG searched in 2.05 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events  with at least one hadronically decaying tau lepton, jets, and large notET in a GMSB framework. No significant excess above the expected background was found and an upper limit on the visible cross section for new phenomena is set. A 95%  C.L. lower limit of 30 TeV on the mGMSB breaking scale Lambda is set for M_{{mess}}() = 250 TeV, N_{{S}}() = 3, mu > 0 and C_{{grav}}() = 1, independent of tan(beta). For large values of tan(beta), the limit on Lambda increases to 43 TeV.


pdgid: S046STA
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AAD 2012CM searched in 4.7 fb**-1 of p p collisions at sqrt(s)=7 TeV for events  with at least one tau lepton, zero or one additional light lepton (e/mu) jets, and  large notET in a GMSB framework. No significant excess above the expected background was found and an upper limit on the visible cross section for new phenomena is set. A 95%  C. L. lower limit of 54 TeV on the mGMSB breaking scale Lambda is set for M_{{mess}} = 250 TeV, N_{{S}} = 3, mu > 0 and C_{{grav}} = 1, for tan(beta) > 20. Here the tautilde_{{1}} is the NLSP.


pdgid: S046STA
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ABBIENDI 2006B use 600 pb**-1 of data from sqrt(s) = 189 -- 209 GeV. They look  for events from pair-produced staus in a GMSB scenario with tautilde NLSP including prompt  tautilde decays to ditaus + notE final states, large impact parameters, kinked tracks  and heavy stable charged particles. Limits on the cross-section are computed as a function of  m(tautilde) and the lifetime, see their Fig. 7. The limit is compared to the  sigma.BR**2 from a scan over the GMSB parameter space.


pdgid: S046STA
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ABDALLAH 2004H use data from LEP~1 and sqrt(s) = 192 -- 208~GeV. They re-use results or re-analyze the data from ABDALLAH 2003M to put limits on the parameter space of anomaly-mediated supersymmetry breaking (AMSB), which is scanned in the region 1<m(3/2)<50~TeV, 0<m_{{0}}()<1000~GeV, 1.5<tan(beta)<35, both signs of mu. The constraints are obtained from the searches for mass degenerate chargino and neutralino, for SM-like and invisible Higgs, for leptonically decaying charginos and from the limit on non-SM Z width of 3.2~MeV. The limit is for mass(t) = 174.3~GeV (see Table 2 for other mass(t) values). The limit improves to 75 GeV for mu < 0.


pdgid: S046STU
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ABDALLAH 2004M use data from sqrt(s) = 192 -- 208~GeV to derive limits on sparticle masses under the assumption of RPV with L L Ebar couplings. The results are valid for mu = -200~GeV, tan(beta) = 1.5, Delta(m) > 5~GeV and assuming a BR of 1 for the given decay. The limit quoted is for indirect decays using the neutralino constraint of 39.5 GeV, also derived in ABDALLAH 2004M. For indirect decays via L L Ebar the limit decreases to 86 GeV if the constraint from the neutralino is not used. Supersedes the result of ABREU 2000U.


pdgid: S046STU
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ABBIENDI 2004F use data from sqrt(s) = 189 -- 209~GeV. They derive limits on sparticle masses under the assumption of RPV with L L Ebar or L Q Dbar couplings. The results are valid for tan(beta) = 1.5, mu = -200~GeV, with, in addition, Delta(m) > 5~GeV for indirect decays via L Q Dbar. The limit quoted applies to direct decays with L L Ebar couplings and improves to 75~GeV for L Q Dbar couplings. The limit on the tautilde_{{R}} mass for indirect decays is 92~GeV for L L Ebar couplings at mass(chitilde()0) = 10~GeV and no exclusion is obtained for L Q Dbar couplings. Supersedes the results of ABBIENDI 2000.


pdgid: S046SLP
text:
AAD 2023BQ searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of long-lived mutilde() in events with muons with impact parameters in the  millimeter range. No significant excess above the Standard Model predictions is observed. Limits  are set on mass(mutilde) as a function of the mutilde lifetime, assuming the mutilde --> mu Gtilde  decay and mass-degenerate mutilde_{{L}} and mutilde_{{R}}. See Figure 4.


pdgid: S046SLP
text:
AAD 2023G searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for stau pair   production in events with high-pt tracks with large ionisation in the pixel detector. No    significant excess above the Standard Model predictions is observed. Limits are set on the stau   mass as a function of its lifetime, see  Figure 19.


pdgid: S046SLP
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TUMASYAN 2023AG searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for or  direct pair production of tau sleptons in events with two hadronically decaying tau leptons. No  significant excess above the Standard Model expectations is observed. Limits are set for the  maximally mixed scenario with long-lived tau sleptons and tautilde lifetimes of 0.01 mm to 2.5  mm, see their figure 8. Limits are also set on the mass of the tau slepton in models with  tautilde --> tau chitilde_1()0 for mass-degenerate, pure left-handed and pure right-handed tau  sleptons, see their figures 4 -- 7.


pdgid: S046SLP
text:
TUMASYAN 2022AF searched for evidence of new long-lived particles decaying to leptons in p p     collisions at sqrt(s) = 13 TeV, corresponding to 118 (113) fb^{-1}  in the ee channel   (emu   and mu mu) channels. The leptons are required to have transverse impact parameter   values   between 0.01 and 10 cm and are not required to form a common vertex. No significant excess   above   the Standard Model expectations is observed. Limits are set on the mass of the top squark   in RPV   models with top squark pair production and ttilde --> b leptonbar and ttilde --> d leptonbar, see     their Figure 4, which contains a wider range of lifetime limits. Limits are also set on a     gauge-mediated SUSY breaking model, where the next-to-lightest SUSY particle is a slepton and the     lightest SUSY particle a gravitino Gtilde, see their Figure 5, which also contains a wider     range of lifetime limits. Limits are also set in a model that produces BSM Higgs bosons (H)   with a   mass of 125 GeV through gluongluon fusion, where the H decays to two long-lived   scalars S, each of   which decays to two oppositely charged and same-flavor leptons.


pdgid: S046SLP
text:
AAD 2021AL searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV  for pair production of long-lived sleptons  in events with highly displaced leptons. No significant  excess above the Standard Model predictions is observed. Limits are set on mass(etilde()), mass(mutilde()), mass(tautilde()) as a function of the slepton lifetime, assuming the leptontilde --> lepton Gtilde decay and mass-degenerate  leptontilde_{{L}}() and  leptontilde_{{R}}(). See Figures 2.


pdgid: S046SLP
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AABOUD 2019AT searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  metastable and stable R-hadrons. Multiple search strategies for a wide range of lifetimes,  corresponding to path lengths of a few meters, are defined. No significant deviations from the  expected Standard Model background are observed. Results are interpreted in terms of exclusion  limits on long-lived stau in the context of GMSB models. Lower limits on the mass for direct  production of staus are set at 430 GeV, see their Fig. 10 (left).


pdgid: S046SLP
text:
KHACHATRYAN 2016BW searched in 2.5 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events  with heavy stable charged particles, identified by their anomalously high energy deposits  in the silicon tracker and/or long time-of-flight measurements by the muon system. No evidence for  an excess over the expected background is observed. Limits are derived for pair production of tau  sleptons as a function of mass, depending on their direct or inclusive production in a minimal GMSB  scenario along the Snowmass Points and Slopes (SPS) line 7, see Fig. 4 and Table 7.


pdgid: S046SLP
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AAD 2015AE searched in 19.1 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for heavy  long-lived charged particles, measured through their specific ionization energy loss in the ATLAS  pixel detector or their time-of-flight in the ALTAS muon system. In the absence of an excess of  events above the expected backgrounds, limits are set on stable tautilde sleptons in various  scenarios, see Figs. 5-7.


pdgid: S046SLP
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AAIJ 2015BD searched in 3.0 fb^{-1} of p p collisions at sqrt(s) = 7 and 8 TeV for  evidence of Drell-Yan pair production of long-lived tautilde particles. No evidence for such  particles is observed and 95% C.L. upper limits on the cross section of tautilde pair  production are derived, see Fig. 7. In the mGMSB, assuming the SPS7 benchmark scenario tautilde  masses between 124 and 309 GeV are excluded at 95% C.L.


pdgid: S046SLP
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ABBIENDI 2003L used e+ e- data at sqrt(s) = 130 -- 209 GeV to select events with two high momentum tracks with anomalous dE/dx. The excluded cross section is compared to the theoretical expectation as a function of the heavy particle mass in their Fig.~3. The limit improves to 98.5 GeV for mutilde_{{L}} and tautilde_{{L}}. The bounds are valid for colorless spin 0 particles with lifetimes longer than 10**-6s. Supersedes the results from ACKERSTAFF 1998P.


pdgid: S046SLP
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ABREU 2000Q searches for the production of pairs of heavy, charged stable particles in e+ e- annihilation at sqrt(s)= 130 -- 189 GeV.  The upper bound improves to 88 GeV for mutilde_{{L}}, tautilde_{{L}}.  These limits include and update the results of ABREU 1998P.


pdgid: S046SLP
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ACCIARRI 1999H searched for production of pairs of back-to-back heavy charged particles  at sqrt(s)=130 -- 183 GeV. The upper bound improves to 82.2 GeV for mutilde_{{L}}, tautilde_{{L}}.


pdgid: S046SLP
text:
The BARATE 1998K mass limit improves to 82 GeV for mutilde_{{L}},tautilde_{{L}}. Data collected at sqrt(s)=161 -- 184 GeV.


pdgid: S046SLP
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AAD 2013AA searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events containing long-lived massive particles in a GMSB framework. No significant excess above the expected background was found. A 95%  C.L. lower limit of 300 GeV is placed on long-lived tautilde's in the GMSB model with M_{{mess}}() = 250 TeV, N_{{S}}() = 3, mu > 0, for tan(beta) = 5 -- 20. The lower limit on the GMSB breaking scale Lambda was found to be 99 -- 110 TeV, for tan(beta) values between 5 and 40, see Fig. 4 (top). Also, directly produced long-lived sleptons, or sleptons decaying to long-lived ones, are excluded at 95% C.L. up to a tautilde mass of 278 GeV for models with slepton splittings smaller than 50 GeV.


pdgid: S046SLP
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ABAZOV 2013B looked in 6.3 fb**-1 of p pbar collisions at sqrt(s) = 1.96 TeV for charged massive long-lived particles in events with muon-like particles that have both speed and ionization energy loss inconsistent with muons produced in beam collisions. In the absence of an excess, limits are set at 95% C.L. on the production cross section of stau leptons in the mass range 100 -- 300 GeV, see their Table 20 and Fig. 23.


pdgid: S046SLP
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CHATRCHYAN 2013AB limits are derived for pair production of tautilde_{{1}} as a function of mass in minimal GMSB scenarios along the Snowmass Points and Slopes (SPS) line 7 (see Fig. 8 and Table 7). The limit given here is valid for direct pair tautilde_{{1}} production.


pdgid: S046SLP
text:
CHATRCHYAN 2013AB looked in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV and in 18.8 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or additionally requiring that it be identified as muon in the muon chambers, from pair production of tautilde_{{1}}'s. No evidence for an excess over the expected background is observed. Supersedes CHATRCHYAN 2012L.


pdgid: S046SLP
text:
CHATRCHYAN 2013AB limits are derived for the production of tautilde_{{1}} as a function of mass in minimal GMSB scenarios along the Snowmass Points and Slopes (SPS) line 7 (see Fig. 8 and Table 7). The limit given here is valid for the production of tautilde_{{1}} from both direct pair production and from the decay of heavier supersymmetric particles.


pdgid: S046SLP
text:
CHATRCHYAN 2012L looked in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or additionally requiring that it be identified as muon in the muon chambers, from pair production of tautilde_{{1}}()'s. No evidence for an excess over the expected background is observed. Limits are derived for the production of tautilde_{{1}}() as a function of mass in minimal GMSB scenarios along the Snowmass Points and Slopes (SPS) line 7 (see Fig. 3). The limit given here is valid for the production of tautilde_{{1}}() in the decay of heavier supersymmetric particles.


pdgid: S046SLP
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AAD 2011P looked in 37 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with two heavy stable  particles, reconstructed in the Inner tracker and the Muon System and identified by their time of flight in the Muon System. No evidence for an excess over the SM expectation is observed. Limits on the mass are derived, see Fig. 3, for tautilde  in a GMSB scenario and for sleptons  produced by electroweak processes only, in which case the limit degrades to 110 GeV.


pdgid: S046SQK
text:
AAD 2024Z searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with exactly two same-sign leptons or at least three leptons. Several signal regions, including a  notET selection targeting RPC models, and selections based on b-jet multiplicities,  targeting RPV models, are considered. No significant excess over the Standard Model expectation is  found. Exclusion limits at 95% C.L. are set on the gluino or squark mass, in multi-step RPC  decays via charginos, neutralinos or sleptons into quarks, leptons and neutralinos, or RPV decays  of either the neutralino LSP or the stop produced in gtilde --> t ttilde into quarks. See their  Fig. 7.


pdgid: S046SQK
text:
HAYRAPETYAN 2024Q searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of stealth supersymmetry in final states with two photons and jets, and low notET.  No significant excess above the Standard Model expectations is observed. The investigated models  include a singlet scalar boson S, and its SUSY fermion Stilde. In the investigated models,  either gluinos or squarks are pair produced and each decay to a chitilde_{{1}}()0 and a gluon or  squark, respectively, followed by the decays chitilde_1()0 --> gamma Stilde,  Stilde --> Gtilde S and  S --> g g. Limits are set on the gtilde and the qtilde mass, see their Fig. 4.


pdgid: S046SQK
text:
AAD 2023AE searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with 2  lepton with same flavour and opposite sign, plus jets and notET, defining signal  region  with the dilepton invariant mass both on- and off-shell with respect to the Z boson. No   significant excess above the Standard Model  predictions is observed. Limits are set on models of   strong and electroweak production. In this case, limits are placed on the mass of pair-produced   squarks, assuming a scenario like in Tsqk2,  see figure 16.


pdgid: S046SQK
text:
TUMASYAN 2023X searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  squark pair production with cascade decays to CP-even singlet-like Higgs bosons (H_{{1}}),   leading   to final states with small missing transverse momentum. This search targets H_{{1}}   decays to b bbar-pairs that are reconstructed in large-area (AK8) jets. No significant  excess  above   the Standard Model expectations is observed.  Limits are set in the next-to-minimal   supersymmetric   extension of the SM, where a singlino of small mass leads to squark and gluino   cascade decays that   can predominantly end in a highly Lorentz-boosted singlet-like H_{{1}}  and a   singlino-like   neutralino chitilde_{{S}}()0 of small transverse momentum. The eight first- and   second-generation  squarks are assumed mass-degenerate, and the gluino mass is set at 1%  larger.


pdgid: S046SQK
text:
AAD 2021AK searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair   production of gluinos and squarks in events with a single isolated electron or muon, originating   from the decay of a W boson, multiple jets and significant notET. No significant excess  above  the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1B   simplified model and on the squark mass in the Tsqk3 simplified model, see their Figure 8.


pdgid: S046SQK
text:
AAD 2021F searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of squarks in events with a high-pT jet and notET. No significant excess  above the Standard Model predictions is observed. Limits are set on the ttilde mass in the  Tstop3 and Tstop4, on the btilde mass in the Tsbot1, and on the qtilde mass in the Tsqk1  simplified model (four-flavour, two chirality states degeneracy).


pdgid: S046SQK
text:
AAD 2021L searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of gluinos and squarks in events with jets, large missing transverse momentum but no  electrons or muons. No significant excess above the Standard Model expectations is observed. Limits  are set on the gluino mass in the Tglu1A and Tglu1B simplified models, on the squark mass in the  Tsqk1 and Tsqk3 simplified models and in a simplified model for gluino-squark production, see their  Figures 13-17.


pdgid: S046SQK
text:
SIRUNYAN 2019AG searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two photons and large notET. No significant excess above the Standard Model  expectations is observed. Limits are set on the gluino mass in the Tglu4B simplified model and on  the squark mass in the Tsqk4B simplified model, see their Figure 3.


pdgid: S046SQK
text:
SIRUNYAN 2019CH searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing multiple jets and large notET. No significant excess above the Standard  Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu1C, Tglu2A and  Tglu3A simplified models, see their Figure 13.  Limits are also set on squark, sbottom and stop  masses in the Tsqk1, Tsbot1, Tstop1 simplified models, see their Figure 14.


pdgid: S046SQK
text:
AABOUD 2018BJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in  events with two opposite-sign charged leptons (electrons and muons), jets and missing transverse  momentum, with various requirements to be sensitive to signals with different kinematic endpoint  values in the dilepton invariant mass distribution. The data are found to be consistent with the SM  expectation. Results are interpreted in the Tsqk2 model in case of mass(chitilde_{{1}}()0) = 1 GeV:  for any mass(chitilde_{{2}}()0), squark masses below 1200 GeV are excluded, see their Fig. 14(b).


pdgid: S046SQK
text:
AABOUD 2018BV searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet identified as c-jet, large missing transverse energy and no  leptons. Good agreement is observed between the number of events in data and Standard Model  predictions. The results are translated into exclusion limits in Tsqk1 models considering only  ctilde_{{1}}. In scenarios with massless neutralinos, scharm masses below 850 GeV are excluded. If  the differences of the ctilde_{{1}} and chitilde_{{1}}()0  masses is below 100 GeV, scharm masses  below 500 GeV are excluded. See their Fig.6 and Fig.7.


pdgid: S046SQK
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AABOUD 2018I searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet with a transverse momentum above 250 GeV and no leptons. Good  agreement is observed between the number of events in data and Standard Model predictions. The  results are translated into exclusion limits in Tsqk1 models.  In the compressed scenario with  similar squark and neutralino masses, squark masses below 710 GeV are excluded. See their Fig.10(b).


pdgid: S046SQK
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AABOUD 2018U searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with at least one isolated photon, possibly jets and significant transverse momentum targeting  generalised models of gauge-mediated SUSY breaking. No significant excess of events is observed  above the SM prediction. Results are interpreted in terms of lower limits on the masses of squark  in Tsqk4B models. Masses below 1820 GeV are excluded for any NLSP mass, see their Fig. 9.


pdgid: S046SQK
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AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in the Tsqk1 model: squark masses below 1550 GeV  are excluded for massless LSP, see their Fig. 13(a).


pdgid: S046SQK
text:
AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in the Tsqk3 model. Assuming that  mass(chitilde_{{1}}()+-) = 0.5 (mass(qtilde) + mass(chitilde_{{1}}()0)), squark masses below 1150 GeV  are excluded for massless LSP, see their Fig. 14(a). Exclusions are also shown assuming  mass(chitilde_{{1}}()0) = 60 GeV, see their Fig. 14(b).


pdgid: S046SQK
text:
SIRUNYAN 2018AY searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing one or more jets and significant notET. No significant excess above the  Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu2A  and Tglu3A simplified models, see their Figure 3. Limits are also set on squark, sbottom and stop  masses in the Tsqk1, Tsbot1, Tstop1 and Tstop4 simplified models, see their Figure 3. Finally,  limits are set on long-lived gluino masses in a Tglu1A simplified model where the gluino is  metastable or long-lived with proper decay lengths in the range E-3 mm < ctau <  E5 mm, see their Figure 4.


pdgid: S046SQK
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AABOUD 2017AR searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one isolated lepton, at least two jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.25 TeV are set  on the 1st and 2nd generation squark masses in Tsqk3 simplified models, with  x = (mass(chitilde_{{1}}()+-)-mass(chitilde_{{1}}()0)) /  (mass(qtilde)-mass(chitilde_{{1}}()0)) = 1/2. Similar limits are obtained for variable  x and fixed  neutralino mass, mass(chitilde_{{1}}()0) = 60 GeV. See their Figure 13.


pdgid: S046SQK
text:
AABOUD 2017N searched in 14.7 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with 2 same-flavour, opposite-sign leptons (electrons or muons), jets and large missing  transverse momentum. The results are interpreted as 95% C.L. limits in Tsqk2 models, assuming  mass(chitilde_{{1}}()0) = 0 GeV and mass(chitilde_{{2}}()0) = 600 GeV. See their Fig. 12 for exclusion  limits as a function of mass(chitilde_{{2}}()0).


pdgid: S046SQK
text:
KHACHATRYAN 2017P searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more jets and large notET. No significant excess above the Standard Model  expectations is observed. Limits are set on  the gluino mass in the Tglu1A, Tglu2A, Tglu3A, Tglu3B,  Tglu3C and Tglu3D simplified models, see their Figures 7 and 8. Limits are also set on the squark  mass in the Tsqk1 simplified model, see their Fig. 7, and on the sbottom mass in the Tsbot1  simplified model, see Fig. 8. Finally, limits are set on the stop mass in the Tstop1, Tstop3,  Tstop4, Tstop6 and Tstop7 simplified models, see Fig. 8.


pdgid: S046SQK
text:
KHACHATRYAN 2017V searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two photons and large notET. No significant excess above the Standard Model  expectations is observed. Limits are set on the gluino and squark mass in the context of general  gauge mediation models Tglu4B and Tsqk4, see their Fig. 4.


pdgid: S046SQK
text:
SIRUNYAN 2017AY searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one photon, jets and large notET. No significant excess above the  Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu4A and Tglu4B  simplified models, and on the squark mass in the Tskq4A and Tsqk4B simplified models, see their  Figure 6.


pdgid: S046SQK
text:
SIRUNYAN 2017AZ searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more jets and large notET. No significant excess above the Standard Model  expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu2A, Tglu3A  simplified models, see their Figures 6.  Limits are also set on the squark mass in the Tsqk1  simplified model (for single light squark and for 8 degenerate light squarks), on the sbottom mass  in the Tsbot1 simplified model and on the stop mass in the Tstop1 simplified model, see their Fig.  7. Finally, limits are set on the stop mass in the Tstop2, Tstop4 and Tstop8 simplified models, see  Fig. 8.


pdgid: S046SQK
text:
SIRUNYAN 2017P searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with multiple jets and large notET. No significant excess above the Standard Model  expectations is observed. Limits are set on  the gluino mass in the Tglu1A, Tglu1C, Tglu2A, Tglu3A  and Tglu3D simplified models, see their Fig. 12. Limits are also set on the squark mass in the  Tsqk1 simplified model, on the stop mass in the Tstop1 simplified model, and on the sbottom mass in  the Tsbot1 simplified model, see Fig. 13.


pdgid: S046SQK
text:
AABOUD 2016D searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with an energetic jet and large missing transverse momentum. The results are interpreted as  95% C.L. limits on masses of first and second generation squarks decaying into a quark and  the lightest neutralino in scenarios with mass(qtilde) - mass(chitilde_{{1}}()0) < 25  GeV. See their Fig. 6.


pdgid: S046SQK
text:
AABOUD 2016N searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing hadronic jets, large notET, and no electrons or muons. No significant excess above  the Standard Model expectations is observed. First- and second-generation squark masses below 1030  GeV are excluded at the 95% C.L. decaying to quarks and a massless lightest neutralino. See  their Fig. 7a.


pdgid: S046SQK
text:
KHACHATRYAN 2016BS searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one energetic jet , no isolated leptons, and significant notET, using  the transverse mass variable M_{{T2}} to discriminate between signal and background processes. No  significant excess above the Standard Model expectations is observed. Limits are set on the squark  mass in the Tskq1 simplified model, both in the assumption of a single light squark and of 8  degenerate squarks, see Fig. 11 and Table 3.


pdgid: S046SQK
text:
AAD 2015BV summarized and extended ATLAS searches for gluinos and first- and   second-generation squarks in final states containing jets and missing transverse momentum, with or   without leptons or b-jets in the sqrt(s) = 8 TeV data set collected in 2012. The paper   reports the results of new interpretations and statistical combinations of previously published   analyses, as well as new analyses. Exclusion limits at 95% C.L. are set on the squark mass in   several R-parity conserving models. See their Figs. 9, 11, 18, 22, 24, 27, 28.


pdgid: S046SQK
text:
AAD 2015CS searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for evidence  of pair production of squarks, decaying into a quark and a neutralino, where a photon was radiated  either from an initial-state quark, from an intermediate squark, or from a final-state quark. No  evidence was found for an excess above the expected level of Standard Model background and a  95% C.L. exclusion limit was set on the squark mass as a function of the squark-neutralino  mass difference, see Fig. 19.


pdgid: S046SQK
text:
AAD 2015K searched in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events  containing at least two jets, where the two leading jets are each identified as originating from  c-quarks, and large missing transverse momentum. No excess of events above the expected  level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the  mass of superpartners of charm quarks (ctilde). Assuming that the decay ctilde --> c chitilde_1()0  takes place 100% of the time, a scalar charm mass below 490 GeV is excluded for  mass(chitilde_{{1}}()0) < 200 GeV. For more details, see their Fig. 2.


pdgid: S046SQK
text:
KHACHATRYAN 2015AF searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with at least two energetic jets and significant notET, using the transverse mass variable M_{{T2}} to discriminate between signal and background processes. No significant excess above the Standard Model expectations is observed. Limits are set on the squark mass in simplified models where the decay qtilde --> q chitilde_1()0 takes place with a branching  ratio of 100%, both for the case of a single light squark or 8 degenerate squarks, see Fig. 12. See also Table 5. Exclusions in the CMSSM, assuming tan(beta) = 30,  A(0) = -2 max(mass(0), mass(1/2)) and mu > 0, are also  presented, see Fig. 15.


pdgid: S046SQK
text:
AAD 2014AE searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for strongly produced supersymmetric particles in events containing jets and large missing transverse momentum, and no electrons or muons. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing squarks that decay via qtilde --> q chitilde_1()0, where either a single light state or two degenerate generations of squarks are assumed, see Fig. 10.


pdgid: S046SQK
text:
CHATRCHYAN 2014AH searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with at least two energetic jets and significant notET, using the razor variables (M_{{R}}() and R^2()) to discriminate between signal and background processes. No significant excess above the Standard Model expectations is observed. Limits are set on squark masses in simplified models where the decay qtilde --> q chitilde_1()0 takes place with a branching ratio of 100%, see Fig. 28. Exclusions in the CMSSM, assuming tan(beta) = 10, A_{{0}}() = 0 and mu > 0, are also presented, see Fig. 26.


pdgid: S046SQK
text:
CHATRCHYAN 2014I searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing multijets and large notET. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing squarks that decay via qtilde --> q chitilde_1()0, where either a single light state or two degenerate generations of squarks are assumed, see Fig. 7a.


pdgid: S046SQK
text:
AAD 2013L searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for the production of squarks and gluinos in events containing jets, missing transverse momentum and no high-pT electrons or muons. No excess over the expected SM background is observed. In mSUGRA/CMSSM models with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, squarks and gluinos of equal mass are excluded for masses below 1360 GeV at 95% C.L. In a simplified model containing only squarks  of the first two generations, a gluino octet and a massless neutralino, squark masses below 1320 GeV are excluded at 95% C.L.  for gluino masses below 2 TeV. See Figures 10 -- 15 for more precise bounds.


pdgid: S046SQK
text:
AAD 2013Q searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events containing a high-pT isolated  photon, at least one jet identified as originating from a bottom quark, and high missing transverse momentum. Such signatures may  originate from supersymmetric models with gauge-mediated supersymmetry breaking in events in which one of a pair of higgsino-like  neutralinos decays into a photon and a gravitino while the other decays into a Higgs boson and a gravitino. No significant excess  above the expected background was found and limits were set  on the squark mass as a function of the neutralino mass in  a generalized GMSB model (GGM) with a higgsino-like neutralino NLSP, see their Fig. 4.  For neutralino masses greater than 220 GeV,  squark masses below 1020 GeV are excluded at 95% C.L.


pdgid: S046SQK
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CHATRCHYAN 2013 looked in 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with two opposite-sign leptons (e, mu, tau), jets and missing transverse energy. No excess beyond the Standard Model expectation is observed. Exclusion limits are derived in the mSUGRA/CMSSM model with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, see Fig. 6.


pdgid: S046SQK
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CHATRCHYAN 2013G searched in 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV for the production of squarks and gluinos in events containing 0,1,2, >=3 b-jets, missing transverse momentum and no electrons or muons. No excess over the expected SM background is observed. In mSUGRA/CMSSM models with tan(beta) = 10, A_{{0}}() = 0, and mu > 0, squarks and gluinos of equal mass are excluded for masses below 1250 GeV at 95% C.L. Exclusions are also derived in various simplified models, see Fig. 7.


pdgid: S046SQK
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CHATRCHYAN 2013H searched in 4.96 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events  with two photons, >=4 jets and low notET due to qtilde --> gamma chitilde_1()0 decays in a stealth SUSY framework, where the chitilde_{{1}}()0 decays through a singlino (Stilde) intermediate state to gamma S Gtilde, with the singlet state S decaying to two jets. No significant excess above the expected background was found and limits were set in a particular R-parity conserving stealth SUSY model. The model assumes mass(chitilde_{{1}}()0) = 0.5 mass(qtilde), mass(Stilde) = 100 GeV and mass(S) = 90 GeV. Under these assumptions, squark masses less than 1430 GeV were excluded at the 95% C.L.


pdgid: S046SQK
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CHATRCHYAN 2013T searched in 11.7 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least two energetic jets and significant notET, using the alpha_{{T}}() variable to discriminate between processes with genuine and misreconstructed notET. No significant excess above the Standard Model expectations is observed. Limits are set on squark masses in simplified models where the decay qtilde --> q chitilde_1()0 takes place with a branching ratio of 100%, assuming an eightfold degeneracy of the masses of the first two generation squarks, see Fig. 8 and Table 9. Also limits in the case of a single light squark are given.


pdgid: S046SQK
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AAD 2012AX searched in 1.04 fb**-1 of p p collisions at sqrt(s) = 7 TeV for supersymmetry in events containing jets, missing transverse momentum and one isolated electron or muon. No excess over the expected SM background is observed and model-independent limits are set on the cross section of new physics contributions to the signal regions. In mSUGRA/CMSSM models with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, squarks and gluinos of equal mass are excluded for masses below 820 GeV at 95% C.L. Limits are also set on simplified models for squark production and decay via an intermediate chargino and on supersymmetric models with bilinear R-parity violation. Supersedes AAD 2011G.


pdgid: S046SQK
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AAD 2012CJ searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events containing one or more isolated leptons (electrons or muons), jets and notET. The observations are in good agreement with the SM expectations and exclusion limits have been set in number of SUSY models. In the mSUGRA/CMSSM model with tan(beta) = 10, A_{{0}}() = 0, and mu > 0, 95% C.L. exclusion limits have been derived for mass(qtilde) < 1200 GeV, assuming equal squark and gluino masses. In minimal GMSB, values of the effective SUSY breaking scale Lambda < 50 TeV are excluded at 95% C.L. for tan(beta) < 45. Also exclusion limits in a number of simplified models have been presented, see Figs. 10 and 12.


pdgid: S046SQK
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AAD 2012CP searched in 4.8 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events  with two photons and large notET due to  chitilde_1()0 --> gamma Gtilde decays in a GMSB framework. No significant excess above the expected  background was found and limits were set  on the squark mass as a function of the neutralino mass in a generalized GMSB model  (GGM) with a bino-like neutralino NLSP. The other sparticle masses were decoupled, tan(beta) = 2 and ctau_{{NLSP}}() < 0.1 mm. Also, in the framework of the SPS8 model, a 95% C.L. lower limit was set on the breaking scale Lambda of 196 TeV.


pdgid: S046SQK
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AAD 2012W searched in 1.04 fb**-1 of p p collisions at sqrt(s) = 7 TeV for the production of squarks and gluinos  in events containing jets, missing transverse momentum and no electrons or muons. No excess over the expected SM background is  observed. In mSUGRA/CMSSM models with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, squarks and gluinos of equal  mass are excluded for masses below 950 GeV at 95% C.L. In a simplified model containing only squarks of the first two generations, a gluino octet and a massless neutralino, squark masses below 875 GeV are excluded at 95% C.L.


pdgid: S046SQK
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CHATRCHYAN 2012 looked in 35 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with e and/or mu  and/or jets, a large total transverse energy, and notET. The event selection is based on the dimensionless razor  variable R, related to the notET and M_{{R}}(), an indicator of the heavy particle mass scale. No evidence for an  excess over the expected background is observed. Limits are derived in the CMSSM (m_{{0}}(), m_{{1/2}}()) plane for  tan(beta) = 3, 10 and 50 (see Fig. 7 and 8). Limits are also obtained for Simplified Model Spectra.


pdgid: S046SQK
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CHATRCHYAN 2012AE searched in 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with at least three jets and large missing transverse momentum. No significant excesses over the expected  SM backgrounds are observed and 95% C.L. limits on the production cross section of squarks in a scenario where  qtilde -->  q chitilde_1()0 with a 100% branching ratio, see Fig. 3. For mass(chitilde_{{1}}()0) < 200 GeV, values of mass(qtilde) below 760 GeV are excluded at 95% C.L. Also limits in the CMSSM are presented, see Fig. 2.


pdgid: S046SQK
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CHATRCHYAN 2012AT searched in 4.73 fb**-1 of p p collisions at sqrt(s) = 7 TeV for the production of squarks and gluinos in events containing jets, missing transverse momentum and no electrons or muons. No excess over the expected SM background is observed. In mSUGRA/CMSSM models with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, squarks with masses below 1110 GeV are excluded at 95% C.L. Squarks and gluinos of equal mass are excluded for masses below 1180 GeV at 95% C.L. Exclusions are also derived in various simplified models, see Fig. 6.


pdgid: S046SQK
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AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in the Tsqk5 model. Squark masses below 1100 GeV  are excluded if (mass(chitilde_{{2}}()0) - mass(chitilde_{{1}}()0))/(mass(qtilde) -  mass(chitilde_{{1}}()0)) < 0.95 and mass(chitilde_{{1}}()0) = 60 GeV, see their Fig. 16(a).


pdgid: S046SQK
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KHACHATRYAN 2016BT performed a global Bayesian analysis of a wide range of CMS results  obtained with data samples corresponding to 5.0 fb^{-1} of p p collisions at sqrt(s) = 7  TeV and in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV. The set of searches  considered, both individually and in combination, includes those with all-hadronic final states,  same-sign and opposite-sign dileptons, and multi-lepton final states. An interpretation was given  in a scan of the 19-parameter pMSSM. No scan points with a gluino mass less than 500 GeV survived  and 98% of models with a squark mass less than 300 GeV were excluded.


pdgid: S046SQK
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AAD 2015AI searched in 20 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events  containing at least one isolated lepton (electron or muon), jets, and large missing transverse  momentum. No excess of events above the expected level of Standard Model background was found.  Exclusion limits at 95% C.L. are set on the squark masses in the CMSSM/mSUGRA, see Fig. 15,  in the NUHMG, see Fig. 16, and in various simplified models, see Figs. 19 -- 21.


pdgid: S046SQK
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KHACHATRYAN 2015AR searched in 19.7 of fb^{-1} of p p collisions at sqrt(s) = 8 TeV  for events containing jets, either a charged lepton or a photon, and low missing transverse momentum. No significant excess above the Standard Model expectations is observed.  Limits are set   on the squark mass in a stealth SUSY model where the decays qtilde --> q chitilde_1()+-, chitilde_1()+- --> Stilde W+-, Stilde --> S Gtilde and S --> g g,  with mass(Stilde) =  100 GeV and mass(S) = 90 GeV, take place with a branching ratio of 100%. See Fig. 6 for  gamma or Fig. 7 for lepton+- analyses.


pdgid: S046SQK
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KHACHATRYAN 2015AZ searched in 19.7 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with either at least one photon, hadronic jets and notET (single photon channel) or  with at least two photons and at least one jet and using the razor variables. No significant excess  above the Standard Model expectations is observed. Limits are set on gluino masses in the general  gauge-mediated SUSY breaking model (GGM), for both a bino-like and wino-like neutralino NLSP  scenario, see Fig. 8 and 9.


pdgid: S046SQK
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AAD 2014E searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for strongly produced supersymmetric particles in events containing jets and two same-sign leptons or three leptons. The search also utilises jets originating from b-quarks, missing transverse momentum and other variables. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing gluinos and squarks, see Figures 5 and 6. In the qtilde --> q^' chitilde_1()+-, chitilde_1()+- --> W^(*)()+- chitilde_2()0, chitilde_2()0 --> Z^(*)() chitilde_1()0  simplified model, the following assumptions have been made: mass(chitilde_{{1}}()+-) = 0.5 mass(chitilde_{{1}}()0) + mass(gtilde), mass(chitilde_{{2}}()0) = 0.5 ( mass(chitilde_{{1}}()0) + mass(chitilde_{{1}}()+-) ). In the qtilde --> q^' chitilde_1()+- or qtilde --> q^' chitilde_2()0, chitilde_1()+- --> lepton+- nu chitilde_1()0  or chitilde_2()0 --> lepton+- lepton-+ ( nu nu ) chitilde_1()0 simplified model, the following assumptions have been made: mass(chitilde_{{1}}()+-) = mass(chitilde_{{2}}()0) = 0.5 ( mass(chitilde_{{1}}()0) + mass(qtilde) ), mass(chitilde_{{1}}()0) < 460 GeV. Limits are also derived in the mSUGRA/CMSSM, bRPV and GMSB models, see their Fig. 8.


pdgid: S046SQK
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CHATRCHYAN 2013AO searched in 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with two opposite-sign isolated leptons accompanied by hadronic jets and notET. No significant excesses over the expected SM backgrounds are observed and 95% C.L. exclusion limits are derived in the mSUGRA/CMSSM model with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, see Fig. 8.


pdgid: S046SQK
text:
CHATRCHYAN 2013AV searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for new heavy particle pairs decaying into jets (possibly b-tagged), leptons and notET using the Razor variables. No significant excesses over the expected SM backgrounds are observed and 95% C.L. exclusion limits are derived in the mSUGRA/CMSSM model with tan(beta) = 10, A_{{0}}() = 0 and mu > 0, see Fig. 3. The results are also interpreted in various simplified models, see Fig. 4.


pdgid: S046SQK
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CHATRCHYAN 2013W searched in 4.93 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with one or more photons, hadronic jets and notET. No significant excess above the Standard Model expectations is observed. Limits are set on squark masses in the general gauge-mediated SUSY breaking model (GGM), for both a wino-like and bino-like neutralino NLSP scenario, see Fig. 5.


pdgid: S046SQK
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DREINER 2012A reassesses constraints from CMS (at 7 TeV, ~4.4 fb**-1) under the assumption that the  fist and second generation squarks and the lightest SUSY particle are quasi-degenerate in mass (compressed spectrum).


pdgid: S046SQK
text:
DREINER 2012A reassesses constraints from CMS (at 7 TeV, ~4.4 fb**-1) under the assumption that the first and second generation squarks, the gluino, and the lightest SUSY particle are quasi-degenerate in mass (compressed spectrum).


pdgid: S046SQV
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HAYRAPETYAN 2024Y searched in 36.6 fb^{-1} of p p collisions at sqrt(s) = 13.6 TeV  for evidence of R-parity violating (RPV) SUSY in events with a pair of oppositely charged muons  originating from a secondary vertex spatially separated from the p p interaction point by  distances ranging from several hundred mum to several meters. No significant excess above the  Standard Model expectations is observed.  Limits are set in the model Tsqk3RPV on the lifetime of  the chitilde_{{1}}()0 for several values of the qtilde mass, see their Fig. 16.  Limits are  also interpreted in the framework of a hidden Abelian Higgs model, in which the Higgs boson decays  to a pair of long-lived dark photons, see their Figs. 14 and 15.


pdgid: S046SQV
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SIRUNYAN 2018EA searched in 38.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  the pair production of resonances, each decaying to at least four quarks. Reconstructed particles  are clustered into two large jets of similar mass, each consistent with four-parton substructure.  No statistically significant excess over the Standard Model expectation is observed. Limits are set  on the squark and gluino mass in RPV supersymmetry models where squarks (gluinos) decay, through  intermediate higgsinos, to four (five) quarks,  see their Figure 4.


pdgid: S046SQV
text:
KHACHATRYAN 2016BX searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing 4 leptons coming from R-parity-violating decays of chitilde_1()0 --> lepton lepton nu  with  lambda_{{121}} not= 0 or lambda_{{122}} not= 0.  No excess over the expected  background is observed. Limits are derived on the gluino, squark and stop masses, see Fig. 23.


pdgid: S046SQV
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AAD 2015CB searched for events containing at least one long-lived particle that decays at a  significant distance from its production point (displaced vertex, DV) into two leptons or into five  or  more charged particles in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV. The  dilepton signature is  characterised by DV formed from at least two lepton candidates. Four  different final states  were considered for the multitrack signature, in which the DV must be  accompanied by a high-transverse  momentum muon or electron candidate that originates from the DV,  jets or missing transverse momentum.  No events were observed in any of the signal regions. Results  were interpreted in SUSY scenarios involving  R-parity violation, split supersymmetry, and  gauge mediation.  See their Fig. 14 -- 20.


pdgid: S046SQV
text:
CHATRCHYAN 2012AL looked in 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV for anomalous production of events with three or more isolated leptons. Limits on squark and gluino masses are set in RPV SUSY models with leptonic LLEbarcouplings, lambda_{{123}}() > 0.05, and hadronic UbarDbarDbar couplings, lambda(112)**'' > 0.05 , see their Fig. 5. In the UbarDbarDbar case the leptons arise from supersymmetric cascade decays. A very specific supersymmetric spectrum is assumed. All decays are prompt.


pdgid: S046SSQ
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AABOUD 2019AT searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  metastable and stable R-hadrons. Multiple search strategies for a wide range of lifetimes,  corresponding to path lengths of a few meters, are defined. No significant deviations from the  expected Standard Model background are observed. Sbottom R-hadrons are excluded at 95%  C.L. for masses below 1250 GeV. Less stringent constraints are achieved with the muon-spectrometer  agnostic analysis. See their Figure 9 (bottom-left).


pdgid: S046SSQ
text:
AABOUD 2019AT searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  metastable and stable R-hadrons. Multiple search strategies for a wide range of lifetimes,  corresponding to path lengths of a few meters, are defined. No significant deviations from the  expected Standard Model background are observed. Stop R-hadrons are excluded at 95% C.L.  for masses below 1340 GeV. Similar constraints are achieved with the muon-spectrometer agnostic  analysis. See their Figure 9 (bottom-right).


pdgid: S046SSQ
text:
SIRUNYAN 2019BH searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived particles decaying into jets, with each long-lived particle having a decay vertex well  displaced from the production vertex. The selected events are found to be consistent with standard  model predictions. Limits are set on the gluino mass in a GMSB model where the gluino is decaying  via gtilde --> g Gtilde, see their Figure 4 and in an RPV model of supersymmetry where the  gluino is decaying via gtilde --> tbar bbar sbar, see their Figures 5. Limits are also set on  the stop mass in two RPV models, see their Figure 6 (for ttilde --> b lepton decays) and Figure  7 (for ttilde --> dbar dbar decays).


pdgid: S046SSQ
text:
AABOUD 2016B searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived R-hadrons using observables related to large ionization losses and slow propagation  velocities, which are signatures of heavy charged particles traveling significantly slower than the  speed of light. Exclusion limits at 95% C.L. are set on the long-lived sbottom masses  exceeding 805 GeV. See their Fig. 5.


pdgid: S046SSQ
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AABOUD 2016B searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived R-hadrons using observables related to large ionization losses and slow propagation  velocities, which are signatures of heavy charged particles traveling significantly slower than the  speed of light. Exclusion limits at 95% C.L. are set on the long-lived stop masses exceeding  890 GeV. See their Fig. 5.


pdgid: S046SSQ
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KHACHATRYAN 2016BW searched in 2.5 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events  with heavy stable charged particles, identified by their anomalously high energy deposits  in the silicon tracker and/or long time-of-flight measurements by the muon system. No evidence for  an excess over the expected background is observed. Limits are derived for pair production of top  squarks as a function of mass, depending on the interaction model, see Fig. 4 and Table 7.


pdgid: S046SSQ
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AAD 2015AE searched in 19.1 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for heavy  long-lived charged particles, measured through their specific ionization energy loss in the ATLAS  pixel detector or their time-of-flight in the ALTAS muon system. In the absence of an excess of  events above the expected backgrounds, limits are set R-hadrons in various scenarios, see Fig. 11.   Limits are also set in LeptoSUSY models where the gluino decays to stable 300 GeV leptons, see Fig. 9.


pdgid: S046SSQ
text:
AAD 2015BM searched in 18.4 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for stable  and metastable non-relativistic charged particles through their anomalous specific ionization  energy loss in the ATLAS pixel detector. In absence of an excess of events above the expected  backgrounds, limits are set on stable  bottom and top squark R-hadrons, see Table 5.


pdgid: S046SSQ
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KHACHATRYAN 2015AK looked in a data set corresponding to fb**-1 of p p collisions at   sqrt(s) = 8 TeV, and a search interval corresponding to 281 h of trigger lifetime, for long-lived   particles that have stopped in the CMS detector. No evidence for an excess over the expected  background in a cloud interaction model is observed. Assuming the decay ttilde --> t chitilde_1()0 and  lifetimes  between 1 mus and 1000 s, limits are derived on ttilde production as a function  of mass(chitilde_{{1}}()0), see Figs. 4 and 7. The exclusions require that mass(chitilde_{{1}}()0) is  kinematically consistent with the minimum values of the jet energy thresholds used.


pdgid: S046SSQ
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AAD 2013AA searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events containing colored long-lived particles that hadronize forming R-hadrons. No significant excess above the expected background was found. Long-lived R-hadrons containing a ttilde are excluded for masses up to 683 GeV at 95% C.L in a general interaction model. Also, limits independent of the fraction of R-hadrons that arrive charged in the muon system were derived, see Fig. 6.


pdgid: S046SSQ
text:
AAD 2013AA searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events containing colored long-lived particles that hadronize forming R-hadrons. No significant excess above the expected background was found. Long-lived R-hadrons containing a btilde are excluded for masses up to 612 GeV at 95% C.L in a general interaction model.  Also, limits independent of the fraction of R-hadrons that arrive charged in the muon system were derived, see Fig. 6.


pdgid: S046SSQ
text:
AAD 2013BC searched in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV and in 22.9 fb**-1 of p p collisions at sqrt(s) = 8 TeV for bottom squark R-hadrons that have come to rest within the ATLAS calorimeter and decay at some later time to hadronic jets and a neutralino. In absence of an excess of events above the expected backgrounds, limits are set on sbottom masses for the decay btilde --> b chitilde_1()0, for different lifetimes, and for a neutralino mass of 100 GeV, see their Table 6 and Fig 10.


pdgid: S046SSQ
text:
AAD 2013BC searched in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV and in 22.9 fb**-1 of p p collisions at sqrt(s) = 8 TeV for bottom squark R-hadrons that have come to rest within the ATLAS calorimeter and decay at some later time to hadronic jets and a neutralino. In absence of an excess of events above the expected backgrounds, limits are set on stop masses for the decay ttilde --> t chitilde_1()0, for different lifetimes, and for a neutralino mass of 100 GeV, see their Table 6 and Fig 10.


pdgid: S046SSQ
text:
CHATRCHYAN 2013AB looked in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV and in 18.8 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or additionally requiring that it be identified as muon in the muon chambers, from pair production of ttilde_{{1}}'s. No evidence for an excess over the expected background is observed. Limits are derived for pair production of stops as a function of mass in the cloud interaction model (see Fig. 8 and Table 6). In the charge-suppressed model, the limit decreases to 818 GeV.


pdgid: S046SBT
text:
AAD 2021AM searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair   production of bottom squarks in events with hadronically decaying tau+--leptons, b-tagged  jets, and large notET. No significant excess above the Standard Model expectations is  observed. Limits are set on the bottom squark mass in the Tsbot4 simplified model, assuming   mass(chitilde_{{2}}()0) - mass(chitilde_{{1}}()0) = 130 GeV, see their Figure 8.


pdgid: S046SBT
text:
AAD 2021S searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV  for pair   production of sbottoms, LQ or dark matter in events with b-jets and notET, also using   dedicated secondary-vertex-finding techniques. No significant excess above the Standard Model   predictions is observed. Limits are set on mass(btilde_{{1}}) in the Tsbot1 simplified model, on the   LQ masses depending on the BR in b nu, on scalar and pseudoscalar dark matter mediator  masses.  See Figures 8, 9, 10.


pdgid: S046SBT
text:
AAD 2020V searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with two same-sign charged leptons (electrons or muons) and jets. No significant excess above the  Standard Model expectations is observed. Exclusion limits at 95% C.L. are set on the bottom  squark masses in the Tsbot2 simplified model for mass(chitilde_{{1}}()+-) = mass(chitilde_{{1}}()0) + 100  GeV, see their Fig. 8(a).


pdgid: S046SBT
text:
SIRUNYAN 2020T searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least two jets, and two isolated same-sign or three or more charged leptons  (electrons or muons). No significant excess above the Standard Model expectations is observed.  Limits are set on the gluino mass in the Tglu3A, Tglu3B, Tglu3C and Tglu3D simplified models, see  their Figure 7, and in the Tglu1C and Tglu1B simplified models, see their Figures 8 and 9. Limits  are also set on the sbottom mass in the Tsbot2 simplified model, see their Figure 10, and on the  stop mass in the Tstop7 simplified model, see their Figure 11. Finally, limits are set on the  gluino mass in RPV simplified models where the gluino decays either via gtilde -->  q q qbar qbar + e / mu / tau or  via gtilde --> t b s, see Figure 12.


pdgid: S046SBT
text:
AAD 2019H searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with no charged leptons, three or more b-jets, and large notET.  Higgs boson candidates  are reconstructed as b-jet pairs. No significant excess above the Standard Model expectations  is observed. Limits up to 1500 GeV are set on the sbottom mass in the Tsbot4 simplified model, see  Figure 8(a), for fixed mass(chitilde_{{1}}()0) = 60 GeV and for mass(chitilde_{{2}}()0) up to 1200 GeV.


pdgid: S046SBT
text:
AAD 2019H searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with no charged leptons, three or more b-jets, and large notET.  Higgs boson candidates  are reconstructed as b-jet  pairs. No significant excess above the Standard Model expectations  is observed. Limits up to 1300 GeV are set on the sbottom mass in the Tsbot4 simplified model, see  Figure 8(b), for mass(chitilde_{{2}}()0) = mass(chitilde_{{1}}()0) + 130 GeV and mass(chitilde_{{2}}()0)  from 200 to 750 GeV.


pdgid: S046SBT
text:
AABOUD 2018I searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet with a transverse momentum above 250 GeV and no leptons. Good  agreement is observed between the number of events in data and Standard Model predictions. The  results are translated into exclusion limits in Tsbot1 models. In the compressed scenario with  sbottom and neutralino masses differing by mass(b), sbottom masses below 430 GeV are excluded. For  mass(chitilde_{{1}}()0) = 0 they exclude sbottom masses up to 610 GeV. See their Fig.10(a).


pdgid: S046SBT
text:
SIRUNYAN 2018AL searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least three charged leptons, in any combination of electrons and muons, jets and  significant notET. No significant excess above the Standard Model expectations is observed.  Limits are set on the gluino mass in the Tglu3A and Tglu1C simplified models, see their Figure 5.  Limits are also set on the sbottom mass in the Tsbot2 simplified model, see their Figure 6, and on  the stop mass in the Tstop7 simplified model, see their Figure 7.


pdgid: S046SBT
text:
SIRUNYAN 2018AR searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing two opposite-charge, same-flavour leptons (electrons or muons), jets and  notET. No significant excess above the Standard Model expectations is observed. Limits are  set on the gluino mass in the Tglu4C simplified model, see their Figure 7. Limits are also set on  the chargino/neutralino mass in the Tchi1n2F simplified model, see their Figure 8, and  on the  neutralino mass in the Tn1n1B and Tn1n1C simplified models, see their Figure 9. Finally, limits are  set on the sbottom mass in the Tsbot3 simplified model, see their Figure 10.


pdgid: S046SBT
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SIRUNYAN 2018B searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for the  pair production of third-generation squarks in events with jets and large notET. No  significant excess above the Standard Model expectations is observed. Limits are set on the sbottom  mass in the Tsbot1 simplified model, see their Figure 5, and on the stop mass in the Tstop4  simplified model, see their Figure 6.


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 700 GeV are set  on the bottom squark mass in Tsbot2 simplified models assuming mass(chitilde_{{1}}()0) = 0 GeV. See  their Figure 4(d).


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AABOUD 2017AX searched in 36 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing two jets identified as originating from b-quarks and large missing transverse  momentum. No excess of events above the expected level of Standard Model background was found.  Exclusion limits at 95% C.L. are set on the masses of bottom squarks. In the Tsbot1  simplified model, a btilde_{{1}} mass below 950 GeV is excluded for mass(chitilde_{{1}}()0) = 0  (<420) GeV. See their Fig. 7(a).


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AABOUD 2017AX searched in 36 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing two jets identified as originating from b-quarks and large missing transverse  momentum, with or without leptons. No excess of events above the expected level of Standard Model  background was found. Exclusion limits at 95% C.L. are set on the masses of bottom squarks.  Assuming 50% BR for Tsbot1 and Tsbot2 simplified models, a btilde_{{1}} mass below 880 (860)  GeV is excluded for mass(chitilde_{{1}}()0) = 0 (<250) GeV. See their Fig. 7(b).


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KHACHATRYAN 2017A searched in 18.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with two forward jets, produced through vector boson fusion, and missing transverse  momentum. No significant excess above the Standard Model expectations is observed. A limit is set  on sbottom masses in the Tsbot1 simplified model, see Fig. 3.


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KHACHATRYAN 2017AW searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least three charged leptons, in any combination of electrons and muons, and  significant notET. No significant excess above the Standard Model expectations is observed.  Limits are set on the gluino mass in the Tglu3A and Tglu1C simplified models, and on the sbottom  mass in the Tsbot2 simplified model, see their Figure 4.


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SIRUNYAN 2017K searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  direct production of stop or sbottom pairs in events with multiple jets and significant  notET. A second search also requires an isolated lepton and is combined with the all-hadronic  search. No significant excess above the Standard Model expectations is observed. Limits are set on  the stop mass in the Tstop1, Tstop8 and Tstop4 simplified models, see their Figures 7, 8 and 9 (for  the Tstop4 limits, only the results of the all-hadronic search are used). Limits are also set on  the sbottom mass in the Tsbot1 simplified model, see Fig. 10 (also here, only the results of the  all-hadronic search are used).


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SIRUNYAN 2017S searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two isolated same-sign leptons, jets, and large notET. No significant excess  above the Standard Model expectations is observed. Limits are set on the mass of the gluino mass in  the Tglu3A, Tglu3B, Tglu3C, Tglu3D and Tglu1B simplified models, see their Figures 5 and 6, and on  the sbottom mass in the Tsbot2 simplified model, see their Figure 6.


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AABOUD 2016D searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with an energetic jet and large missing transverse momentum. The results are interpreted as  95%C.L. limits on mass of sbottom decaying into a b-quark and the lightest neutralino in  scenarios with mass(btilde_{{1}})- mass(chitilde_{{1}}()0) between 5 and 20 GeV. See their Fig. 6.


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AABOUD 2016Q searched in 3.2 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  containing two jets identified as originating from b-quarks and large missing transverse  momentum. No excess of events above the expected level of Standard Model background was found.  Exclusion limits at 95% C.L. are set on the masses of third-generation squarks. Assuming that  the decay btilde_1 --> b chitilde_1()0 (Tsbot1) takes place 100% of the time, a  btilde_{{1}} mass below 840 (800) GeV is excluded for mass(chitilde_{{1}}()0)< 100 (360) GeV.   Differences in mass above 100 GeV between the btilde_{{1}} and the chitilde_{{1}}()0 are excluded  up to a btilde_{{1}} mass of 500 GeV.  For more details, see their Fig. 4.


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AAD 2016BB searched in 3.2 fb^{-1} of pp collisions at sqrt(s) = 13 TeV for events with  exactly two same-sign leptons or at least three leptons, multiple hadronic jets, b-jets, and  notET. No significant excess over the Standard Model expectation is found. Exclusion limits  at 95% C.L. are set on the sbottom mass for the Tsbot2 model, assuming mass(chitilde_{{1}}()+-)  = mass(chitilde_{{1}}()0) + 100 GeV. See their Fig. 4c.


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KHACHATRYAN 2016BJ searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two isolated same-sign dileptons and jets in the final state. No significant excess  above the Standard Model expectations is observed.  Limits are set on the sbottom mass in the  Tsbot2 simplified model, see Fig. 6.


pdgid: S046SBT
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KHACHATRYAN 2016BS searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one energetic jet , no isolated leptons, and significant notET, using  the transverse mass variable M_{{T2}} to discriminate between signal and background processes. No  significant excess above the Standard Model expectations is observed. Limits are set on the sbottom  mass in the Tsbot1 simplified model, see Fig. 11 and Table 3.


pdgid: S046SBT
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KHACHATRYAN 2016BY searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two opposite-sign, same-flavour leptons, jets, and missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits are set on the gluino  mass in the Tglu4C simplified model, see Fig. 4, and on sbottom masses in the Tsbot3 simplified  model, see Fig. 5.


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AAD 2015CJ searched in 20 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for   evidence  of third generation squarks by combining a large number of searches covering various   final states.  Limits on the sbottom mass are shown, either assuming the btilde --> b  chitilde_1()0  decay, see Fig. 11, or assuming the btilde --> t chitilde_1()+- decay, with chitilde_1()+- -->  W^(*)() chitilde_1()0,  see Fig. 12a, or assuming the btilde --> b chitilde_2()0 decay,  with chitilde_2()0 -->  h chitilde_1()0, see  Fig. 12b.  Interpretations in the pMSSM are also discussed, see Figures 13 -- 15.


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KHACHATRYAN 2015AF searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for   events with at least two energetic jets and significant notET, using the transverse mass   variable M_{{T2}} to discriminate between signal and background processes. No significant excess   above the Standard Model expectations is observed. Limits are set on the sbottom mass in simplified   models where the decay btilde --> b chitilde_1()0 takes place with a branching ratio of   100%, see Fig. 12. See also Table 5. Exclusions in the CMSSM, assuming tan(beta) =  30, A(0) = -2 max(mass(0), mass(1/2)) and mu > 0, are also presented, see Fig. 15.


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KHACHATRYAN 2015AH searched in 19.4 or 19.7 fb^{-1} of p p collisions at sqrt(s) = 8   TeV for events containing either a fully reconstructed top quark, or events containing dijets   requiring one or both jets to originate from b-quarks, or events containing a mono-jet. No   significant excess above the Standard Model expectations is observed. Limits are set on the sbottom   mass in simplified models where the decay btilde --> b chitilde_1()0 takes place with a   branching ratio of 100%, see Fig. 12. Limits are also set in a simplified model where   the decay btilde --> c chitilde_1()0 takes place with a branching ratio of 100%,   see Fig. 12.


pdgid: S046SBT
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KHACHATRYAN 2015I searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events in which b-jets and four W-bosons are produced. Five individual search channels  are combined (fully hadronic, single lepton, same-sign dilepton, opposite-sign dilepton,  multilepton). No significant excess above the Standard Model expectations is observed. Limits are  set on the sbottom mass in a simplified model where the decay btilde --> t chitilde_1()+-, with  chitilde_1()+- --> W+- chitilde_1()0, takes place with a branching ratio of 100%, see  Fig. 7.


pdgid: S046SBT
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AAD 2014T searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for monojet-like events. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the masses of third-generation squarks in simplified models which assume that the decay btilde_1 --> b chitilde_1()0 takes place 100% of the time, see Fig. 12.


pdgid: S046SBT
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CHATRCHYAN 2014AH searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with at least two energetic jets and significant notET, using the razor variables (M_{{R}}() and R^2()) to discriminate between signal and background processes. A second analysis requires at least one of the jets to be originating from a b-quark. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay btilde --> b chitilde_1()0 takes place with a branching ratio of 100%, see Figs. 28 and 29. Exclusions in the CMSSM, assuming tan(beta) = 10, A_{{0}}() = 0 and mu >0, are also presented, see Fig. 26.


pdgid: S046SBT
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CHATRCHYAN 2014R searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least three leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in a simplified model where the decay btilde --> t chitilde_1()+-, with chitilde_1()+- --> W+- chitilde_1()0, takes place with a branching ratio of 100%, see Fig. 11.


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KHACHATRYAN 2015AD searched in 19.4 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events with two opposite-sign same flavor isolated leptons featuring either a kinematic edge, or a peak at the Z-boson mass, in the invariant mass spectrum. No evidence for a statistically significant excess over the expected SM backgrounds is observed and 95% C.L. exclusion limits   are derived in a simplified model of sbottom pair production where the sbottom decays into a b-quark, two opposite-sign dileptons and a neutralino LSP, through an intermediate state containing either an off-shell Z-boson or a slepton, see Fig. 8.


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AAD 2014AX searched in 20.1 fb**-1 of p p collisions at sqrt(s) = 8 TeV for the strong production  of supersymmetric particles in events containing either zero or at last one high high-pT lepton, large  missing transverse momentum, high jet multiplicity and at least three jets identified as originating from  b-quarks. No excess over the expected SM background is observed. Limits are derived in mSUGRA/CMSSM models  with tan(beta) = 30, A_{{0}}() = -2 m_{{0}}() and mu > 0, see their Fig. 14. Also,  exclusion limits are set in simplified models containing scalar bottom quarks, where the decay  btilde --> b chitilde_2()0 and chitilde_2()0 --> h chitilde_1()0 takes place with a branching ratio of 100%, see their Figures 11.


pdgid: S046SBT
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AAD 2014E searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for strongly produced supersymmetric particles in events containing jets and two same-sign leptons or three leptons. The search also utilises jets originating from b-quarks, missing transverse momentum and other variables. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing bottom, see Fig. 7. Limits are also derived in the mSUGRA/CMSSM, bRPV and GMSB models, see their Fig. 8.


pdgid: S046SBT
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CHATRCHYAN 2014H searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in a simplified models where the decay btilde --> t chitilde_1()+-, chitilde_1()+- --> W+- chitilde_1()0 takes place with a branching ratio of 100%, with varying mass of the chitilde_{{1}}()+-, for mass(chitilde_{{1}}()0) = 50 GeV, see Fig. 6.


pdgid: S046SBT
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AAD 2013AU searched in 20.1 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing two jets identified as originating from b-quarks and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the masses of third-generation squarks. Assuming that the decay btilde_1 --> b chitilde_1()0 takes place 100% of the time, a btilde_{{1}} mass below 620 GeV is excluded for mass(chitilde_{{1}}()0)< 120 GeV. For more details, see their Fig. 5.


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CHATRCHYAN 2013AT provides interpretations of various searches for supersymmetry by the CMS experiment based on 4.73 -- 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV in the framework of simplified models. Limits are set on the sbottom mass in a simplified models where sbottom quarks are pair-produced and the decay btilde --> b chitilde_1()0 takes place with a branching ratio of 100%, see Fig. 4.


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CHATRCHYAN 2013T searched in 11.7 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least two energetic jets and significant notET, using the alpha_{{T}}() variable to discriminate between processes with genuine and misreconstructed notET. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay btilde --> b chitilde_1()0 takes place with a branching ratio of 100%, see Fig. 8 and Table 9.


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CHATRCHYAN 2013V searched in 10.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with two isolated same-sign dileptons and at least two b-jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the bottom mass in a simplified models where the decay btilde --> t chitilde_1()+-, chitilde_1()+- --> W+- chitilde_1()0 takes place with a branching ratio of 100%, with varying mass of the chitilde_{{1}}()+-, for mass(chitilde_{{1}}()0) = 50 GeV, see Fig. 4.


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AAD 2012AN searched in 2.05 fb**-1 of p p collisions at sqrt(s) = 7 TeV for scalar bottom quarks in events with large missing transverse momentum and two b-jets in the final state. The data are found to be consistent with the Standard Model expectations. Limits are set in an R-parity conserving minimal supersymmetric scenario, assuming B(btilde_1() --> b chitilde_1()0) = 100%, see their Fig. 2.


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CHATRCHYAN 2012AI looked in 4.98 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with two same-sign leptons (e, mu), but not necessarily same flavor, at least 2 b-jets and missing transverse energy. No excess beyond the Standard Model expectation is observed. Exclusion limits are derived in a simplified model for sbottom pair production, where the sbottom decays through btilde_1() --> t chitilde_1() W, see Fig. 8.


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CHATRCHYAN 2012BO searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for scalar bottom quarks in events with large missing transverse momentum and two b-jets in the final state. The data are found to be consistent with the Standard Model expectations. Limits are set in an R-parity conserving minimal supersymmetric scenario, assuming B(btilde_1() --> b chitilde_1()0) = 100%, see their Fig. 2.


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AAD 2011K looked in 34 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with heavy stable particles,  identified by their anomalous dE/dx in the tracker or time of flight in the tile calorimeter, from pair production  of btilde. No evidence for an excess over the SM expectation is observed and limits on the mass are derived  for pair production of sbottom, see Fig. 4.


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AAD 2011O looked in 35 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with jets, of which at least  one is a b-jet, and notET. No excess above the Standard Model was found. Limits are derived in the  (mass(gtilde), mass(btilde_{{1}})) plane (see Fig. 2) under the assumption of 100% branching ratios and btilde_{{1}}  being the lightest squark. The quoted limit is valid for mass(btilde_{{1}}) < 500 GeV. A similar approach for  ttilde_{{1}} as the lightest squark with gtilde --> ttilde_1 t and ttilde_1 --> b chitilde_1()+- with 100%  branching ratios leads to a gluino mass limit of 520 GeV for 130 < mass(ttilde_{{1}}) < 300 GeV. Limits are also derived in the CMSSM (m_{{0}}(), m_{{1/2}}()) plane for tan(beta) = 40, see Fig. 4,  and in scenarios based on the gauge group SO(10).


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CHATRCHYAN 2011D looked in 35 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with >= 2 jets,  at least one of which is b-tagged, and notET, where the b-jets are decay products of ttilde or btilde. No evidence for an excess over the expected background is observed. Limits are derived in the CMSSM  (m_{{0}}(), m_{{1/2}}()) plane for tan(beta) = 50 (see Fig. 2).


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AALTONEN 2010R searched in 2.65 fb**-1 of p pbar collisions at sqrt(s) = 1.96 TeV for events with notET and exactly two jets, at least one of which is b-tagged. The results are in agreement with the SM prediction, and a limit on the cross section of 0.1 pb is obtained for the range of masses 80 < mass(btilde_{{1}})< 280 GeV assuming that the sbottom decays exclusively to b chitilde_1^0(). The excluded mass region in the framework of conserved R_{{p}} is shown in a plane of (mass(btilde_{{1}}), mass(chitilde_{{1}}^0())), see their Fig.2.


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ABAZOV 2010L looked in 5.2 fb**-1 of p pbar collisions at sqrt(s) = 1.96 TeV for events with at least 2 b-jets and notET from the production of btilde_1 btilde_1. No evidence for an excess over the SM expectation is observed, and a limit on the cross section is derived under the assumption of 100% branching ratio. The excluded mass region in the framework of conserved R_{{p}} is shown in a plane of (mass(btilde_{{1}}),mass(chitilde_{{1}}^0())), see their Fig. 3b. The exclusion also extends to mass(chitilde_{{1}}^0()) = 110 GeV for 160< mass(btilde_{{1}}) < 200 GeV.


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KHACHATRYAN 2016BX searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing 2 leptons coming from R-parity-violating decays of supersymmetric particles.  No  excess over the expected background is observed. Limits are derived on the sbottom mass, assuming  the RPV btilde --> t d or btilde --> t s decay, see Fig. 15.


pdgid: S046STP
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AAD 2024AC searched in 140 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for evidence  of stop pair production in events with one lepton, multiple jets, and large notET, using a  neural network for the top system reconstruction. The stop analysis is optimised for scenarios with  mass(ttilde_{{1}}) - mass(chitilde_{{1}}()0) ~ mass(t). No significant excess above the  Standard Model expectations is observed. Limits are set in models for stop pair production, Tstop1  (with the t possibly off-shell), see their figures 10 and 11.


pdgid: S046STP
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AAD 2024AO searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for evidence  of stop pair production in events with no leptons, jets, b- and c-jets, and large  notET. The search analysis is optimized for events where a top quark and a c quarks are  produced in the decay of the stops. No significant excess above the Standard Model expectations is  observed. Limits are set on models for stop pair production with equal branching ratio for  ttilde --> t chitilde_1()0 and ttilde --> c chitilde_1()0, Tstop9 (but also investigating  large mass gaps between ttilde and chitilde_{{1}}()0). See their figures 9 and 10.


pdgid: S046STP
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TUMASYAN 2023AB searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for    evidence of top squark pair production in a final state with at least one hadronically decaying   tau lepton and large missing transverse momentum. No significant excess above the Standard Model   expectations is observed. Limits are set on  the mass of ttilde for the model Tstop16, see   their Figure 9. The exclusion limits are not very  sensitive to the choice of the tautilde mass   parameter, chosen between 0.25 <  (mass(tautilde_{{1}}()+-) -   mass(chitilde_{{1}}()0))/(mass(chitilde_{{1}}()+-) -  mass(chitilde_{{1}}()0)) < 0.75 because of   the complementary nature of the signal diagrams.


pdgid: S046STP
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TUMASYAN 2023K searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of top squark pair production in events with a high-momentum jet, an electron or muon with  low transverse  momentum, and significant notET. No significant excess above the  Standard  Model expectations  is observed.  Limits are set on the top squark mass in the simplified  model  Tstop3 for  10 GeV  < mass(ttilde)-mass(chitilde_{{1}}()0)  < 80 GeV, see  their Figure 10.


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AAD 2021AW searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair   production of stops in events with one or two hadronically decaying tau leptons, jets,   b-jets and notET. No significant excess above the Standard Model predictions is observed.   Limits are set on the ttilde_{{1}} mass as a function of the tautilde_{{1}} in the Tstop5  scenario.  See their Fig. 8.


pdgid: S046STP
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AAD 2021O searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of top squarks in events with one electron or muon, jets, and large missing transverse  momentum. No significant excess above the Standard Model expectations is observed. Limits are set  on the top squark mass in the Tstop1 and Tstop3 simplified models and dark matter models, see their  Figures 13, 14 and 15.


pdgid: S046STP
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AAD 2021P searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of top squarks in events with two opposite-sign leptons, jets, and large missing  transverse momentum. No significant excess above the Standard Model expectations is observed.  Limits are set on the top squark mass in the Tstop1, Tstop2, and Tstop3 simplified models, see  their Figures 14.


pdgid: S046STP
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SIRUNYAN 2021AD searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  supersymmetry in events with multiple jets, no leptons, and large notET. No significant  excess above the Standard Model expectations is observed. Limits are set on the top squark mass in  the simplified models Tstop1, Tstop2 with mass(chitilde_{{1}}()+-) = (mass(ttilde) +  mass(chitilde_{{1}}()0))/2, and a 50:50 mixture of these with mass(chitilde_{{1}}()+-) -  mass(chitilde_{{1}}()0) = 5 GeV, see their Figure 8. Limits are also set on the top squark mass for 10  GeV < mass(ttilde) - mass(chitilde_{{1}}()+-) < 80 GeV in the simplified models  Tstop2, Tstop 3, and Tstop4, see their Figure 9.  For indirect top squark production, limits are  set on the gluino mass in the simplified models Tglu3A, Tglu3C with mass(ttilde) -  mass(chitilde_{{1}}()0) = 20 GeV, and Tglu3D with mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) =  5 GeV, see their Figure 10.


pdgid: S046STP
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SIRUNYAN 2021B searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for the  pair production of top squarks in events with two oppositely charged leptons (electrons or muons),   jets identified as originating from a b-quark and significant notET. No significant  excess above the Standard Model expectations is observed. Limits are set on the stop mass in the  Tstop1, Tstop2 and Tstop11 simplified models, see their Figures 6 and 7.


pdgid: S046STP
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TUMASYAN 2021I searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of top squarks in events with at least two jets and large notET, categorized into  events with 0, 1, or 2 leptons. No significant excess above the Standard Model expectations is  observed.  Limits are set on the top squark mass in the simplified model Tstop1 in the top corridor    |mass(ttilde) - mass(chitilde_{{1}}()0) - 175 GeV| < 30 GeV using dilepton  events, see their Figure 7.  Limits are also set for a combination of earlier searches with 0, 1,  and 2 leptons in the models Tstop1, Tstop2 and a 50:50 mixture of these models, see their Figure 9.  The results are interpreted in an alternative signal model of dark matter production via a spin-0  mediator in association with a top quark pair as well.


pdgid: S046STP
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AABOUD 2020 searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing one electron-muon pair with opposite charge. The search targets a region of parameter  space where the kinematics of top squark pair production and top quark pair production is very  similar and makes use of the double-differential angular distributions of the leptons. No excess  above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop1  model, see Figures 16 and 17.


pdgid: S046STP
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AAD 2020AS searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for evidence  of top squarks in events containing either a pair of jets consistent with SM Higgs boson decay into  b-quarks or a same-flavour opposite-sign dilepton pair with an invariant mass consistent with a  Z boson. No significant excess over the expected background is observed. Limits at 95%  C.L. are set in Tstop6 simplified model. Assuming mass(chitilde_{{1}}()0) = 0 GeV, ttilde_{{1}} masses  up to 1220 GeV are excluded for mass(chitilde_{{2}}()0) around 900 GeV. Limits reduce down to  ttilde_{{1}} masses up to 900 GeV for mass(chitilde_{{2}}()0)=130 GeV. See their Fig. 10. Limits are  presented also in case of B(chitilde_2()0 --> chitilde_1()0 h) = 0 and 1, see their Fig. 11.


pdgid: S046STP
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AAD 2020AS searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for evidence  of top squarks in events containing either a pair of jets consistent with SM Higgs boson decay into  b-quarks or a same-flavour opposite-sign dilepton pair with an invariant mass consistent with a  Z boson. No significant excess over the expected background is observed. Limits at 95%  C.L. are set in simplified model featuring ttilde_{{2}} pair production, ttilde_2 --> ttilde_1 Z and  ttilde_1 --> b f f^' chitilde_1()0. Assuming mass(chitilde_{{1}}()0) = 300 GeV, and a mass  difference between ttilde_{{1}} and chitilde_{{1}}()0 of 40 GeV, ttilde_{{2}} masses up to 860 GeV  are excluded. See their Fig. 12.


pdgid: S046STP
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AAD 2020S searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing multiple jets and large notET. No significant excess above the Standard Model  expectations is observed. Exclusion limits at 95% C.L.  are set on top squark masses in the  Tstop1 model up to 1250 GeV for lightest neutralino masses below 200 GeV. Additional constraints  are set in the case where mass(ttilde) - mass(chitilde_{{1}}()0) ~ mass(t) for which top  squark masses in the range 300 -- 630 GeV are excluded. See their Fig. 13.


pdgid: S046STP
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AAD 2020S searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing multiple jets and large notET. No significant excess above the Standard Model  expectations is observed. Exclusion limits at 95% C.L.  are set on top squark masses in the  Tstop3 model in the range 300 -- 660 GeV. In case mass(ttilde) - mass(chitilde_{{1}}()0)  ~ 5 GeV or above, mass(ttilde) below 500 GeV are excluded. See their Fig. 13(b).


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AAD 2020V searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with two same-sign charged leptons (electrons or muons) and jets. No significant excess above the  Standard Model expectations is observed. Exclusion limits at 95% C.L. are set on the top  squark mass up to 765 GeV assuming ttilde_1 --> t chitilde_2()0 with chitilde_2()0 --> chitilde_1()+- W and  chitilde_1()+- --> chitilde_1()0 W. Masses of the charginos and lightest neutralinos are set as  mass(chitilde_{{1}}()0) = mass(ttilde_{{1}}) - 275 GeV, mass(chitilde_{{2}}()0) = mass(chitilde_{{1}}()0)  + 100 GeV and  mass(chitilde_{{1}}()+-) ~ mass(chitilde_{{1}}()0). See their Fig. 8(b).


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SIRUNYAN 2020AH searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  pair production of top squarks in events with a single isolated electron or muon, multiple jets and  large notET. No significant excess above the Standard Model expectations is observed. Limits  are set on the stop mass in the Tstop1, Tstop2 and Tstop8  simplified models, see Figures 6, 7 and  8, respectively.


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SIRUNYAN 2020T searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least two jets, and two isolated same-sign or three or more charged leptons  (electrons or muons). No significant excess above the Standard Model expectations is observed.  Limits are set on the gluino mass in the Tglu3A, Tglu3B, Tglu3C and Tglu3D simplified models, see  their Figure 7,  and in the Tglu1C and Tglu1B simplified models, see their Figures 8 and 9. Limits  are also set on the sbottom mass in the Tsbot2 simplified model, see their Figure 10, and on the  stop mass in the Tstop7 simplified model, see their Figure 11. Finally, limits are set on the  gluino mass in RPV simplified models where the gluino decays either via gtilde -->  q q qbar qbar + e / mu / tau or  via gtilde --> t b s, see Figure 12.


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SIRUNYAN 2020U searched in 77.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for the  pair production of top squarks in events with two hadronically decaying taus, jets identified as  originating from a b-quark and large notET. No significant excess above the Standard  Model expectations is observed. Limits are set on the stop mass in the Tstop11 simplified model  assuming the final state leptons are taus. Different values of the scalar tau mass are considered;  the impact on the lower bound is negligible.


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SIRUNYAN 2019AU searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at last one photon, jets, some of which are identified as originating from  b-quarks, and large notET. No significant excess above the Standard Model expectations is  observed.  In the framework of GMSB, limits are set on the gluino mass in the Tglu4C, Tglu4D and  Tglu4E simplified models, and on the top squark mass in the Tstop13 simplified model, see their  Figure 5.


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SIRUNYAN 2019S searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with zero or one charged leptons, jets and notET. The razor variables (M_{{R}} and  R^2) are used to categorize the events. No significant excess above the Standard Model  expectations is observed. Limits are set on the gluino mass in the Tglu3A and Tglu3C simplified  models, see Figures 22 and 23, and on the stop mass in the Tstop1 simplified model, see their  Figure 24.


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SIRUNYAN 2019U searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing one electron-muon pair with opposite charge. The search targets a region of  parameter space where the kinematics of top squark pair production and top quark pair production is  very similar, due to the mass difference between the top squark and the neutralino being close to  the top quark mass. No excess above the Standard Model expectations is observed. Limits are set on  the stop mass in the Tstop1 model, with mass(ttilde_{{1}})-mass(chitilde_{{1}}()0) close to  mass(t), see Figure 5.


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AABOUD 2018AQ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for top  squark pair production in final states with one isolated electron or muon, several energetic jets,  and missing transverse momentum. No significant excess over the Standard Model prediction is  observed. In case of Tstop1 models, top squark masses up to 940 GeV are excluded assuming  mass(chitilde_{{1}}()0) = 0 GeV, see their Fig. 20. If the top quark is not on-shell (3-body) decay,  exclusions up to 500 GeV are obtained for mass(chitilde_{{1}}()0) = 300 GeV.  Exclusions as a function  of mass(ttilde_{{1}})-mass(chitilde_{{1}}()0) are given in their Fig. 21.


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AABOUD 2018AQ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for top  squark pair production in final states with one isolated electron or muon, several energetic jets,  and missing transverse momentum. No significant excess over the Standard Model prediction is  observed. In case of Tstop3 models (4-body), top squark masses up to 370 GeV are excluded for  mass(ttilde) - mass(chitilde_{{1}}()0) as low as 20 GeV. Top squark masses below 195 GeV are  excluded for all mass(chitilde_{{1}}()0), see their Fig. 20 and Fig. 21.


pdgid: S046STP
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AABOUD 2018AQ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for top  squark pair production in final states with one isolated electron or muon, several energetic jets,  and missing transverse momentum. No significant excess over the Standard Model prediction is  observed. In case of Tstop2 models, top squark masses up to 840 GeV are excluded for mass(ttilde)  - mass(chitilde_{{1}}()+-) = 10 GeV. See their Fig. 23. Exclusion limits for this decay mode are  presented also in the context of Higgsino-LSP phenomenological MSSM models, where  mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) = 5 GeV, see their Fig 26.


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AABOUD 2018BV searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet identified as c-jet, large missing transverse energy and no  leptons. Good agreement is observed between the number of events in data and Standard Model  predictions. The results are translated into exclusion limits in Tstop4 models. In scenarios with  differences of the stop and neutralino masses below 100 GeV, stop masses below 500 GeV are  excluded. See their Fig.6 and Fig.7.


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AABOUD 2018BV searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet identified as c-jet, large missing transverse energy and no  leptons. Good agreement is observed between the number of events in data and Standard Model  predictions. The results are translated into exclusion limits in Tstop1 models. In scenarios with  massless neutralinos, top squark masses below 850 GeV are excluded. See their Fig.6.


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AABOUD 2018I searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet with a transverse momentum above 250 GeV and no leptons. Good  agreement is observed between the number of events in data and Standard Model predictions. The  results are translated into exclusion limits in Tstop3 models. Stop masses below 390 GeV are  excluded for mass(ttilde) - mass(chitilde_{{1}}()0) = mass(b). See their Fig.9(b).


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AABOUD 2018I searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one jet with a transverse momentum above 250 GeV and no leptons. Good  agreement is observed between the number of events in data and Standard Model predictions. The  results are translated into exclusion limits in Tstop4 models. In scenarios with differences of the  stop and neutralino masses around 5 GeV, stop masses below 430 GeV are excluded. See their  Fig.9(a).


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AABOUD 2018Y searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  direct pair production of top squarks in final states with two tau leptons, b-jets, and missing  transverse momentum. At least one hadronic  tau is required. No significant deviation from the  SM predictions is observed in the data. The analysis results are interpreted in Tstop5 models with  a nearly massless gravitino.  Top squark masses up to 1.16 TeV and tau slepton masses up to 1 TeV  are excluded, see their Fig 7.


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SIRUNYAN 2018AN searched in 19.7 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing one or two photons and a pair of top quarks from the decay of a pair of top  squark in a natural gauge-mediated scenario. The final state consists of a lepton (electron or  muon), jets and one or two photons. No significant excess above the Standard Model expectations is  observed. Limits are set on the stop mass in the Tstop12 simplified model, see their Figure 6.


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SIRUNYAN 2018C searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for the  pair production of top squarks in events with two oppositely charged leptons (electrons or muons), jets identified as originating from a b-quark and large notET. No significant excess  above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop1,  Tstop2 and Tstop11 simplified models, see their Figures 11 and 12. The Tstop1 and Tstop2 results  are combined with complementary searches in the all-hadronic and single lepton channels, see their  Figures 13 and 14.


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SIRUNYAN 2018D searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing identified hadronically decaying top quarks, no leptons, and notET. No  significant excess above the Standard Model expectations is observed. Limits are set on the stop  mass in the Tstop1 simplified model, see their Figure 8, and on the gluino mass in the Tglu3A,  Tglu3B, Tglu3C and Tglu3E simplified models, see their Figure 9.


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SIRUNYAN 2018DI searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  pair production of top squarks in events with a low transverse momentum lepton (electron or muon),  a high-momentum jet and significant missing transverse momentum. No significant excess above the  Standard Model expectations is observed. Limits are set on the stop mass in the Tstop3 and Tstop10  simplified models, see their Figures 7 and 8. A combination of this search with the all-hadronic  search is presented in Figure 9.


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 700 GeV are set  on the top squark mass in Tstop11 simplified models, assuming  mass(chitilde_{{1}}()0) = mass(ttilde) - 275 GeV and mass(chitilde_{{2}}()0) =  mass(chitilde_{{1}}()0) + 100 GeV. See their Figure 4(e).


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AABOUD 2017AX searched in 36 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing two jets identified as originating from b-quarks and large missing transverse  momentum, with or without leptons. No excess of events above the expected level of Standard Model  background was found. Exclusion limits at 95% C.L. are set on the masses of top squarks.  Assuming 50% BR for Tstop1 and Tstop2 simplified models, a ttilde_{{1}} mass below 880 (860)  GeV is excluded for mass(chitilde_{{1}}()0) = 0 (<250) GeV. See their Fig. 7(b).


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AABOUD 2017AY searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least four jets and large missing transverse momentum. No significant excess above  the Standard Model expectations is observed. Limits in the range 250 -- 1000 GeV are set on  the top squark mass in Tstop1 simplified models. For the first time, additional constraints are set  for the region mass(ttilde_{{1}}) ~ mass(t) + mass(chitilde_{{1}}()0), with exclusion of the  ttilde_1 mass range 235 -- 590 GeV. See their Figure 8.


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AABOUD 2017AY searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least four jets and large missing transverse momentum. No significant excess above  the Standard Model expectations is observed. Limits in the range 450-850 GeV are set on the top  squark mass in a mixture of Tstop1 and Tstop2 simplified models with BR=50% and assuming  mass(chitilde_{{1}}()+-)  - mass(chitilde_{{1}}()0) = 1 GeV and $m_{chi^0_1}<240,$GeV.  Constraints are given for various values of the BR. See their Figure 9.


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AABOUD 2017BE searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two opposite-charge leptons (electrons and muons) and large missing transverse  momentum. No significant excess above the Standard Model expectations is observed. Limits up to 720  GeV are set on the top squark mass in Tstop1 simplified models, assuming massless neutralinos. See  their Figure 9 (2-body area).


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AABOUD 2017BE searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two opposite-charge leptons (electrons and muons) and large missing transverse  momentum. No significant excess above the Standard Model expectations is observed. Limits up to 400  GeV are set on the top squark mass in Tstop3 simplified models, assuming  mass(ttilde_{{1}})-mass(chitilde_{{1}}()0) = 40 GeV. See their Figure 9 (4-body area).


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AABOUD 2017BE searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two opposite-charge leptons (electrons and muons) and large missing transverse  momentum. No significant excess above the Standard Model expectations is observed. Limits up to 430  GeV are set on the top squark mass in Tstop1 simplified models where top quarks are offshell,  assuming mass(ttilde_{{1}})-mass(chitilde_{{1}}()0) close to the W mass. See their Figure 9  (3-body area).


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AABOUD 2017BE searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two opposite-charge leptons (electrons and muons) and large missing transverse  momentum. No significant excess above the Standard Model expectations is observed. Limits up to 700  GeV are set on the top squark mass in Tstop2  simplified models, assuming  mass(ttilde_{{1}})-mass(chitilde_{{1}}()+-) = 10 GeV and massless neutralinos. See their Figure 10.


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KHACHATRYAN 2017 searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing four or more jets, no more than one lepton, and missing transverse momentum,  using the razor variables (M_{{R}} and R^2) to discriminate between signal and background  processes. No evidence for an excess over the expected background is observed. Limits are derived  on the stop mass in the Tstop1 simplified model, see Fig. 17.


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KHACHATRYAN 2017AD searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing at least four jets (including b-jets), missing transverse momentum and tagged  top quarks. No evidence for an excess over the expected background is observed. Top squark masses  in the range 250 -- 740 GeV and neutralino masses up to 240 GeV are excluded at 95%  C.L. See Fig. 12.


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KHACHATRYAN 2017AD searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing at least four jets (including b-jets), missing transverse momentum and tagged  top quarks. No evidence for an excess over the expected background is observed. Limits are derived  on the ttilde mass in simplified models that are a mixture of Tstop1 and Tstop2 with branching  fractions 50% for each of the two decay modes: top squark masses of up to 610 GeV and  neutralino masses up to 190 GeV are excluded at 95% C.L. The chitilde_{{1}}()+- and the  chitilde_{{1}}()0 are assumed to be nearly degenerate in mass, with a 5 GeV difference between  their masses. See Fig. 12.


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KHACHATRYAN 2017S searched in 18.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing multiple jets and missing transverse momentum, using the alpha_{{T}} variable to  discriminate between signal and background processes. No evidence for an excess over the expected  background is observed. Limits are derived on the stop mass in the Tstop4 model: for Deltam  = mass(ttilde) - mass(chitilde_{{1}}()0) equal to 10 and 80 GeV, masses of stop below 240 and  260 GeV are excluded, respectively. See their Fig.3.


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KHACHATRYAN 2017S searched in 18.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing multiple jets and missing transverse momentum, using the alpha_{{T}} variable to  discriminate between signal and background processes. No evidence for an excess over the expected  background is observed. Limits are derived on the stop mass in the Tstop3 model: for Deltam  = mass(ttilde) - mass(chitilde_{{1}}()0) equal to 10 and 80 GeV, masses of stop below 225 and  130 GeV are excluded, respectively. See their Fig.3.


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KHACHATRYAN 2017S searched in 18.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing multiple jets and missing transverse momentum, using the alpha_{{T}} variable to  discriminate between signal and background processes. No evidence for an excess over the expected  background is observed. Limits are derived on the stop mass in the Tstop2 model: assuming  mass(chitilde_{{1}}()+-) = 0.25 mass(ttilde) + 0.75 mass(chitilde_{{1}}()0), masses of stop up to 325  GeV and masses of the  neutralino up to 225 GeV are excluded. See their Fig.3.


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KHACHATRYAN 2017S searched in 18.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing multiple jets and missing transverse momentum, using the alpha_{{T}} variable to  discriminate between signal and background processes. No evidence for an excess over the expected  background is observed. Limits are derived on the stop mass in the Tstop2 model: assuming  mass(chitilde_{{1}}()+-) = 0.75 mass(ttilde) + 0.25 mass(chitilde_{{1}}()0), masses of stop up to 400  GeV are excluded for low neutralino masses. See their Fig.3.


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KHACHATRYAN 2017S searched in 18.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing multiple jets and missing transverse momentum, using the alpha_{{T}} variable to  discriminate between signal and background processes. No evidence for an excess over the expected  background is observed. Limits are derived on the stop mass in the Tstop1 model: assuming masses of  stop up to 500 GeV and masses of the neutralino up to 105 GeV are excluded. See their Fig.3.


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SIRUNYAN 2017AS searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with a single lepton  (electron or muon), jets, and large notET. No significant excess  above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop1,  Tstop2 and Tstop8 simplified models, see their Figures 5, 6 and 7.


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SIRUNYAN 2017AT searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  direct production of top squarks in events with jets and large notET. No significant excess  above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop1,  Tstop2 , Tstop3, Tstop4, Tstop8 and Tstop10 simplified models, see their Figures 9 to 14.


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AABOUD 2016D searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with an energetic jet and large missing transverse momentum. The results are interpreted as  95% C.L. limits on mass of stop decaying into a charm-quark and the lightest neutralino in  scenarios with mass(ttilde_{{1}})- mass(chitilde_{{1}}()0) between 5 and 20 GeV. See their Fig. 5.


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AABOUD 2016J searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with one isolated electron or muon, jets, and missing transverse momentum. For the direct  stop pair production model where the stop decays via top and lightest neutralino, the results  exclude at 95% C.L. stop masses between 745 GeV and 780 GeV for a massless chitilde_1()0.  See their Fig. 8.


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AAD 2016AY searched in 20 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events  with either two hadronically decaying tau leptons, one hadronically decaying tau and one light  lepton, or two light leptons. No significant excess over the Standard Model expectation is found.  Exclusion limits at 95% C.L. on the mass of top squarks decaying via tautilde to a nearly  massless gravitino are placed depending on mass(tautilde) which is ranging from the 87 GeV LEP  limit to mass(ttilde_{{1}}). See their Figs. 9 and 10.


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KHACHATRYAN 2016AV searched in 19.7 fb^{-1}  of p p collisions at sqrt(s) = 8 TeV for events with one or two isolated leptons, hadronic jets, b-jets and notET. No significant excess above the Standard Model expectations is observed.  Limits are set on the stop mass in the Tstop1 and Tstop2 simplified models, see Fig. 11.


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KHACHATRYAN 2016BK searched in 18.9 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with hadronic jets and notET. No significant excess above the Standard Model  expectations is observed. Limits are set on the stop mass in the Tstop1 and Tstop2 simplified  models, see Fig. 16.


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KHACHATRYAN 2016BS searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one energetic jet , no isolated leptons, and significant notET, using  the transverse mass variable M_{{T2}} to discriminate between signal and background processes. No  significant excess above the Standard Model expectations is observed. Limits are set on the stop  mass in the Tstop1 simplified model, see Fig. 11 and Table 3.


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KHACHATRYAN 2016Y searched in 19.7 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with one or two soft isolated leptons, hadronic jets, and notET. No significant excess  above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop3  simplified model, see Fig. 3.


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AAD 2015CJ searched in 20 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for evidence of  third generation squarks by combining a large number of searches covering various final states. Stop decays with and without charginos in the decay chain are considered and summaries of all ATLAS   Run 1  searches for direct stop production can be found in Fig. 4 (no intermediate charginos) and   Fig. 7 (intermediate charginos). Limits are set on stop masses in compressed mass regions regions,   with B(ttilde --> c chitilde_1()0) + B(ttilde --> b f f^' chitilde_1()0) = 1, see Fig.   5. Limits are also set on stop masses assuming that both the decay  ttilde --> t chitilde_1()0   and ttilde --> b chitilde_1()+- are possible,  with both their branching rations summing up to   1, assuming chitilde_1()+- --> W^(*)() chitilde_1()0 and mass(chitilde_{{1}}()+-) =  2 mass(chitilde_{{1}}()0), see Fig. 6. Limits on the mass of the next-to-lightest stop ttilde_{{2}},   decaying either to Z ttilde_1, h ttilde_1 or t chitilde_1()0, are also  presented,  see  Figs. 9 and 10.Interpretations in the pMSSM are also discussed, see Figs 13 -- 15.


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AAD 2015J interpreted the measurement of spin correlations in t tbar production using  20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV in exclusion limits on the pair  production of light ttilde_{{1}} squarks with masses similar to the top quark mass. The  ttilde_{{1}} is assumed to decay through ttilde_1 --> t chitilde_1()0 with predominantly  right-handed top and a 100% branching ratio. The data are found to be consistent with the  Standard Model expectations and masses between the top quark mass and 191 GeV are excluded, see  their Fig. 2


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KHACHATRYAN 2015AF searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for   events with at least two energetic jets and significant notET, using the transverse mass  variable M_{{T2}} to discriminate between signal and background processes. No significant excess   above the Standard Model expectations is observed. Limits are set on the stop mass in simplified   models where the decay ttilde --> t chitilde_1()0 takes place with a branching ratio of   100%, see Fig. 12. See also Table 5. Exclusions in the CMSSM, assuming tan(beta) =   30, A(0) = -2 max(mass(0), mass(1/2)) and mu > 0,  are also presented, see Fig. 15.


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KHACHATRYAN 2015AH searched in 19.4 or 19.7 fb^{-1} of p p collisions at sqrt(s) = 8  TeV for events containing either a fully reconstructed top quark, or events containing dijets  requiring one or both jets to originate from b-quarks, or events containing a mono-jet. No  significant excess above the Standard Model expectations is observed. Limits are set on the stop  mass in simplified models where the decay ttilde --> t chitilde_1()0 takes place with a  branching ratio of 100%, see Fig. 9. Limits are also set in simplified models where the  decays ttilde --> t chitilde_1()0 and ttilde --> b chitilde_1()+-, with  mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) = 5 GeV, each take place with a branching ratio of  50%, see Fig. 10, or with other fractions, see Fig. 11. Finally, limits are set in a  simplified model where the decay ttilde --> c chitilde_1()0 takes place with a branching ratio  of 100%, see Figs. 9, 10 and 11.


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KHACHATRYAN 2015AH searched in 19.4 or 19.7 fb^{-1} of p p collisions at sqrt(s) = 8  TeV for events containing either a fully reconstructed top quark, or events containing dijets  requiring one or both jets to originate from b-quarks, or events containing a mono-jet. No  significant excess above the Standard Model expectations is observed. Limits are set on the stop  mass in simplified models where the decay ttilde --> t chitilde_1()0 takes place with a  branching ratio of 100%, see Fig. 9. Limits are also set in simplified models where the  decays ttilde --> t chitilde_1()0 and ttilde --> b chitilde_1()+-, with  mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) = 5 GeV, each take place with a branching ratio  of 50%, see Fig. 10, or with other fractions, see Fig. 11. Finally, limits are set in a  simplified model where the decay ttilde --> c chitilde_1()0 takes place with a branching ratio  of 100%, see Figs. 9, 10, and 11.


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KHACHATRYAN 2015X searched in 19.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with at least two energetic jets, at least one of which is required to originate from a b quark, possibly a lepton, and significant notET,  using the razor variables (M(R) and R**2) to discriminate between signal and background processes.   No significant excess  above the Standard Model expectations is observed.  Limits are set on the   stop mass in simplified models where the decay ttilde --> t chitilde_1()0 and the decay ttilde --> b chitilde_1()+-, with mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) = 5 GeV,  take place with  branching ratios varying between 0 and 100%, see Figs. 15, 16 and 17.


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AAD 2014AJ searched in 20.1 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing four or more jets and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the masses of third-generation squarks in simplified models which either assume that the decay ttilde_1 --> t chitilde_1()0 takes place 100% of the time, see Fig. 8, or that this decay takes place 50% of the time, while the decay ttilde_1 --> b chitilde_1()+- takes place the other 50% of the time, see Fig. 9.


pdgid: S046STP
text:
AAD 2014BD searched in 20 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing one isolated lepton, jets and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the masses of third-generation squarks in simplified models which either assume that the decay ttilde_1 --> t chitilde_1()0 takes place 100% of the time, see Fig. 15, or the decay ttilde_1 --> b chitilde_1()+- takes place 100% of the time, see Fig. 16 -- 22. For the mixed decay scenario, see Fig. 23.


pdgid: S046STP
text:
AAD 2014F searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing two leptons (e or mu), and possibly jets and missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the masses of third-generation squarks in simplified models which either assume that the decay ttilde_1 --> b chitilde_1()+- takes place 100% of the time, see Figs. 14 -- 17 and 20, or that the decay ttilde_1 --> t chitilde_1()0 takes place 100% of the time, see Figs. 18 and 19.


pdgid: S046STP
text:
AAD 2014T searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for monojet-like and c-tagged events. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set on the masses of third-generation squarks in simplified models which assume that the decay ttilde_1 --> c chitilde_1()0 takes place 100% of the time, see Fig. 9 and 10. The results of the monojet-like analysis are also interpreted in terms of stop pair production in the four-body decay ttilde_1 --> b f f^' chitilde_1()0, see Fig. 11.


pdgid: S046STP
text:
CHATRCHYAN 2014AH searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with at least two energetic jets and significant notET, using the razor variables (M_{{R}}() and R^2()) to discriminate between signal and background processes. A second analysis requires at least one of the jets to be originating from a b-quark. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay ttilde --> t chitilde_1()0 takes place with a branching ratio of 100%, see Figs. 28 and 29. Exclusions in the CMSSM, assuming tan(beta) = 10, A_{{0}}() = 0 and mu >0, are also presented, see Fig. 26.


pdgid: S046STP
text:
CHATRCHYAN 2014R searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least three leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the stop mass in a natural higgsino NLSP simplified model (GMSB) where the decay ttilde --> b chitilde_1()+-, with chitilde_1()+- --> ( q q^' / lepton nu ) H , Z Gtilde, takes place with a branching ratio of 100% (the particles between brackets have a soft pT spectrum), see Figs. 4 -- 6.


pdgid: S046STP
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AABOUD 2017AF searched in 36 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of top squarks in events containing 2 leptons, jets, b-jets and notET. In Tstop6  model, assuming mass(chitilde_{{1}}()0) = 0 GeV, ttilde_{{1}} masses up to 850 GeV are excluded for  mass(chitilde_{{2}}()0) > 200 GeV.


pdgid: S046STP
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AABOUD 2017AF searched in 36 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of ttilde_{{2}} in events containing 2 leptons, jets, b-jets and notET. In  Tstop7 model, assuming mass(chitilde_{{1}}()0) = 50 GeV and 100% decays via Z boson,  ttilde_{{2}} masses up to 800 GeV are excluded. Exclusion limits are also shown as a function of  the ttilde_{{2}} branching ratios in their Figure 7.


pdgid: S046STP
text:
AABOUD 2017AF searched in 36 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of ttilde_{{2}} in events containing 2 leptons, jets, b-jets and notET. In  Tstop7 model, assuming mass(chitilde_{{1}}()0) = 50 GeV and 100% decays via higgs boson,  ttilde_{{2}} masses up to 880 GeV are excluded. Exclusion limits are also shown as a function of  the ttilde_{{2}} branching ratios in their Figure 7.


pdgid: S046STP
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AABOUD 2017AY searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least four jets and large missing transverse momentum. No significant excess above  the Standard Model expectations is observed. Limits are set on the top squark mass assuming three  pMSSM-inspired models. The first one, referred to as Higgsino LSP model, assumes  mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) = 5 GeV and mass(chitilde_{{2}}()0) -  mass(chitilde_{{1}}()0) = 10 GeV, with a mixture of decay modes as in Tstop1, Tstop2 and Tstop6. See  their Figure 10. The second and third models are referred to as Wino NLSP and well-tempered pMSSM  models, respectively. See their Figure 11 and Figure 12, and text for details on assumptions.


pdgid: S046STP
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AAD 2014B searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events  containing a Z boson, with or without additional leptons, plus jets originating from  b-quarks and significant missing transverse momentum. No excess over the expected SM background  is observed. Limits are derived in simplified models featuring ttilde_{{2}} production, with  ttilde_2 --> Z ttilde_1, ttilde_1 --> t chitilde_1()0 with a 100% branching ratio,  see Fig. 4, and in the framework of natural GMSB, see Fig. 6.


pdgid: S046STP
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CHATRCHYAN 2014U searched in 19.7 fb**-1 of p p collisions at sqrt(s) = 8 TeV for evidence of direct pair production of top squarks, with Higgs bosons in the decay chain. The search is performed using a selection of events containing two Higgs bosons, each decaying to a photon pair, missing transverse energy and possibly b-quark jets. No significant excesses over the expected SM backgrounds are observed. The results are interpreted in the context of a ``natural SUSY'' simplified model where the decays ttilde_1 --> b chitilde_1()+-, with chitilde_1()+- --> f f^' chitilde_1()0, and chitilde_1()0 --> H Gtilde, all happen with 100% branching ratio, see Fig. 4.


pdgid: S046STP
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KHACHATRYAN 2014C searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for evidence of direct pair production of top squarks, with Higgs or Z-bosons in the decay chain. The search is performed using a selection of events containing leptons and b-quark jets. No significant excesses over the expected SM backgrounds are observed. The results are interpreted in the context of a simplified model with pair production of a heavier top-squark mass eigenstate ttilde_{{2}} decaying to a lighter top-squark eigenstate ttilde_{{1}} via either ttilde_2 --> H ttilde_1 or ttilde_2 --> Z ttilde_1, followed in both cases by ttilde_1 --> t chitilde_1()0. The interpretation is performed in the region where the mass difference between the ttilde_{{1}} and chitilde_{{1}}()0 is approximately equal to the top-quark mass, which is not probed by searches for direct ttilde_{{1}} pair production, see Figs. 5 and 6. The analysis excludes top squarks with masses mass(ttilde_{{2}})< 575 GeV and mass(ttilde_{{1}})< 400 GeV at 95% C.L.


pdgid: S046STV
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AAD 2024BT searched in 140 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of stops decaying RPV to a lepton and a b-quark. The final state consists of two  resonant lepton-b pairs. No excess over the SM prediction is observed. Limits are set  on the mass of the ttilde assuming decays in a single lepton flavour, or into the three lepton  flavours with BR of 1/3, see their Figure 9. Limits are also extracted as a function of the  branching fraction into each lepton flavour, assuming that the ttilde decays only via ttilde --> b lepton, see  their Figure 8.


pdgid: S046STV
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TUMASYAN 2023L searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for    pairs of dijet resonances with the same mass in final states with at least four jets, for the      case where the four-jet production proceeds via an intermediate resonant state and for  nonresonant    production.  No significant excess above the Standard Model expectations is observed.   Limits  are   set in the nonresonant search on the top squark mass in the simplified model Tstop1aRPV with    lambda_{{312}} coupling, assuming B(d s) = 1, see their figure 12.    Limits are also set   on   resonant pair production of dijet resonances via high mass intermediate states and compared to  a   signal model of diquarks that decay into pairs of vector-like quarks, see their figures 10 and  11.


pdgid: S046STV
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TUMASYAN 2022AF searched for evidence of new long-lived particles decaying to leptons in p p   collisions at sqrt(s) = 13 TeV, corresponding to 118 (113) fb^{-1}  in the ee channel (emu   and mu mu) channels. The leptons are required to have transverse impact parameter values   between 0.01 and 10 cm and are not required to form a common vertex. No significant excess above   the Standard Model expectations is observed. Limits are set on the mass of the top squark in RPV   models with top squark pair production and ttilde --> b leptonbar and ttilde --> d leptonbar, see   their Figure 4, which contains a wider range of lifetime limits. Limits are also set on a   gauge-mediated SUSY breaking model, where the next-to-lightest SUSY particle is a slepton and the   lightest SUSY particle a gravitino Gtilde, see their Figure 5, which also contains a wider   range of lifetime limits. Limits are also set in a model that produces BSM Higgs bosons (H) with a   mass of 125 GeV through gluongluon fusion, where the H decays to two long-lived scalars S, each  of  which decays to two oppositely charged and same-flavor leptons.


pdgid: S046STV
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SIRUNYAN 2021U searched in 132 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  supersymmetry in events with displaced tracks and displaced vertices associated with a dijet  system. No significant excess above the Standard Model expectations is observed. Limits are set on    long-lived gluinos in an RPC GMSB SUSY model of gluino pair production, with gtilde --> g Gtilde, see    their Figure 9, in Tglu1A in a mini-split model, see their Figure 10, and in an RPV model of gluino  pair production, with gtilde --> t b s with coupling lambda_{{323}}^'', see their Figure 11.  Limits are also set on long-lived top squarks in Tstop2RPV, see their Figure 12, in an RPV model  with ttilde --> d leptonbar and lambda_{{x31}}^' coupling, see their Figure 13, and in a    dynamical RPV model with ttilde --> dbar dbar via a nonholomorphic RPV coupling eta_{{311}}^'',  see their Figure 14. The best mass limit is achieved in all cases at ctau = 30 mm.


pdgid: S046STV
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SIRUNYAN 2021V searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for   supersymmetry in events with one charged lepton (e+- or mu+-) and >=7 jets. No   significant excess above the Standard Model expectations is observed. Limits are set on an RPV SUSY   model like Tstop1 with the additional decay chitilde_1()0 --> q q q with coupling   lambda_{{abc}}^'', with a,b,c in {1,2}, and on a stealth SUSY model called SYY,   with one scalar particle S with even R-parity and its superpartner Stilde, both singlets   under all SM interactions, and with a portal mediated by loop interactions involving a new   vectorlike messenger field (Y), where pair produced top squarks decay as ttilde --> t g Stilde, and   Stilde --> Gtilde S, and S --> g g, see their Figure 6 and 7.


pdgid: S046STV
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AAD 2020M searched for long-lived particles decaying into hadrons and at least one muon in  events containing a displaced muon track and a displaced vertex. The analysis uses a dataset of  p p collisions at sqrt(s) = 13 TeV corresponding to an integrated luminosity of 136  fb^{-1}. Using the Tstop3RPV simplified model, top squarks with masses up to 1.7 TeV are  excluded for a lifetime of 0.1 ns, and masses below 1.3 TeV are excluded for lifetimes between 0.01  ns and 30 ns, see their Fig. 7. The dependence on the RPV coupling lambda_{{23k}} multiplied by  costheta_{{t}}, with theta_{{t}} the mixing angle between the left- and right-handed ttilde  squarks, is also shown, see their Fig. 7.


pdgid: S046STV
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SIRUNYAN 2019BI searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in  final states with two muons and two jets, or with one muon, two jets, and missing transverse  momentum.  Limits are set in a model of pair-produced, prompt or long-lived top squarks with  R-parity violating decays to a b-quark and a lepton (Tstop2RPV), branching fraction of  ttilde --> b mu equal to 1/3 and ctau between 0.1 cm and 10 cm in the case of  long-lived top squarks. See their Fig. 10.


pdgid: S046STV
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SIRUNYAN 2019BJ searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in  final states with two electrons and two jets, or with one electron, two jets, and missing  transverse momentum. Limits are set in a model of pair-produced, prompt top squarks with R-parity  violating decays to a b-quark and a lepton (Tstop2RPV), assuming branching fraction of  ttilde --> b e equal to 1/3 and ctau = 0 cm. See their Fig.10.


pdgid: S046STV
text:
AABOUD 2018BB searched in 36.7 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  massive colored resonances which are pair-produced and decay into two jets.  No significant  deviation from the background prediction is observed. Results are interpreted in a SUSY simplified  model as Tstop1RPV with ttilde --> d s. Top squarks with masses in the range 100 -- 410  GeV are excluded, see their Figure 9(a). The lambda_{{312}}^'' coupling is assumed to be  sufficiently large for the decays to be prompt, but small enough to neglect the single-top-squark  resonant production through RPV couplings.


pdgid: S046STV
text:
AABOUD 2018BB searched in 36.7 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  massive coloured resonances which are pair-produced and decay into two jets. No significant  deviation from the background prediction is observed. Results are interpreted in Tstop1RPV. Top  squarks with masses in the range 100 -- 470 GeV or 480 -- 610 GeV are excluded, see  their Figure 9(b). The lambda_{{323}}^'' coupling is assumed to be sufficiently large for the  decays to be prompt, but small enough to neglect the single-top-squark resonant production through  RPV couplings.


pdgid: S046STV
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AABOUD 2018P searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  pair-produced top squarks that decay through RPV lambda_{{i33}}^' (i = 1, 2, 3) couplings to a  final state with two leptons and two jets, at least one of which is identified as a b-jet. No  significant excess is observed over the SM background. In the Tstop2RPV model, lower limits on the  top squark masses between 600 and 1500 GeV are set depending on the branching fraction to b e,  b mu, and b tau final states. See their Figs 6 and 7.


pdgid: S046STV
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SIRUNYAN 2018AD searched in 2.6 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived particles by exploiting the multiplicity of displaced jets to search for the presence of  signal decays occurring at distances between 1 and 1000 mm. Limits are set in a model of  pair-produced, long-lived top squarks with R-parity violating decays to a b-quark and a lepton,  see their Figure 3.


pdgid: S046STV
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SIRUNYAN 2018DV searched in 38.5 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived particles in events with multiple jets and two displaced vertices composed of many  tracks. No events with two well-separated high-track-multiplicity vertices were observed. Limits  are set on the stop and the gluino mass in RPV models of supersymmetry where the stop (gluino) is  decaying solely into dijet (multijet) final states, see their Figures 6 and 7.


pdgid: S046STV
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SIRUNYAN 2018DY searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  the pair production of resonances, each decaying to two quarks. The search is conducted separately  in a boosted (two-jet) and resolved (four-jet) jet topology. The mass spectra are found to be  consistent with the Standard Model expectations. Limits are set on the stop mass in the Tstop3RPV  and Tstop1RPV simplified models,  see their Figure 11.


pdgid: S046STV
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AABOUD 2017AI searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more isolated lepton, at least eight jets, either zero or many b-jets, for  evidence of R-parity violating decays of the top squark. No significant excess above the  Standard Model expectations is observed. Limits up to 1.25 (1.10) TeV are set on the top squark  mass in R-parity-violating supersymmetry models where ttilde_{{1}} decays for a bino LSP as:  ttilde --> t chitilde_1()0 and for a higgsino LSP as ttilde -->  t chitilde_1,2()0/b chitilde_1()+. These  is followed by the decays through the non-zero lambda_{{323}}^'' coupling chitilde_1,2()0 --> t b s,  chitilde_1()+- --> b b s. See their Figure 10 and text for details on model assumptions.


pdgid: S046STV
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AAD 2016AM searched in 17.4 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events  containing two large-radius hadronic jets. No deviation from the background prediction is observed.  Top squarks with masses between 100 and 315 GeV are excluded at 95% C.L. in the hypothesis  that they both decay via R-parity violating coupling lambda_{{323}}^"() to b- and  s-quarks. See their Fig. 10.


pdgid: S046STV
text:
KHACHATRYAN 2015L searched in 19.4 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for    pair  production of heavy resonances decaying to pairs of jets in four jet events. No significant    excess above the Standard Model expectations is observed.  Limits are set on the stop mass in R-parity-violating supersymmetry models where  ttilde --> q q (lambda(312)**'' notequal 0), see Fig. 6 (top) and ttilde --> q b (lambda(323)**'' notequal 0), see Fig. 6 (bottom).


pdgid: S046STV
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KHACHATRYAN 2014T searched in 19.7 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with tau-leptons and b-quark jets, possibly with extra light-flavour jets. No excess above the Standard Model expectations is observed. Limits are set on stop masses in RPV SUSY models with LQDbar couplings, in two simplified models. In the first model, the decay ttilde --> tau b is considered, with lambda_{{333}}^'()not=0, see Fig. 3. In the second model, the decay ttilde --> chitilde()+- b, with the subsequent decay chitilde()+- --> q q tau+- is considered, with lambda_{{3jk}}^'()not=0 and the mass splitting between the top squark and the charging chosen to be 100 GeV, see Fig. 4.


pdgid: S046STV
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AAD 2021B searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with at least eight jets and at least 5 b-jets, for evidence of R-parity violating decays of  the top squark. No significant excess above the Standard Model expectations is observed. Limits up  to 950 GeV are set on the top squark mass in Tstop4RPV simplified model. See their Figure 7 for  more detailed mass bounds.


pdgid: S046STV
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KHACHATRYAN 2016AC searched in 19.7 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with low missing transverse momentum, two oppositely charged electrons or muons, and at  least five jets, at least one of which is a b-jet, for evidence of R-parity violating,  charging-mediated decays of the top squark. No significant excess above the Standard Model  expectations is observed. Limits are set on the stop mass in R-parity-violating supersymmetry  models where ttilde --> b chitilde_1()+- with chitilde_1()+- --> lepton+- j j,  lambda_{{ijk}}^'  not= 0 (i,j, k <= 2), and with mass(ttilde) -  mass(chitilde_{{1}}()+-) =  100 GeV, see Fig. 3.


pdgid: S046STV
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KHACHATRYAN 2016BX searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing 4 leptons coming from R-parity-violating decays of chitilde_1()0 --> lepton lepton nu  with lambda_{{121}} not= 0 or lambda_{{122}} not= 0. No excess over the expected  background is observed. Limits are derived on the gluino, squark and stop masses, see Fig. 23.


pdgid: S046STV
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KHACHATRYAN 2015E searched for long-lived particles decaying to leptons in 19.7 fb^{-1} of  p p collisions at sqrt(s) = 8 TeV. Events were selected with an electron and muon with  opposite charges and each with transverse impact parameter values between 0.02 and 2 cm.  Limits  are set on SUSY benchmark models with pair production of top squarks decaying into an e mu  final state via RPV interactions. See their Fig. 2


pdgid: S046GNO
text:
HAYRAPETYAN 2024M searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of wino- and Higgsino-like charginos in final states with one or more disappearing tracks  from the decay chitilde_1()+- --> pi+- chitilde_1()0 where the soft pion is not reconstructed,  notET, and varying numbers of jets, b-tagged jets, electrons, and muons. No significant  excess above the Standard Model expectations is observed. Limits are set on the btilde mass in  the model Tbot1LL for various proper decay lengths ctau of the chitilde_{{1}}()+- as well as on  the ttilde mass in the model Tstop1LL, see their Fig. 10. Limits are also set in the model  Tglu1LL, see their Fig. 11. In addition, limits are set in specific pure wino as well as pure  higgsino dark matter models, in which the relationships among the electroweakino masses, the  chitilde_{{1}}()+- lifetime, and the chitilde_{{1}}()+- decay width are constrained by radiative  corrections that account for a large difference between the LSP mass and the SUSY-breaking scale,  see their Fig. 12.


pdgid: S046GNO
text:
HAYRAPETYAN 2024P searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of gluino pair production in events with long-lived particles with mean proper decay  lengths between 0.1 and 1000 mm, whose decay products produce a final state with at least one  displaced vertex and large notET. No significant excess above the Standard Model expectations  is observed. Limits are set on the gtilde mass in a model for split SUSY, shown in Fig. 8,  where the SUSY breaking scale is assumed to be >> E6 TeV, and all scalar masses are set  to that scale, except for a single, fine-tuned, Higgs boson mass. The decay is as in the model  Tglu1A, but the gtilde is long-lived because of its decay through a high-mass, virtual squark.  Limits are also set in a GMSB model, where the pair-produced gtilde decays to a gluon and a  nearly massless gravitino Gtilde, see their Fig. 9.


pdgid: S046GNO
text:
HAYRAPETYAN 2024Q searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of stealth supersymmetry in final states with two photons and jets, and low notET.  No significant excess above the Standard Model expectations is observed. The investigated models  include a singlet scalar boson S, and its SUSY fermion Stilde. In the investigated models,  either gluinos or squarks are pair produced and then each decay to a chitilde_{{1}}()0 and a gluon  or squark, respectively, followed by the decays chitilde_1()0 --> gamma Stilde,  Stilde --> Gtilde S  and S --> g g. Limits are set on the gtilde and the qtilde mass, see their Fig. 4.


pdgid: S046GNO
text:
AAD 2023AB searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for an  excess of events with one photon, jets and notET. No significant excess above the Standard  Model predictions is observed. Limits are set on the mass of pair produced gluinos decaying to  gtilde --> q q chitilde_1()0 followed by chitilde_1()0 --> gamma Gtilde or chitilde_1()0 --> X Gtilde with  equal probability, see Figure 4. X can be Z (left figure) or h (right figure).


pdgid: S046GNO
text:
AAD 2023AE searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with 2 lepton with same flavour and opposite sign, plus jets and notET, defining  signal  region with the dilepton invariant mass both on- and off-shell with respect to the Z  boson. No  significant excess above the Standard Model  predictions is observed. Limits are set  on models of  strong and electroweak production. In this case, limits are placed on the mass of  pair-produced   gluinos, assuming a scenario like in Tglu1G,  see figure 16.


pdgid: S046GNO
text:
AAD 2023AE searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events   with 2 lepton with same flavour and opposite sign, plus jets and notET, defining  signal  region with the dilepton invariant mass both on- and off-shell with respect to the Z  boson. No  significant excess above the Standard Model  predictions is observed. Limits are set  on models of  strong and electroweak production. In this case, limits are placed on the gluino  mass assuming  gluino pair production, assuming a scenario like in Tglu1H,  see figure 16.


pdgid: S046GNO
text:
AAD 2023AL searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with 0 or 1 lepton and at least three b-tagged jets. No significant excess above the Standard  Model prediction is observed. Results are interpreted in terms of gluino pair production followed  by the decay of gluinos into off-shell third generation squarks, yielding final states with top and  bottom quarks, and missing transverse momentum from a chitilde_{{1}}()0 LSP. Limits are set on the  mass of the gluino as a function of the chitilde_{{1}}()0 assuming B(gtilde --> ttilde t) =  100% or B(gtilde --> btilde b) = 100%, see figure 10.


pdgid: S046GNO
text:
AAD 2023AL searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with 0 or 1 lepton and at least three b-tagged jets. No significant excess above the Standard  Model prediction is observed. Results are interpreted in terms of gluino pair production followed  by the decay of gluinos into off-shell third generation squarks, yielding final states with top and  bottom quarks, and missing transverse momentum from a chitilde_{{1}}()0 LSP. Limits are set on the  mass of the gluino as a function of mass(chitilde_{{1}}()0), assuming B(gtilde --> ttilde t) +  B(gtilde --> btilde b) + B(gtilde --> t b chitilde_1()+-) = 100%, and  mass(chitilde_{{1}}()+-)-mass(chitilde_{{1}}()0) = 2 GeV, see figures 11 -- 13.


pdgid: S046GNO
text:
TUMASYAN 2023AY searched in 138 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  evidence of gluino pair production in events with a single electron or muon and multiple hadronic  jets. No significant excess above the Standard Model expectations is observed. Limits are set in  the models Tglu3A and Tglu1B, see their figure 11. For Tglu1B, the chargino mass is set to  mass(chitilde_{{1}}()+-) = 0.5 (mass(gtilde) + mass(chitilde_{{1}}()0)).


pdgid: S046GNO
text:
AAD 2022U searched for the signature of disappearing track from a long-lived chargino in 139  fb^{-1} of p p collisions at sqrt(s) = 13 TeV. Long-lived charginos decay into  quasi-degenerate neutralino emitting a low-momentum particle whose identification is not attempted.  The signal is identified by requiring short tracklets in the four pixel layers with no continuation  in the SCT (strip) detector. The main background from fake tracklets is estimated directly with the  data. No significant excess above the background prediction is found. The results are interpreted  in an AMSB scenario (win LSP), on p p --> chitilde+- chitilde+- and p p --> chitilde+- chitilde_1()0,  assuming B(chitilde+- --> chitilde_1()0 pi+-) = 100%, see their figure 7. Results are  also interpreted in a higgsino-LSP model, with p p --> chitilde+- chitilde-+ , and p p --> chitilde+- chitilde_1,2()0,  assuming B(chitilde+- --> chitilde_1()0 pi+-) = 95.5%, B(chitilde+- --> chitilde_1()0 e+-)  = 3%, B(chitilde+- --> chitilde_1()0 mu+-) = 1.5%, see their figure 8. Finally,  results are interpreted in a simplified model of gluino pair production, with p p --> gtilde gtilde and  B(gtilde --> q q chitilde_1()0) = B(gtilde --> q q chitilde+) = B(gtilde --> q q chitilde-)  = 1/3, see their figure 9.


pdgid: S046GNO
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TUMASYAN 2022V searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for   evidence of electroweakino pair production with decay to two Higgs bosons H, with H --> b bbar,   resulting either in 4 resolved b-jets or two large-radius jets, and large notET. No   significant excess above the Standard Model expectations is observed. Limits are set on the mass of   chitilde_{{2}}()0 and chitilde_{{1}}()+- in the models Tn1n1A, see their Figures 11 and 12, or in  a  model where higgsino-like nearly mass degenerate chitilde_{{2}}()0 and chitilde_{{3}}()0 are  pair  produced and each decay to H and a bino-like chitilde_{{1}}()0, see their Figure 13.  Limits are  also set on the gluino mass in the model Tglu1I, see their Figure 14.


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AAD 2021AK searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for pair  production of gluinos and squarks in events with a single isolated electron or muon, originating  from the decay of a W boson, multiple jets and significant notET. No significant excess  above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1B  simplified model and on the squark mass in the Tsqk3 simplified model, see their Figure 8.


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AAD 2021X searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for the decay  of long-lived R-hadrons stopped by the calorimeter, producing high-momentum jets resulting in large  out-of-time energy deposits in the calorimeters. These decays are detected using data collected  during periods in the LHC bunch structure when collisions are absent. No significant excess above  the predicted background is observed. Limits are set on the R-hadron mass  in the Tglu1A simplified  model ad a function of the R-hadron lifetime, for different mass(chitilde_{{1}}()0). See Figures 9, 10.


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SIRUNYAN 2021AD searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  supersymmetry in events with multiple jets, no leptons, and large notET. No significant  excess above the Standard Model expectations is observed. Limits are set on the top squark mass in  the simplified models Tstop1, Tstop2 with mass(chitilde_{{1}}()+-) = (mass(ttilde) +  mass(chitilde_{{1}}()0))/2, and a 50:50 mixture of these with mass(chitilde_{{1}}()+-) -  mass(chitilde_{{1}}()0) = 5 GeV, see their Figure 8. Limits are also set on the top squark mass for 10  GeV < mass(ttilde) - mass(chitilde_{{1}}()+-) < 80 GeV in the simplified models  Tstop2, Tstop 3, and Tstop4, see their Figure 9. For indirect top squark production, limits are set  on the gluino mass in the simplified models Tglu3A, Tglu3C with mass(ttilde) -  mass(chitilde_{{1}}()0) = 20 GeV, and Tglu3D with mass(chitilde_{{1}}()+-) - mass(chitilde_{{1}}()0) =  5 GeV, see their Figure 10.


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SIRUNYAN 2021M searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for    supersymmetry in events with two opposite-sign same-flavor leptons (electrons, muons) and    notET.  No significant excess above the Standard Model expectations is observed. Limits are    set on the gluino mass in the simplified model Tglu4C, see their Figure 10, on the    chitilde_{{2}}()0 and chitilde_{{1}}()+- mass in Tchi1n2Fa, see their Figure 11, on the    chitilde_{{1}}()0 mass in Tn1n1C and Tn1n1B for   mass(chitilde_{{2}}()0)=mass(chitilde_{{1}}()+-)=mass(chitilde_{{1}}()0), see their Figure 12. Limits are   also set on the light squark mass for the  simplified model Tsqk2A, on the sbottom mass in Tsbot3,   see their Figure 13, and on the slepton  mass in direct electroweak pair production of   mass-degenerate left- and right-handed sleptons  (selectrons and smuons), see their Figure 14.


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AAD 2020AL searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with 8 or more jets and moderate missing transverse momentum. The selection makes requirements  according to the number of b-tagged jets and the scalar sum of masses of large-radius jets. No  significant excess above the Standard Model expectations is observed. Limits up to about 2 TeV are  set on the gluino mass in Tglu1E simplified model. Limits up to about 1.8 TeV are set on the gluino  mass in Tglu3A simplified model. See their Fig. 10(a).


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AAD 2020V searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with same-sign charged leptons (electrons or muons) and jets. No significant excess over the  Standard Model expectation is observed. In the Tglu1E model, considering off-shell intermediate  W and Z bosons in the decay chains, gluino masses are excluded at 95% C.L. up to 1600  GeV for neutralino masses of 100 GeV or above (up to 1000 GeV). See their Fig. 7(a).


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SIRUNYAN 2020BJ searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing two hadronically decaying, highly energetic Z bosons and large notET.  No significant excess above the Standard Model expectations is observed. Limits are set on the  gluino mass in the Tglu1H simplified model, see their Figure 9.


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SIRUNYAN 2020E searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with a single electron or muon and multiple jets, including at least one identified as  originating from a b-quark, and large notET. No significant excess above the Standard  Model expectations is observed. Limits are set on the gluino mass in the Tglu3A simplified model,  see their Fig. 10, and the Tglu3C simplified model, see their Fig. 11.


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AABOUD 2019I searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with hadronic jets, 1 or two hadronically decaying tau and notET. In Tglu1F,  gluino masses are excluded at 95% C.L. up to 2000 GeV for neutralino masses of 100 GeV or  below. Neutralino masses up to 1000 GeV are excluded for all gluino masses below 1400 GeV. See  their Fig. 9. Limits are also presented in the context of Gauge-Mediated Symmetry Breaking models:  in this case, values of Lambda below 110 TeV are excluded at the 95% CL for all values of  tanbeta in the range 2 < tanbeta < 60, see their Fig 10.


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SIRUNYAN 2019CE searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  new particles decaying to a photon and two gluons in events with at least three large-radius jets  of which two have substructure and are composed of a photon and two gluons. No statistically  significant excess is observed above the SM background expectation. Upper limits at 95%  confidence level on the cross section for gluino pair production are set, using a simplified  Tglu1A-like stealth SUSY model. Gluino masses up to 1500-1700 GeV are excluded, depending on the  neutralino mass, with the highest exclusion set for mass(chitilde_{{1}}()0) = 200 GeV. See their Fig 4.


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AABOUD 2018AR searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  gluino pair production in events containing large missing transverse momentum and several energetic  jets, at least three of which must be identified as originating from b-quarks. No excess is  found above the predicted background. In Tglu3A models, gluino masses of less than 1.97 TeV are  excluded for mass(chitilde_{{1}}()0) below 300 GeV, see their Fig. 10(a). Interpretations are also  provided for scenarios where Tglu3A modes mix with Tglu2A and Tglu3D, see their Fig 11.


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AABOUD 2018AR searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  gluino pair production in events containing large missing transverse momentum and several energetic  jets, at least three of which must be identified as originating from b-quarks. No excess is  found above the predicted background. In Tglu2A models,  gluino masses of less than 1.92 TeV are  excluded for mass(chitilde_{{1}}()0) below 600 GeV, see their Fig. 10(b). Interpretations are also  provided for scenarios where Tglu2A modes mix with Tglu3A and Tglu3D, see their Fig 11.


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AABOUD 2018AS searched for in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  gluino pair production in the context of AMSB or phenomenological MSSM scenarios with wino-like LSP  and long-lived charginos. Events with a disappearing track due to a low-momentum pion  accompanied  by at least four jets are considered. No significant excess above the Standard Model expectations  is observed.  Exclusion limits are set at 95% confidence level on the mass of gluinos for  different chargino lifetimes. Gluino masses up to 1.65 TeV are excluded assuming a chargino mass of  460 GeV and lifetime of 0.2 ns, corresponding to a mass-splitting between the charged and neutral  wino of around 160 MeV. See their Fig. 9.


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AABOUD 2018BJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in  events with two opposite-sign charged leptons (electrons and muons), jets and missing transverse  momentum, with various requirements to be sensitive to signals with different kinematic endpoint  values in the dilepton invariant mass distribution. The data are found to be consistent with the SM  expectation. Results are interpreted in the Tglu1G model: gluino masses below 1850 GeV are excluded  for mass(chitilde_{{1}}()0) = 100 GeV, see their Fig. 12(a).


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AABOUD 2018BJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in  events with two opposite-sign charged leptons (electrons and muons), jets and missing transverse  momentum, with various requirements to be sensitive to signals with different kinematic endpoint  values in the dilepton invariant mass distribution. The data are found to be consistent with the SM  expectation. Results are interpreted in the Tglu1H model: gluino masses below 1650 GeV are excluded  for mass(chitilde_{{1}}()0) = 100 GeV, see their Fig. 13(a).


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AABOUD 2018U searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with at least one isolated photon, possibly jets and significant transverse momentum targeting  generalised models of gauge-mediated SUSY breaking. No significant excess of events is observed  above the SM prediction. Results for the di-photon channel are interpreted in terms of lower limits  on the masses of gluinos in Tglu4B models, which reach as high as 2.3 TeV. Gluinos with masses  below 2.15 TeV are excluded for any NLSP mass, see their Fig. 8.


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AABOUD 2018U searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with at least one isolated photon, possibly jets and significant transverse momentum targeting  generalised models of gauge-mediated SUSY breaking. No significant excess of events is observed  above the SM prediction. Results of the gamma + jets + notET channel are interpreted in  terms of lower limits on the masses of gluinos in GGM higgsino-bino models (mix of Tglu4B and  Tglu4C), which reach as high as 2050 GeV. Gluino masses below 1600 GeV are excluded for any NLSP  mass provided that mass(gtilde)-mass(chitilde_{{1}}()0)> 50 GeV. See their Fig. 11.


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AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in the Tglu1A model: gluino masses below 2030 GeV  are excluded for massless LSP, see their Fig. 13(b).


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AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in the Tglu1B model. Assuming that  mass(chitilde_{{1}}()+-) = 0.5 (mass(gtilde) + mass(chitilde_{{1}}()0)), gluino masses below 1980 GeV  are excluded for massless LSP, see their Fig. 14(c). Exclusions are also shown assuming  mass(chitilde_{{1}}()0) = 60 GeV, see their Fig. 14(d).


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AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in the Tglu1E model: gluino masses below 1750 GeV  are excluded for mass(chitilde_{{1}}()0) = 1 GeV and any mass(chitilde_{{2}}()0) above 100 GeV, see their  Fig. 15. Gluino mass exclusion up to 2 TeV is found for mass(chitilde_{{2}}()0) = 1 TeV.


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SIRUNYAN 2018AC searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with a single electron or muon and multiple jets. No significant excess above the Standard  Model expectations is observed. Limits are set on the gluino mass in the Tglu3A and Tglu1B  simplified models, see their Figure 5.


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SIRUNYAN 2018M searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more high-momentum Higgs bosons, decaying to pairs of b-quarks, and large  notET. No significant excess above the Standard Model expectations is observed. Limits are  set on the gluino mass in the Tglu1I and Tglu1J simplified models, see their Figure 3.


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.75 TeV are set  on the gluino mass in Tglu3A simplified models in case of off-shell top squarks and for  mass(chitilde_{{1}}()0) = 100 GeV. See their Figure 4(a).


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.57 TeV are set  on the gluino mass in Tglu1E simplified models (2-step models) for mass(chitilde_{{1}}()0) = 100 GeV.  See their Figure 4(b).


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.86 TeV are set  on the gluino mass in Tglu1G simplified models for mass(chitilde_{{1}}()0) = 200 GeV. See their Figure  4(c).


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AABOUD 2017AR searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one isolated lepton, at least two jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 2.1 TeV are set  on the gluino mass in Tglu1B simplified models, with  x = (mass(chitilde_{{1}}()+-)-mass(chitilde_{{1}}()0)) /  (mass(gtilde)-mass(chitilde_{{1}}()0)) = 1/2.Similar limits are obtained for variable  x and fixed  neutralino mass, mass(chitilde_{{1}}()0) = 60 GeV. See their Figure 13.


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AABOUD 2017AR searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one isolated lepton, at least two jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.74 TeV are set  on the gluino mass in Tglu1E simplified model. Limits up to 1.7 TeV are also set on pMSSM models  leading to similar signal event topologies. See their Figure 13.


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AABOUD 2017AY searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least four jets and large missing transverse momentum. No significant excess above  the Standard Model expectations is observed. Limits up to 1.8 TeV are set on the gluino mass in  Tglu3A simplified models assuming mass(ttilde_{{1}}) - mass(chitilde_{{1}}()0) = 5 GeV. See their  Figure 13.


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AABOUD 2017AZ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least seven jets and large missing transverse momentum. Selected events are further  classified based on the presence of large R-jets or b-jets and no leptons. No significant  excess above the Standard Model expectations is observed. Limits up to 1.8 TeV are set on the  gluino mass in Tglu1E simplified models. See their Figure 6b.


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AABOUD 2017AZ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least seven jets and large missing transverse momentum. Selected events are further  classified based on the presence of large R-jets or b-jets and no leptons. No significant  excess above the Standard Model expectations is observed. Limits up to 1.54 TeV are set on the  gluino mass in Tglu3A simplified models. See their Figure 7a.


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AABOUD 2017N searched in 14.7 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with 2 same-flavor, opposite-sign leptons (electrons or muons), jets and large missing  transverse momentum. In Tglu1J models, gluino masses are excluded at 95% C.L. up to 1300 GeV  for mass(chitilde_{{1}}()0) = 0 GeV and mass(chitilde_{{2}}()0) = 1100 GeV. See their Fig. 12 for  exclusion limits as a function of mass(chitilde_{{2}}()0). Limits are also presented assuming  mass(chitilde_{{2}}()0) = mass(chitilde_{{1}}()0) + 100 GeV, see their Fig. 13.


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AABOUD 2017N searched in 14.7 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with 2 same-flavor, opposite-sign leptons (electrons or muons), jets and large missing  transverse momentum. In Tglu1H models, gluino masses are excluded at 95% C.L. up to 1310 GeV  for mass(chitilde_{{1}}()0) < 400 GeV and assuming mass(chitilde_{{2}}()0) = (mass(gtilde) +  mass(chitilde_{{1}}()0))/2. See their Fig. 15.


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AABOUD 2017N searched in 14.7 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with 2 same-flavor, opposite-sign leptons (electrons or muons), jets and large missing  transverse momentum. In Tglu1G models, gluino masses are excluded at 95% C.L. up to 1700 GeV  for small mass(chitilde_{{1}}()0). The results probe kinematic endpoints as small as  mass(chitilde_{{2}}()0) - mass(chitilde_{{1}}()0) = (mass(gtilde) - mass(chitilde_{{1}}()0))/2  = 50 GeV. See their Fig. 14.


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KHACHATRYAN 2017 searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing four or more jets, no more than one lepton, and missing transverse momentum,  using the razor variables (M_{{R}} and R^2) to discriminate between signal and background  processes. No evidence for an excess over the expected background is observed. Limits are derived  on the gluino mass in the Tglu1A, Tglu2A and Tglu3A simplified models, see Figs. 16 and 17. Also,  assuming gluinos decay only via three-body processes involving third-generation quarks plus a  neutralino/chargino, and assuming mass(chitilde_{{1}}()+-) = mass(chitilde_{{1}}()0) + 5 GeV, a branching  ratio-independent limit on the gluino mass is given, see Fig. 16.


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KHACHATRYAN 2017AD searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing at least four jets (including b-jets), missing transverse momentum and tagged  top quarks. No evidence for an excess over the expected background is observed. Gluino masses up to  1550 GeV and neutralino masses up to 900 GeV are excluded at 95% C.L. See Fig. 13.


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KHACHATRYAN 2017AD searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing at least four jets (including b-jets), missing transverse momentum and tagged  top quarks. No evidence for an excess over the expected background is observed. Gluino masses up to  1450 GeV and neutralino masses up to 820 GeV are excluded at 95% C.L. See Fig. 13.


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KHACHATRYAN 2017AS searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with a single electron or muon and multiple jets. No significant excess above the Standard  Model expectations is observed. Limits are set on the gluino mass in the Tglu3A and Tglu1B  simplified models, see their Fig. 7.


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SIRUNYAN 2017AF searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with a single lepton  (electron or muon), jets, including at least one jet originating from  a b-quark, and large notET. No significant excess above the Standard Model expectations  is observed. Limits are set on the gluino mass in the Tglu3A and Tglu3B simplified models, see  their Figure 2.


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AABOUD 2016AC searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with hadronic jets, 1 or two hadronically decaying tau and notET. In Tglu1F,  gluino masses are excluded at 95% C.L. up to 1570 GeV for neutralino masses of 100 GeV or  below. Neutralino masses up to 700 GeV are excluded for all gluino masses between 800 GeV and 1500  GeV, while the strongest neutralino-mass exclusion of 750 GeV is achieved for gluino masses around  1400 GeV. See their Fig. 8. Limits are also presented in the context of Gauge-Mediated Symmetry  Breaking models: in this case, values of Lambda below 92 TeV are excluded at the 95% CL,  corresponding to gluino masses below 2000 GeV. See their Fig. 9.


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AABOUD 2016J searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with one isolated electron or muon, hadronic jets, and notET.  Gluino-mediated pair  production of stops with a nearly mass-degenerate stop and neutralino are targeted and gluino  masses are excluded at 95% C.L. up to 1460 GeV. A 100% of stops decaying via charm +  neutralino is assumed. The results are also valid in case of 4-body decays ttilde_1 --> f f^' b chitilde_1()0. See  their Fig. 8.


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AABOUD 2016M searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with two photons, hadronic jets and notET. No significant excess above the Standard Model  expectations is observed. Exclusion limits at 95% C.L. are set on gluino masses in the  general gauge-mediated SUSY breaking model (GGM), for bino-like NLSP. See their Fig.3.


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AABOUD 2016N searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing hadronic jets, large notET, and no electrons or muons. No significant excess above  the Standard Model expectations is observed. Gluino masses below 1510 GeV are excluded at the  95% C.L. in a simplified model with only gluinos and the lightest neutralino. See their Fig.  7b.


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AABOUD 2016N searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing hadronic jets, large notET, and no electrons or muons. No significant excess above  the Standard Model expectations is observed. Gluino masses below 1500 GeV are excluded at the  95% C.L. in a simplified model with gluinos decaying via an intermediate chitilde_1()+-  to two quarks, a W boson and a chitilde_1()0, for mass(chitilde_{{1}}()0) = 200 GeV. See their  Fig 8.


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AAD 2016AD searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  containing several energetic jets, of which at least three must be identified as b-jets, large  notET and no electrons or muons. No significant excess above the Standard Model expectations  is observed.  For chitilde_{{1}}()0 below 800 GeV, gluino masses below 1780 GeV are excluded at  95% C.L. for gluinos decaying via bottom squarks. See their Fig. 7a.


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AAD 2016AD searched in 3.2 fb^{-1} of pp collisions at sqrt(s) = 13 TeV for events  containing several energetic jets, of which at least three must be identified as b-jets, large  notET and one electron or muon. Large-radius jets with a high mass are also used to identify  highly boosted top quarks. No significant excess above the Standard Model expectations is observed.  For chitilde_{{1}}()0 below 700 GeV, gluino masses below 1760 GeV are excluded at 95% C.L.  for gluinos decaying via top squarks. See their Fig. 7b.


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AAD 2016BB searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with exactly two same-sign leptons or at least three leptons, multiple hadronic jets, b-jets,  and notET. No significant excess over the Standard Model expectation is found. Exclusion  limits at 95% C.L. are set on the gluino mass in various simplified models (Tglu1D, Tglu1E,  Tglu3A). See their Figs. 4.a, 4.b, and 4.d.


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AAD 2016BG searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in final  states with one isolated electron or muon, hadronic jets, and notET. The data agree with the  SM background expectation in the six signal selections defined in the search, and the largest  deviation is a 2.1 standard deviation excess. Gluinos are excluded at 95% C.L. up to 1600 GeV  assuming they decay via the lightest chargino to the lightest neutralino as in the model Tglu1B for  mass(chitilde_{{1}}()0)=100 GeV, assuming mass(chitilde_{{1}}()+-)=(mass(gtilde) +  mass(chitilde_{{1}}()0))/2. See their Fig.6.


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AAD 2016V searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with notET various hadronic jet multiplicities from >=7 to >=10 and with various  b-jet multiplicity requirements. No significant excess over the Standard Model expectation is  found. Exclusion limits at 95% C.L. are set on the gluino mass in one simplified model  (Tglu1E) and a pMSSM-inspired model. See their Fig. 5.


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KHACHATRYAN 2016AM searched in 19.7 fb^{-1}  of p p collisions at sqrt(s) = 8 TeV for  events with highly boosted W-bosons and b-jets, using the razor variables (M_{{R}} and  R^2) to discriminate between signal and background processes. No significant excess above the  Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu3C and Tglu3B  simplified models, see Fig. 12.


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KHACHATRYAN 2016BJ searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two isolated same-sign dileptons and jets in the final state. No significant excess  above the Standard Model expectations is observed.  Limits are set on the gluino mass in the  following simplified models: Tglu3A and Tglu3D, see Fig. 4, Tglu3B and Tglu3C, see Fig. 5, and  Tglu1B, see Fig. 7.


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KHACHATRYAN 2016BS searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least one energetic jet , no isolated leptons, and significant notET, using  the transverse mass variable M_{{T2}} to discriminate between signal and background processes. No  significant excess above the Standard Model expectations is observed. Limits are set on the gluino  mass in the Tglu1A, Tglu2A and Tglu3A simplified models, see Fig. 10 and Table 3.


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KHACHATRYAN 2016V searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events with at least four energetic jets and significant notET, no identified isolated electron or muon or charged track. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu1C, Tglu2A, and Tglu3A simplified  models, see Fig. 8.


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AAD 2015BG searched in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with jets, missing E(T), and two opposite-sign same flavor isolated leptons featuring  either a kinematic edge, or a peak at the  Z-boson mass, in the invariant mass spectrum. No  evidence for a statistically significant  excess over the expected SM backgrounds are observed and  95% C.L. exclusion limits are  derived in a GGM simplified model of gluino pair production  where the gluino decays into quarks, a  Z-boson, and a massless gravitino LSP, see Fig. 12.   Also, limits are set in simplified models  with slepton/sneutrino intermediate states, see Fig. 13.


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AAD 2015BV summarized and extended ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets in the sqrt(s) =8 TeV data set collected in 2012. The paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as new analyses. Exclusion limits at 95% C.L. are set on the gluino mass in several R-parity conserving models, leading to a generalized constraint on gluino masses exceeding 1150 GeV for lightest supersymmetric particle masses below 100 GeV. See their Figs. 10, 19, 20, 21,  23, 25, 26, 29-37.


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AAD 2015BX interpreted the results of a wide range of ATLAS direct searches for   supersymmetry, during the first run of the LHC using the sqrt(s) =7 TeV and sqrt(s) = 8 TeV data   set collected in 2012, within the wider framework of the phenomenological MSSM (pMSSM). The   integrated luminosity was up to 20.3 fb^{-1}. From an initial random sampling of 500 million   pMSSM points, generated from the 19-parameter pMSSM, a total of 310,327 model points with   chitilde_{{1}}()0 LSP were selected each of which satisfies constraints from previous collider   searches, precision measurements, cold dark matter energy density measurements and direct dark   matter searches. The impact of the ATLAS Run 1 searches on this space was presented, considering   the fraction of model points surviving, after projection into two-dimensional spaces of sparticle   masses. Good complementarity is observed between different ATLAS analyses, with almost all showing   regions of unique sensitivity. ATLAS searches have good sensitivity at LSP mass below 800 GeV.


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AAD 2015CA searched in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events  with  one or more photons, hadronic jets or b-jets and notET. No significant excess above  the  Standard Model expectations is observed.  Limits are set on gluino masses in the general   gauge-mediated SUSY breaking model (GGM), for bino-like or higgsino-bino admixtures NLSP, see Fig.   8, 10, 11


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KHACHATRYAN 2015AF searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with at least two energetic jets and significant notET, using the transverse mass   variable M_{{T2}} to discriminate between signal and background processes. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified   models where the decay gtilde --> q qbar chitilde_1()0 takes place with a branching ratio of    100%, see Fig. 13(a), or where the decay gtilde --> b bbar chitilde_1()0 takes  place with a branching ratio of 100%, see Fig. 13(b), or where the decay gtilde --> t tbar chitilde_1()0 takes place with a branching ratio of 100%, see Fig. 13(c). See also Table 5. Exclusions in  the CMSSM, assuming tan(beta) = 30, A(0) =   -2 max(mass(0), mass(1/2)) and mu > 0, are also presented, see  Fig. 15.


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KHACHATRYAN 2015I searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events  in which b-jets and four W-bosons are produced. Five individual search channels  are  combined (fully hadronic, single lepton, same-sign dilepton, opposite-sign dilepton,  multilepton).  No significant excess above the Standard Model expectations is observed. Limits are  set on the  gluino mass in a simplified model where the decay gtilde --> t tbar chitilde_1()0  takes place  with a branching ratio of 100%, see Fig. 5. Also a simplified model with gluinos  decaying  into on-shell top squarks is considered, see Fig. 6.


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KHACHATRYAN 2015X searched in 19.3fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with at least two energetic jets, at least one of which is required to originate from a  b quark, and significant notET, using the razor variables (M(R)) and  R**2) to discriminate between signal and background processes. No significant excess  above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified  models where the decay gtilde --> b bbar chitilde_1()0 and the decay gtilde --> t tbar chitilde_1()0  take place with branching ratios varying between 0, 50 and 100%, see Figs. 13 and 14.


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AAD 2014AE searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for strongly produced supersymmetric particles in events containing jets and large missing transverse momentum, and no electrons or muons. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing gluinos and squarks, see Figures 5, 6 and 7. Limits are also derived in the mSUGRA/CMSSM with parameters tan(beta) = 30, A_{{0}}() = -2 mass(0) and mu > 0, see their Fig. 8.


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AAD 2014AG searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing one hadronically decaying tau-lepton, zero or one additional light leptons (electrons or muons), jets and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95% C.L. are set in several SUSY scenarios. For an interpretation in the minimal GMSB model, see their Fig. 8. For an interpretation in the mSUGRA/CMSSM with parameters tan(beta) = 30, A_{{0}}() = -2 mass(0) and mu > 0, see their Fig. 9. For an interpretation in the framework of natural Gauge Mediation, see Fig. 10. For an interpretation in the bRPV scenario, see their Fig. 11.


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AAD 2014X searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least four leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in a general gauge-mediation model (GGM) where the decay gtilde --> q qbar chitilde_1()0, with chitilde_1()0 --> lepton+- lepton-+ Gtilde, takes place with a branching ratio of 100%, for two choices of tan(beta) = 1.5 and 30, see Fig. 11. Also some constraints on the higgsino mass parameter mu are discussed.


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CHATRCHYAN 2014AH searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for  events with at least two energetic jets and significant notET, using the razor variables  (M_{{R}}() and R^2()) to discriminate between signal and background processes. No significant  excess above the Standard Model expectations is observed. Limits are set on sbottom masses in  simplified models where the decay gtilde --> q qbar chitilde_1()0 takes place with a branching  ratio of 100%, see Fig. 28. Exclusions in the CMSSM, assuming tan(beta) = 10,  A_{{0}}() = 0 and mu > 0, are also presented, see Fig. 26.


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CHATRCHYAN 2014AH searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with at least two energetic jets and significant notET, using the razor variables (M_{{R}}() and R^2()) to discriminate between signal and background processes. A second analysis requires at least one of the jets to be originating from a b-quark. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay gtilde --> b bbar chitilde_1()0 takes place with a branching ratio of 100%, see Figs. 28 and 29. Exclusions in the CMSSM, assuming tan(beta) = 10, A_{{0}}() = 0 and mu > 0, are also presented, see Fig. 26.


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CHATRCHYAN 2014AH searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with at least two energetic jets and significant notET, using the razor variables (M_{{R}}() and R^2()) to discriminate between signal and background processes. A second analysis requires at least one of the jets to be originating from a b-quark. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay gtilde --> t tbar chitilde_1()0 takes place with a branching ratio of 100%, see Figs. 28 and 29. Exclusions in the CMSSM, assuming tan(beta) = 10, A_{{0}}() = 0 and mu >0, are also presented, see Fig. 26.


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CHATRCHYAN 2014I searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing multijets and large notET. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing gluinos that decay via gtilde --> q qbar chitilde_1()0 with a 100% branching ratio, see Fig. 7b, or via gtilde --> t tbar chitilde_1()0 with a 100% branching ratio, see Fig. 7c, or via gtilde --> q qbar W / Z chitilde_1()0, see Fig. 7d.


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CHATRCHYAN 2014N searched in 19.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events containing a single isolated electron or muon and multiple jets, at least two of which are identified as originating from a b-quark. No significant excesses over the expected SM backgrounds are observed. The results are interpreted in three simplified models of gluino pair production with subsequent decay into virtual or on-shell top squarks, where each of the top squarks decays in turn into a top quark and a chitilde_{{1}}()0, see Fig. 4. The models differ in which masses are allowed to vary.


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CHATRCHYAN 2014R searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least three leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in a slepton co-NLSP simplified model (GMSB) where the decay gtilde --> q lepton+- lepton-+ Gtilde takes place with a branching ratio of 100%, see Fig. 8.


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CHATRCHYAN 2014R searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least three leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in a simplified model where the decay gtilde --> t tbar chitilde_1()0 takes place with a branching ratio of 100%, see Fig. 11.


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AABOUD 2018BJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in  events with two opposite-sign charged leptons (electrons and muons), jets and missing transverse  momentum, with various requirements to be sensitive to signals with different kinematic endpoint  values in the dilepton invariant mass distribution. The data are found to be consistent with the SM  expectation. Results are interpreted in the Tglu1H model in case of mass(chitilde_{{1}}()0) = 1 GeV:  for any mass(chitilde_{{2}}()0), gluino masses below 1500 GeV are excluded, see their Fig. 14(a).


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AABOUD 2018V searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV in events  with no charged leptons, jets and missing transverse momentum. The data are found to be consistent  with the SM expectation. Results are interpreted in a Tglu1C-like model, assuming 50% BR for  each gluino decay mode. Gluino masses below 1770 GeV are excluded for any mass(chitilde_{{2}}()0)  - mass(chitilde_{{1}}()0) and mass(chitilde_{{1}}()0) = 60 GeV, see their Fig. 16(b).


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AABOUD 2017AZ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least seven jets and large missing transverse momentum. Selected events are further  classified based on the presence of large R-jets or b-jets and no leptons. No significant  excess above the Standard Model expectations is observed. Limits are set for pMSSM models with  M_{{1}} = 60 GeV, tan(beta) = 10, mu < 0 varying the soft-breaking parameters M_{{3}}  and mu. Gluino masses up to 1600 GeV are excluded for mass(chitilde_{{1}}()+-) = 200 GeV. See  their Figure 6a and text for details on the model.


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KHACHATRYAN 2016AY searched in 2.3 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one isolated high transverse momentum lepton (e or mu), hadronic jets of which  at least one is identified as coming from a b-quark, and large notET.  No significant  excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the  Tglu3A simplified model, see Fig. 10, and in the Tglu3B model, see Fig. 11.


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AAD 2015AB searched for the decay of neutral, weakly interacting, long-lived particles in  20.3 fb^{-1} of pp collisions at sqrt(s) = 8 TeV.  Signal events require at least two  reconstructed vertices possibly originating from long-lived particles decaying to jets in the inner  tracking detector and muon spectrometer. No significant excess of events over the expected  background was found. Results were interpreted in Stealth SUSY benchmark models where a pair of  gluinos decay to long-lived singlinos, Stilde, which in turn each decay to a low-mass gravitino and a pair  of jets. The 95% confidence-level limits are set on the cross section x  branching  ratio for the decay gtilde --> Stilde g, as a function of the singlino proper lifetime  (ctau). See their Fig. 10(f)


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AAD 2015AI searched in 20 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events  containing at least one isolated lepton (electron or muon), jets, and large missing transverse  momentum. No excess of events above the expected level of Standard Model background was found.  Exclusion limits at 95% C.L. are set on the gluino mass in the CMSSM/mSUGRA, see Fig. 15, in  the NUHMG, see Fig. 16, and in various simplified models, see Figs. 18 -- 22.


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AAD 2015CB searched for events containing at least one long-lived particle that decays at a  significant distance from its production point (displaced vertex, DV) into two leptons or into five  or  more charged particles in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV. The  dilepton signature is  characterised by DV formed from at least two lepton candidates. Four  different final states  were considered for the multitrak signature, in which the DV must be  accompanied by a high-transverse  momentum muon or electron candidate that originates from the DV,  jets or missing transverse momentum.  No events were observed in any of the signal regions. Results  were interpreted in SUSY scenarios involving  R-parity violation, split supersymmetry, and  gauge mediation. See their Fig. 12 -- 20.


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KHACHATRYAN 2015AD searched in 19.4 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for events with two opposite-sign same flavor isolated leptons featuring either a kinematic edge, or a peak at the Z-boson mass, in the invariant mass spectrum. No evidence for a statistically significant excess over the expected SM backgrounds is observed and 95% C.L. exclusion limits   are derived in a simplified model of gluino pair production where the gluino decays into quarks, a Z-boson, and a massless gravitino LSP, see Fig. 9.


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KHACHATRYAN 2015AZ searched in 19.7 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events with either at least one photon, hadronic jets and notET (single photon channel) or  with at least two photons and at least one jet and using the razor variables. No significant excess  above the Standard Model expectations is observed.  Limits are set on gluino masses in the general  gauge-mediated SUSY breaking model (GGM), for both a bino-like and wino-like neutralino NLSP  scenario, see Fig. 8 and 9.


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AAD 2014AX searched in 20.1 fb**-1 of p p collisions at sqrt(s) = 8 TeV for the strong production of supersymmetric particles in events containing either zero or at last one high high-pT lepton, large missing transverse momentum, high jet multiplicity and at least three jets identified as originating from b-quarks. No excess over the expected SM background is observed. Limits are derived in mSUGRA/CMSSM models  with tan(beta) = 30, A_{{0}}() = -2m_{{0}}() and mu > 0, see their Fig. 14. Also, exclusion limits in simplified models containing gluinos and scalar top and bottom quarks are set, see their Figures 12, 13.


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AAD 2014E searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for strongly produced supersymmetric particles in events containing jets and two same-sign leptons or three leptons. The search also utilises jets originating from b-quarks, missing transverse momentum and other variables. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing gluinos and squarks, see Figures 5 and 6. In the gtilde --> q q^' chitilde_1()+-, chitilde_1()+- --> W^(*)()+- chitilde_2()0, chitilde_2()0 --> Z^(*)() chitilde_1()0 simplified model, the following assumptions have been made: mass(chitilde_{{1}}()+-) = 0.5 mass(chitilde_{{1}}()0) + mass(gtilde), mass(chitilde_{{2}}()0) = 0.5 (mass(chitilde_{{1}}()0) + mass(chitilde_{{1}}()+-)), mass(chitilde_{{1}}()0) < 520 GeV. In the gtilde --> q q^' chitilde_1()+-, chitilde_1()+- --> lepton+- nu chitilde_1()0 or gtilde --> q q^' chitilde_2()0, chitilde_2()0 --> lepton+- lepton-+ ( nu nu ) chitilde_1()0 simplified model, the following assumptions have been made: mass(chitilde_{{1}}()+-) = mass(chitilde_{{2}}()0) = 0.5 (mass(chitilde_{{1}}()0) + mass(gtilde)), mass(chitilde_{{1}}()0) < 660 GeV. Limits are also derived in the mSUGRA/CMSSM, bRPV and GMSB models, see their Fig. 8.


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CHATRCHYAN 2014H searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified models where the decay gtilde --> t tbar chitilde_1()0 takes place with a branching ratio of 100%, or where the decay gtilde --> ttilde t, ttilde --> t chitilde_1()0 takes place with a branching ratio of 100%, with varying mass of the chitilde_{{1}}()0, or where the decay gtilde --> btilde b, btilde --> t chitilde_1()+-, chitilde_1()+- --> W+- chitilde_1()0 takes place with a branching ratio of 100%, with varying mass of the chitilde_{{1}}()+-, see Fig. 5.


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CHATRCHYAN 2014H searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified models where the decay gtilde --> q q^' chitilde_1()+-, chitilde_1()+- --> W+- chitilde_1()0 takes place with a branching ratio of 100%, with varying mass of the chitilde_{{1}}()+- and chitilde_{{1}}()0, see Fig. 7.


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CHATRCHYAN 2014H searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified models where the decay gtilde --> b tbar chitilde_1()+-, chitilde_1()+- --> W+- chitilde_1()0 takes place with a branching ratio of 100%, for two choices of mass(chitilde_{{1}}()+-) and fixed mass(chitilde_{{1}}()0), see Fig. 6.


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AAD 2024AF searched in 140 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for evidence  of gluino pair production followed by direct RPV gluino decays into three jets or gtilde --> q q chitilde_1()0  followed by the decay of chitilde_{{1}}()0 into three jets. No excess above the Standard Model  prediction is observed, and the results are interpreted in models with non-vanishing  lambda(112)**'' or lambda(113)**'', Tglu1RPV and Tglu1A with  chitilde_{{1}}()0 RPV decay, see their Figures 9 and 10.


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AAD 2020AL searched in 139 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for events  with 8 or more jets and moderate missing transverse momentum. The selection makes requirements  according to the number of b-tagged jets and the scalar sum of masses of large-radius jets. No  significant excess above the Standard Model expectations is observed. Exclusion limits at 95%  C.L. are set on the gluino mass in RPV simplified models where the gluino decays via gtilde --> t b d or  gtilde --> t b s. They extend up to almost 1.6 TeV for a ttilde_{{1}} mass of 900 GeV. See  their Fig. 10(c).


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AAD 2020V searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for events  with two same-sign charged leptons (electrons or muons) and jets. No significant excess above the  Standard Model expectations is observed. Exclusion limits at 95% C.L. are set on the gluino  mass in RPV simplified models where the gluino decays via gtilde --> t b d, see Figure 7(b).


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SIRUNYAN 2019F searched in 35.9 fb**-1 of p p collisions at sqrt(s) = 13 TeV for  three-jet resonances produced in the decay of a gluino in R-parity violating supersymmetric models.  The mass range from 200 to 2000GeV is explored in four separate mass regions. The observations show  agreement with standard model expectations. The results are interpreted within the framework of  R-parity violating SUSY, where pair-produced gluinos decay to a six quark final state. Gluino  masses below 1500GeV are excluded at 95% C.L. See their Fig.5.


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SIRUNYAN 2018AK searched in 35.9 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events containing a single lepton, large jet and b-quark jet multiplicities, coming from  R-parity-violating decays of gluinos. No excess over the expected background is observed. Limits  are derived on the gluino mass, assuming the RPV gtilde --> t b s decay, see their Figure 9.


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AABOUD 2017AI searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more isolated lepton, at least eight jets, either zero or many b-jets, for  evidence of R-parity violating decays of the gluino. No significant excess above the Standard  Model expectations is observed. Limits up to 2.1 TeV are set on the gluino mass in  R-parity-violating supersymmetry models as Tglu3A with LSP decay through the non-zero  lambda_{{112}}^'' coupling as chitilde_1()0 --> u d s. See their Figure 9.


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AABOUD 2017AI searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more isolated lepton, at least eight jets, either zero or many b-jets, for  evidence of R-parity violating decays of the gluino. No significant excess above the Standard  Model expectations is observed. Limits up to 1.65 TeV are set on the gluino mass in  R-parity-violating supersymmetry models with gtilde --> t ttilde, ttilde --> b s  through the non-zero lambda_{{323}}^'' coupling. See their Figure 9.


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AABOUD 2017AI searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with one or more isolated lepton, at least eight jets, either zero or many b-jets, for  evidence of R-parity violating decays of the gluino. No significant excess above the Standard  Model expectations is observed. Limits up to 1.8 TeV are set on the gluino mass in  R-parity-violating supersymmetry models as Tglu1A with the LSP decay through the non-zero  lambda^' coupling as chitilde_1()0 --> q q lepton. See their Figure 9.


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.8 TeV are set  on the gluino mass in R-parity-violating supersymmetry models as Tglu3A with LSP decaying  through the non-zero lambda_{{112}}^'' coupling as chitilde_1()0 --> u d s. See their Figure  5(d).


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.75 TeV are set  on the gluino mass in R-parity-violating supersymmetry models as Tglu1A with LSP decaying  through the non-zero lambda^' coupling as chitilde_1()0 --> q q lepton. See their Figure  5(c).


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.45 TeV are set  on the gluino mass in R-parity-violating supersymmetry models where gtilde --> t ttilde_1  and ttilde_1 --> s d through the non-zero lambda_{{321}}^'' coupling. See their Figure 5(b).


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 1.45 TeV are set  on the gluino mass in R-parity-violating supersymmetry models where gtilde --> t ttilde_1  and ttilde_1 --> b d through the non-zero lambda_{{313}}^'' coupling. See their Figure 5(a).


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AABOUD 2017AJ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with two same-sign or three leptons, jets and large missing transverse momentum. No  significant excess above the Standard Model expectations is observed. Limits up to 400 GeV are set  on the down type squark (dtilde_R mass in R-parity-violating supersymmetry models where  dtilde_R --> t b through the non-zero lambda_{{313}}^'' coupling or dtilde_R --> t s  through the non-zero lambda_{{321}}^''. See their Figure 5(e) and 5(f).


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AABOUD 2017AZ searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with at least seven jets and large missing transverse momentum. Selected events are further  classified based on the presence of large R-jets or b-jets and no leptons. No significant  excess above the Standard Model expectations is observed. Limits are set for R-parity violating  decays of the gluino assuming gtilde --> t ttilde_1 and ttilde_1 --> b s through the  non-zero lambda_{{323}}^'' couplings. The range 625 -- 1375 GeV is excluded for  mass(ttilde_{{1}}) = 400 GeV. See their Figure 7b.


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KHACHATRYAN 2017Y searched in 19.7 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing at least 8 or 10 jets, possibly b-tagged, coming from R-parity-violating  decays of supersymmetric particles. No excess over the expected background is observed. Limits are  derived on the gluino mass, assuming various RPV decay modes, see Fig. 7.


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KHACHATRYAN 2016BX searched in 19.5 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  events containing 0 or 1 leptons and b-tagged jets, coming from R-parity-violating decays of  supersymmetric particles. No excess over the expected background is observed. Limits are derived on  the gluino mass, assuming the RPV gtilde --> t b s decay, see Fig. 7 and 10.


pdgid: S046GNV
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AAD 2014X searched in 20.3 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with at least four leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in an R-parity violating simplified model where the decay gtilde --> q qbar chitilde_1()0, with chitilde_1()0 --> lepton+- lepton-+ nu, takes place with a branching ratio of 100%, see Fig. 8.


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CHATRCHYAN 2014P searched in 19.4 fb**-1 of p p collisions at sqrt(s) = 8 TeV for three-jet resonances produced in the decay of a gluino in R-parity violating supersymmetric models. No excess over the expected SM background is observed. Assuming a 100% branching ratio for the gluino decay into three light-flavour jets, limits are set on the cross section of gluino pair production, see Fig. 7, and gluino masses below 650 GeV are excluded at 95% C.L. Assuming a 100% branching ratio for the gluino decaying to one b-quark jet and two light-flavour jets, gluino masses between 200 GeV and 835 GeV are excluded at 95% C L.


pdgid: S046GNV
text:
AABOUD 2018CF searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events with several jets, possibly b-jets, and large-radius jets for evidence of R-parity  violating decays of the gluino. No significant excess above the Standard Model expectations is  observed. Limits between 1000 and 1875 GeV are set on the gluino mass in R-parity-violating  supersymmetry models as Tglu2RPV with the LSP decay through the non-zero lambda^'' coupling as  chitilde_1()0 --> q q q. The most stringent limit is obtained for mass(chitilde_{{1}}()0) = 1000  GeV, the weakest for mass(chitilde_{{1}}()0) = 50 GeV. See their Figure 7(b). Figure 7(a) presents  results for gluinos directly decaying into 3 quarks, Tglu1RPV.


pdgid: S046GNV
text:
AAD 2015X searched in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV  for events  containing large number of jets, no requirements on missing transverse momentum and no isolated  electrons or muons.  The sensitivity of the search is enhanced by considering the number of  b-tagged jets and the scalar sum of masses of large-radius jets in an event. No evidence was  found for excesses above the expected level of Standard Model background. Exclusion limits at 95% C.L. are set on the gluino mass assuming the gluino decays to various quark flavors, and for  various neutralino masses. See their Fig. 11 -- 16.


pdgid: S046GNV
text:
CHATRCHYAN 2014H searched in 19.5 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified models where the R-parity violating decay gtilde --> t b s takes place with a branching ratio of 100%, see Fig. 8.


pdgid: S046LGN
text:
AAD 2023G searched in 139 fb**-1 of p p collisions at sqrt(s) = 13 TeV for R-hadron  pair   production in events with high-pt tracks with large ionisation in the pixel detector. No    significant excess above the Standard Model predictions is observed. Limits are set on the R-hadron    mass for different masses of the LSP and for different R-hadron lifetimes, see  Figure 18.


pdgid: S046LGN
text:
SIRUNYAN 2021AF searched in 140 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  supersymmetry in events with with two displaced vertices from long-lived particles decaying into  multijet or dijet final states. No significant excess above the Standard Model expectations is  observed. Limits are set on the gluino mass in the simplified model Tglu2RPV with lambda_{{323}}^''  coupling, on the chitilde_{{1}}()0 mass in an RPV model with chitilde_{{1}}()0 pair production and  the RPV decay chitilde_1()0 --> tbs with lambda_{{323}}^'' coupling and on the ttilde mass  in an RPV model with top squark pair production and the RPV decay ttilde --> dbar_i dbar_j with  lambda_{{3ij}}^'' coupling, see their Figure 7.


pdgid: S046LGN
text:
SIRUNYAN 2021U searched in 132 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for   supersymmetry in events with displaced tracks and displaced vertices associated with a dijet   system. No significant excess above the Standard Model expectations is observed. Limits are set on   long-lived gluinos in an RPC GMSB SUSY model of gluino pair production, with gtilde --> g Gtilde, see   their Figure 9, in Tglu1A in a mini-split model, see their Figure 10, and in an RPV model of gluino   pair production, with gtilde --> t b s with coupling lambda_{{323}}^'', see their Figure 11.   Limits are also set on long-lived top squarks in Tstop2RPV, see their Figure 12, in an RPV model   with ttilde --> d leptonbar and lambda_{{x31}}^' coupling, see their Figure 13, and in a   dynamical RPV model with ttilde --> dbar dbar via a nonholomorphic RPV coupling eta_{{311}}^'',   see their Figure 14. The best mass limit is achieved in all cases at ctau = 30 mm.


pdgid: S046LGN
text:
AABOUD 2019AT searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  metastable and stable R-hadrons. Multiple search strategies for a wide range of lifetimes,  corresponding to path lengths of a few meters, are defined. No significant deviations from the  expected Standard Model background are observed. Gluino R-hadrons with lifetimes of the order  of 50 ns are excluded at 95% C.L. for masses below 1980 GeV using the muon-spectrometer  agnostic analysis.  Using the full-detector search, the observed lower limits on the mass are 2000  GeV. See their Figure 9 (top).


pdgid: S046LGN
text:
AABOUD 2019C searched in 36.1 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  metastable and stable R-hadrons arising as excesses in the mass distribution of reconstructed  tracks with high transverse momentum and large dE/dx. Gluino R-hadrons with lifetimes above 10  ns are excluded at 95% C.L. with lower mass limit range between 1000 GeV and 2060 GeV, see  their Figure 5(a). Masses smaller than 1290 GeV are excluded for a lifetime of 1 ns, see their  Figure 6. In the case of stable R-hadrons, the lower mass limit is 1890 GeV, see their Figure  5(b).


pdgid: S046LGN
text:
SIRUNYAN 2019BT searched in 137 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived particles decaying to displaced, nonprompt jets and missing transverse momentum.   Candidate signal events are identified using the timing capabilities of the CMS electromagnetic  calorimeter. The results of the search are found to be consistent with the background predictions.  Limits are set on the gluino mass in a GMSB model where long-lived gluinos are pair produced and  decaying via  gtilde --> g Gtilde, see their Figures 4 and 5.


pdgid: S046LGN
text:
AABOUD 2018S searched in 32.8 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for long-lived gluinos in final states with large missing transverse momentum and at least one  high-mass displaced vertex with five or more tracks. The observed yield is consistent with the  expected background. Exclusion limits are derived for Tglu1A models predicting the existence of  long-lived gluinos reaching roughly m(gtilde) = 2000 GeV to 2370 GeV for m(chitilde_{{1}}()0) =  100 GeV and  gluino lifetimes between 0.02 and 10 ns, see their Fig. 8. Limits are presented also  as a function of the lifetime (for a fixed gluino-neutralino mass difference of 100 GeV) and of the  gluino and neutralino masses (for a fixed lifetime of 1 ns). See their Fig. 9 and 10 respectively.


pdgid: S046LGN
text:
KHACHATRYAN 2017AR searched in 17.6 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  R-parity-violating SUSY in which long-lived neutralinos or gluinos decay into multijet final  states.  No significant excess above the Standard Model expectations is observed. Limits are set on  the gluino mass for a range of mean proper decay lengths (ctau), see their Fig. 7. The upper limits on the production cross section times branching ratio squared (Fig. 7) are also  applicable to long-lived neutralinos.


pdgid: S046LGN
text:
AABOUD 2016B searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived R-hadrons using observables related to large ionization losses and slow propagation  velocities, which are signatures of heavy charged particles traveling significantly slower than the  speed of light. Exclusion limits at 95% C.L. are set on the long-lived gluino masses  exceeding 1580 GeV. See their Fig. 5.


pdgid: S046LGN
text:
AABOUD 2016C searched in 3.2 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  long-lived and stable R-hadrons identified by anomalous specific ionization energy loss in the  ATLAS Pixel detector. Gluino R-hadrons with lifetimes above 0.4 ns are excluded at 95%  C.L. with lower mass limit range between 740 GeV and 1590 GeV. In the case of stable R-hadrons,  the lower mass limit is 1570 GeV. See their Figs. 5 and 6.


pdgid: S046LGN
text:
KHACHATRYAN 2016BW searched in 2.5 fb^{-1} of p p collisions at sqrt(s) = 13 TeV for  events  with heavy stable charged particles, identified by their anomalously high energy deposits  in the silicon tracker and/or long time-of-flight measurements by the muon system. No evidence for  an excess over the expected background is observed. Limits are derived for pair production of  gluinos as a function of mass, depending on the interaction model and on the fraction f, of  produced gluinos hadronizing into a gtilde - gluon state, see Fig. 4 and Table 7.


pdgid: S046LGN
text:
AAD 2015AE searched in 19.1 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for heavy  long-lived charged particles, measured through their specific ionization energy loss in the ATLAS  pixel detector or their time-of-flight in the ALTAS muon system. In the absence of an excess of  events above the expected backgrounds, limits are set R-hadrons in various scenarios, see Fig. 11.  Limits are also set in LeptoSUSY models where the gluino decays to stable 300 GeV leptons, see Fig. 9.


pdgid: S046LGN
text:
AAD 2015BM searched in 18.4 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for stable  and metastable non-relativistic charged particles through their anomalous specific ionization  energy loss in the ATLAS pixel detector. In absence of an excess of events above the expected  backgrounds, limits are set within a generic R-hadron model, on stable gluino R-hadrons (see Table 5) and on metastable gluino  R-hadrons decaying to (g / q qbar) plus a light chitilde_{{1}}^0() (see Fig. 7) and  decaying to t tbar plus a light chitilde_{{1}}()0 (see Fig. 9).


pdgid: S046LGN
text:
KHACHATRYAN 2015AK looked in a data set corresponding to 18.6 fb**-1 of p p  collisions at sqrt(s) = 8 TeV, and a search interval corresponding to 281 h of trigger lifetime,  for long-lived particles that have stopped in the CMS detector. No evidence for an excess over the  expected background in a cloud interaction model is observed. Assuming the decay gtilde --> g chitilde_1()0 and  lifetimes between 1 mus and 1000 s, limits are derived on gtilde production as a function  of mass(chitilde_{{1}}()0), see Figs. 4 and 6. The exclusions require that mass(chitilde_{{1}}()0) is  kinematically consistent with the minimum values of the jet energy thresholds used.


pdgid: S046LGN
text:
AAD 2013AA searched in 4.7 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events containing colored long-lived particles that hadronize forming R-hadrons. No significant excess above the expected background was found. Long-lived R-hadrons containing a gtilde are excluded for masses up to 985 GeV at 95% C.L in a general interaction model.  Also, limits independent of the fraction of R-hadrons that arrive charged in the muon system were derived, see Fig. 6.


pdgid: S046LGN
text:
AAD 2013BC searched in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV and in 22.9 fb**-1 of p p collisions at sqrt(s) = 8 TeV for bottom squark R-hadrons that have come to rest within the ATLAS calorimeter and decay at some later time to hadronic jets and a neutralino. In absence of an excess of events above the expected backgrounds, limits are set on gluino masses for different decays, lifetimes, and neutralino masses, see their Table 6 and Fig. 10.


pdgid: S046LGN
text:
CHATRCHYAN 2013AB looked in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV and in 18.8 fb**-1 of p p collisions at sqrt(s) = 8 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or additionally requiring that it be identified as muon in the muon chambers, from pair production of gtilde's. No evidence for an excess over the expected background is observed. Limits are derived for pair production of gluinos as a function of mass (see Fig. 8 and Table 5), depending on the fraction, f, of formation of gtilde-g (R-gluonball) states. The quoted limit is for f = 0.1, while for f = 0.5 it degrades to 1276 GeV. In the conservative scenario where every hadronic interaction causes it to become neutral, the limit decreases to 928 GeV for f = 0.1.


pdgid: S046LGN
text:
AAD 2012P looked in 31 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with pair production of long-lived gluinos. The hadronization of the gluinos leads to R-hadrons which may stop inside the detector and later decay via gtilde --> g chitilde_1()0 during gaps between the proton bunches. No significant excess over the expected background is observed. From a counting experiment, a limit at 95% C.L. on the cross section as a function of mass(gtilde) is derived for mass(chitilde_{{1}}()0) = 100 GeV, see Fig. 4. The limit is valid for lifetimes between E-5 and E3 seconds and assumes the Generic matter interaction model for the production cross section.


pdgid: S046LGN
text:
CHATRCHYAN 2012AN looked in 4.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with pair production of long-lived gluinos. The hadronization of the gluinos leads to R-hadrons which may stop inside the detector and later decay via gtilde --> g chitilde_1()0 during gaps between the proton bunches. No significant excess over the expected background is observed. From a counting experiment, a limit at 95% C.L. on the cross section as a function of mass(gtilde) is derived, see Fig. 3. The mass  limit is valid for lifetimes between E-5 and E3 seconds, for what they call ''the daughter gluon energy E_{{g}}() >'' 100 GeV and assuming the cloud interaction model for R-hadrons. Supersedes KHACHATRYAN 2011.


pdgid: S046LGN
text:
CHATRCHYAN 2012L looked in 5.0 fb**-1 of p p collisions at sqrt(s) = 7 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or additionally requiring that it be identified as muon in the muon chambers, from pair production of gtilde's. No evidence for an excess over the expected background is observed. Limits are derived for pair production of gluinos as a function of mass (see Fig. 3), depending on the fraction, f, of formation of gtilde-g (R-glueball) states. The quoted limit is for f = 0.1, while for f = 0.5 it degrades to 1046 GeV. In the conservative scenario where every hadronic interaction causes it to become neutral, the limit decreases to 928 GeV for f=0.1. Supersedes KHACHATRYAN 2011C.


pdgid: S046LGN
text:
AAD 2011K looked in 34 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with heavy stable particles,  identified by their anomalous dE/dx in the tracker or time of flight in the tile calorimeter, from pair production  of gtilde. No evidence for an excess over the SM expectation is observed. Limits are derived for pair production of gluinos as a function of mass (see Fig. 4), for a fraction, f = 10%, of formation of gtilde-g (R-gluonball). If instead of a phase space driven approach for the hadronic scattering of the R-hadrons, a triple-Regge  model or a bag-model is used, the limit degrades to 566 and 562 GeV, respectively.


pdgid: S046LGN
text:
AAD 2011P looked in 37 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with heavy stable particles,  reconstructed and identified by their time of flight in the Muon System. There is no requirement on their observation  in the tracker to increase the sensitivity to cases where gluinos have a large fraction, f, of formation of neutral  gtilde-g (R-gluonball). No evidence for an excess over the SM expectation is observed. Limits are derived  as a function of mass (see Fig. 4), for f=0.1.  For fractions f = 0.5 and 1.0 the limit degrades to 537 and 530 GeV, respectively.


pdgid: S046LGN
text:
KHACHATRYAN 2011 looked in 10 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with pair production of long-lived gluinos. The hadronization of the gluinos leads to R-hadrons which may stop inside the detector and later decay via gtilde --> g chitilde_1^0() during gaps between the proton bunches. No significant excess over the expected background is observed. From a counting experiment, a limit at 95% C.L. on the cross section times branching ratio is derived for mass(gtilde)-mass(chitilde_{{1}}^0())> 100 GeV, see their Fig. 2. Assuming 100% branching ratio, lifetimes between 75 ns and 3E5 s are excluded for mass(gtilde) = 300 GeV. The gtilde mass exclusion is obtained with the same assumptions for lifetimes between  10 mu s and 1000 s, but shows some dependence on the model for R-hadron interactions with matter, illustrated in Fig. 3. From a time-profile analysis, the mass exclusion is 382 GeV  for a lifetime of 10 mu s under the same assumptions as above.


pdgid: S046LGN
text:
KHACHATRYAN 2011C looked in 3.1 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or additionally requiring that it be identified as muon in the muon chambers, from pair production of gtilde. No evidence for an excess over the expected background is observed. Limits are derived for pair production of gluinos as a function of mass (see Fig. 3), depending on the fraction, f, of formation of gtilde-g (R-gluonball). The quoted limit is for f=0.1, while for f=0.5 it degrades to 357 GeV. In the conservative scenario where every hadronic interaction causes it to become neutral, the limit decreases to 311 GeV for f=0.1.


pdgid: S046GTN
text:
AAD 2015BH searched in 20.3 fb^{-1} of p p collisions at sqrt(s) = 8 TeV for  associated production of a light gravitino and a squark or gluino. The squark (gluino) is assumed  to decay exclusively to a quark (gluon) and a gravitino. No evidence was found for an excess above  the expected level of Standard Model background and 95% C.L. lower limits were set on the  gravitino mass as a function of the squark/gluino mass, both in the case of degenerate and  non-degenerate squark/gluino masses, see Figs. 14 and 15.


pdgid: S046GTN
text:
ABDALLAH 2005B use data from sqrt(s) = 180 -- 208~GeV.  They look for events with a single photon + notE final states from which a cross section limit of sigma < 0.18~pb at 208~GeV is obtained, allowing a limit on the mass to be set. Supersedes the results of ABREU 2000Z.


pdgid: S046GTN
text:
ACHARD 2004E use data from sqrt(s) = 189 -- 209~GeV. They look for events with a single photon + notE final states from which a limit on the Gravitino mass is set corresponding to sqrt(F) > 238~GeV. Supersedes the results of ACCIARRI 1999R.


pdgid: S046GTN
text:
ACOSTA 2002H looked in 87 pb**-1 of p pbar collisions at sqrt(s)=1.8 TeV for events with a high-E(T) photon and notET. They compared the data with a GMSB model where the final state could arise from q qbar --> Gtilde Gtilde gamma. Since the cross section for this process scales as 1/|F |**4, a limit at 95% CL is derived on |F |**1/2 > 221 GeV. A model independent limit for the above topology is also given in the paper.


pdgid: S046OTH
text:
AAD 2024AH combined a number of ATLAS analyses to use them and interpret in a series of  models derived from a flat-prior scan to pMSSM parameter space. Limits are provided in terms of  fraction of models excluded as a function of one or two parameters, while marginalising over the  others.


pdgid: S046OTH
text:
AAD 2020C uses a statistical combination of six final states b bbar b bbar, b bbar W W, b bbar tau tau, W W W W, b bbar gamma gamma,  and W W gamma gamma to search for non-resonant and resonant production of Higgs boson pairs.  The search uses 36.1 fb^{-1} of p p collisions data at sqrt(s) = 13 TeV. Constraints in the  habemus Minimal Supersymmetric Standard Model in the (mass(A), tanbeta) parameter space are  placed, see their Figure 7(b).


pdgid: S046OTH
text:
AAD 2020L used 27.8 fb^{-1} of p p collision data at sqrt(s) = 13 TeV to search for  heavy neutral Higgs bosons produced in association with at least one b-quark and decaying into  a pair of b-quarks. The data are compatible with SM expectations, yielding no significant  excess of events in the mass range 450 -- 1400 GeV, see their Fig. 11. Exclusion limits at  95% C.L. were derived in hMSSM scenarios as a function of mass(A) and tanbeta, see their  Fig. 9 and 10.


pdgid: S046OTH
text:
AABOUD 2016AF uses a selection of searches by ATLAS for the electroweak production of SUSY  particles studying resulting constraints on dark matter candidates. They use 20 fb**-1 of p p  collisions at sqrt(s) = 8 TeV. A likelihood-driven scan of an effective model focusing on the  gaugino-higgsino and Higgs sector of the pMSSM is performed. The ATLAS searches impact models where  mass(chi_{{1}}()0) < 65 GeV, excluding 86% of them. See their Figs. 2, 4, and 6.


pdgid: S046OTH
text:
AAD 2016AG searches for prompt lepton-jets using 20 fb**-1 of p p collisions at  sqrt(s) = 8 TeV collected with the ATLAS detector. Lepton-jets are expected from decays of  low-mass dark photons in SUSY-portal and Higgs-portal models. No significant excess of events is  observed and  95% CL upper limits are computed on the production cross section times  branching ratio for two prompt lepton-jets in models predicting 2 or 4 gamma_{{d}} via SUSY-portal  topologies, for gamma_{{d}} mass values between 0 and 2 GeV. See their Figs 9 and 10.  The results  are also interpreted in terms of a 90% CL exclusion region in kinetic mixing and dark-photon  mass parameter space. See their Fig. 13.


pdgid: S046OTH
text:
AAD 2013P searched in 5 fb**-1 of p p collisions at sqrt(s) = 7 TeV for single lepton-jets with at least four muons;  pairs of lepton-jets, each with two or more muons; and pairs of lepton-jets with two or more electrons. All of these could  be signatures of Hidden Valley supersymmetric models. No statistically significant deviations from the Standard Model expectations  are found. 95% C.L. limits are placed on the production cross section times branching ratio of dark photons for several  parameter sets of a Hidden Valley model.


pdgid: S046OTH
text:
AALTONEN 2012AB looked in 5.1 fb**-1 of p pbar collisions at sqrt(s) = 1.96 TeV for anomalous production  of multiple low-energy leptons in association with a W or Z boson. Such events may occur in hidden valley models  in which a supersymmetric Higgs boson is produced in association with a W or Z boson, with H --> chitilde_1()0 chitilde_1()0 pair and with the chitilde_{{1}}()0 further decaying into a dark photon (gamma_{{D}})  and the unobservable lightest SUSY particle of the hidden sector. As the gamma_{{D}} is expected to be light, it may decay  into a lepton pair. No significant excess over the SM expectation is observed and a limit at 95% C.L. is set on the cross section for a benchmark model of supersymmetric hidden-valley Higgs production.


pdgid: S046OTH
text:
AAD 2011AA looked in 34 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with >=4 jets  originating from pair production of scalar gluons, each decaying to two gluons. No two-jet resonances are observed over the  SM background. Limits are derived on the cross section times branching ratio (see Fig. 3). Assuming 100% branching  ratio for the decay to two gluons, the quoted exclusion range is obtained, except for a 5 GeV mass window around 140 GeV.


pdgid: S046OTH
text:
CHATRCHYAN 2011E looked in 35 pb**-1 of p p collisions at sqrt(s) = 7 TeV for events with collimated mu pairs (leptonic jets) from the decay of hidden sector states. No evidence for new resonance production is found. Limits are derived and compared to various SUSY models (see Fig. 4) where the LSP, either the chitilde_{{1}}()0 or a qtilde, decays to dark sector particles.


pdgid: S046OTH
text:
ABAZOV 2010N looked in 5.8 fb**-1 of p pbar collisions at sqrt(s) = 1.96 TeV for events from hidden valley models in which a chitilde_{{1}}^0() decays into a dark photon, gamma_{{D}}, and the unobservable lightest SUSY particle of the hidden sector.  As the gamma_{{D}} is expected to be light, it may decay into a tightly collimated lepton pair, called lepton jet. They searched for events with notET and two isolated lepton jets observable by an opposite charged lepton pair e e , e mu or mu mu. No significant excess over the SM expectation is observed, and a limit at 95% C.L. on the cross section times branching ratio is derived, see their Table I. They also examined the invariant mass of the lepton jets for a narrow resonance, see their Fig. 4, but found no evidence for a signal.


pdgid: S057DSB
text:
AAD 2020AM search for a top-color Z^' decaying to t tbar in p p collisions at  sqrt(s) = 13 TeV. The quoted limit is for width(Z^')/M(Z^') = 0.01. The limit becomes  M(Z^') > 4700 GeV for width(Z^')/M(Z^') = 0.03.


pdgid: S057DSB
text:
AAD 2020W search for techni-rho decaying to pi_T W in p p collisions at sqrt(s)  = 13 TeV. See their Fig. 5a for limits on .


pdgid: S057DSB
text:
AAD 2016W search for color octet vector resonance decaying to b B in p p collisions  at sqrt(s) = 8 TeV. The vector like quark B is assumed to decay to b H. See their Fig.3  and Fig.4 for limits on sigma.B.


pdgid: S057DSB
text:
KHACHATRYAN 2016E search for top-color Z^' decaying to t tbar. The quoted limit is for width(Z^')/mass(Z^')  = 0.012. Also exclude mass(Z^') < 2.9 TeV for wider topcolor Z^' with width(Z^')/mass(Z^') = 0.1.


pdgid: S057DSB
text:
AAD 2015AB search for long-lived hidden valley pi_{{v}} particles which are produced in pairs by the decay of a scalar boson. pi_{{v}} is assumed to decay into dijets. See their Fig. 10 for the limit on sigmaB.


pdgid: S057DSB
text:
AAD 2015AO search for top-color Z^' decaying to t tbar. The quoted limit is for  width(Z^')/mass(Z^')  = 0.012.


pdgid: S057DSB
text:
AAD 2015BB search for minimal walking technicolor (MWT) isotriplet vector and axial-vector resonances decaying to W h or Z h. See their Fig. 3 for the exclusion limit in the MWT parameter space.


pdgid: S057DSB
text:
AAD 2015Q search for long-lived hidden valley pi_{{v}} particles which are produced in pairs by the decay of scalar boson. pi_{{v}} is assumed to decay into dijets. See their Fig. 5 and Fig. 6 for the limit on sigmaB.


pdgid: S057DSB
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AAIJ 2015AN search for long-lived hidden valley pi_{{v}} particles which are produced in pairs by the decay of scalar boson with a mass of 120GeV. pi_{{v}} is assumed to decay into dijets. See their Fig. 4 for the limit on sigma B.


pdgid: S057DSB
text:
KHACHATRYAN 2015C search for a vector techni-resonance decaying to W Z. The limit assumes M(pi_{{T}}) = (3/4) M(rho_{{T}}) - 25 GeV. See their Fig.3 for the limit in M(pi_{{T}})-M(rho_{{T}}) plane of the low scale technicolor model.


pdgid: S057DSB
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KHACHATRYAN 2015W search for long-lived hidden valley pi_{{v}} particles which are produced in pairs in the decay of heavy higgs boson H. pi_{{v}} is assumed to decay into lepton+ lepton-. See their Fig. 7 and Fig. 8 for the limits on sigma B.


pdgid: S057DSB
text:
AAD 2014AT search for techni-omega and techni-a resonances decaying to V gamma with V = W(lepton nu) or Z(lepton+ lepton-).


pdgid: S057DSB
text:
AAD 2014V search for vector techni-resonances decaying into electron or muon pairs  in p p collisions at sqrt(s) = 8 TeV. See their table IX for exclusion limits with various assumptions.


pdgid: S057DSB
text:
CHATRCHYAN 2013AP search for top-color leptophobic Z^' decaying to t tbar. The quoted limit is for width(Z^')/mass(Z^') = 0.012.


pdgid: S057DSB
text:
BAAK 2012 give electroweak oblique parameter constraints on the QCD-like technicolor models. See their Fig. 28.


pdgid: S057DSB
text:
CHATRCHYAN 2012AF search for a vector techni-resonance decaying to W Z. The limit assumes M(pi_{{T}})= (3/4) M(rho_{{T}})- 25GeV. See their Fig. 3 for the limit in M(pi_{{T}})-M(rho_{{T}}) plane of the low scale technicolor model.


pdgid: S057DSB
text:
Using the LHC limit on the Higgs boson production cross section, CHIVUKULA 2011 obtain a limit on the top-Higgs mass > 300 GeV at 95% CL assuming 150 GeV top-pion mass.


pdgid: S057DSB
text:
Using the LHC limit on the Higgs boson production cross section, CHIVUKULA 2011A obtain a limit on the techinipion mass ruling out the region 110 GeV < mass(P) < 2mass(t). Existence of color techni-fermions, top-color mechanism, and N_{{TC}}() >= 3 are assumed.


pdgid: S057DSB
text:
AALTONEN 2010I search for the vector techni-resonances (rho_{{T}}, omega_{{T}}) decaying into W pi_T with W --> lepton nu and pi_T --> b bbar, b cbar, or b ubar. See their Fig.3 for the exclusion plot in M(pi_{{T}})-M(rho_{{T}}) plane.


pdgid: S057DSB
text:
ABAZOV 2010A search for a vector techni-resonance decaying into W Z.  The limit assumes M(rho_{{T}})< M(pi_{{T}}) + M(W).


pdgid: S057DSB
text:
ABAZOV 2007I search for the vector techni-resonances (rho_{{T}}, omega_{{T}}) decaying into W pi_T with W --> e nu and pi_T --> b bbar or b cbar. See their Fig. 2 for the exclusion plot in M(pi_{{T}})-M(rho_{{T}}) plane.


pdgid: S057DSB
text:
ABULENCIA 2005A search for resonances decaying to electron or muon pairs in p pbar collisions. at sqrt(s) = 1.96 TeV. The limit assumes Technicolor-scale mass parameters M_{{V}} = M_{{A}} = 500 GeV.


pdgid: S057DSB
text:
CHEKANOV 2002B search for color octet techni-pi P decaying into dijets in e p collisions. See their Fig.5 for the limit on sigma(e p --> e P X).B(P --> 2j).


pdgid: S057DSB
text:
ABAZOV 2001B searches for vector techni-resonances (rho_{{{T}}},omega_{{{T}}}) decaying to e+ e-.  The limit assumes M(rho_{{{T}}}) = M(omega_{{{T}}}) <M(pi_{{{T}}})+M(W).


pdgid: S057DSB
text:
The limit is independent of the pi_{{{T}}} mass.  See their Fig.9 and Fig.10 for the exclusion plot in the M(rho_{{{T}}})-M(pi_{{{T}}}) plane. ABDALLAH 2001 limit on the techni-pion mass is M(pi_{{{T}}})>79.8 GeV for N(D)=2, assuming its point-like coupling to gauge bosons.


pdgid: S057DSB
text:
AFFOLDER 2000F search for rho_{{{T}}} decaying into W pi_T or pi_T pi_T with W --> lepton nu and pi_T --> bbar b, bbar c. See Fig.1 in the above Note on ``Dynamical Electroweak Symmetry  Breaking'' for the exclusion plot in the M(rho_{{{T}}})-M(pi_{{{T}}}) plane.


pdgid: S057DSB
text:
AFFOLDER 2000K search for the rho_{{{T8}}} decaying into pi_LQ pi_LQ with pi_LQ --> b nu. For pi_LQ --> c nu, the limit is M(rho_{{{T8}}})>510GeV. See their Fig.2 and Fig.3 for the exclusion plot in the M(rho_{{{T8}}})-M(pi_{{LQ}}) plane.


pdgid: S057DSB
text:
ABE 1999F search for a new particle X decaying into b bbar in p pbar collisions at Ecm= 1.8 TeV. See Fig.7 in the above Note on ``Dynamical Electroweak Symmetry  Breaking'' for the upper limit on sigma(p pbar --> X)*B(X --> b bbar). ABE 1999F also exclude top gluons of width Gamma=0.3M in the mass interval 280<M<670 GeV, of width Gamma=0.5M in the mass interval 340<M<640 GeV, and of width Gamma=0.7M in the mass interval 375<M<560 GeV.


pdgid: S057DSB
text:
ABE 1999N search for the techni-omega decaying into gamma pi_T.  The technipion is assumed to decay pi_T --> b bbar. See Fig.2 in the above Note on ``Dynamical Electroweak Symmetry  Breaking'' for the exclusion plot in the M(omega_{{{T}}})-M(pi_{{{T}}}) plane.


pdgid: S057DSB
text:
ABE 1997G search for a new particle X decaying into dijets in p pbar collisions at Ecm= 1.8 TeV. See Fig.5 in the above Note on ``Dynamical Electroweak Symmetry  Breaking'' for the upper limit on sigma(p pbar --> X)*B(X --> 2j).


pdgid: S054CTL
text:
BABICH 2003 obtain a bound -0.175 TeV**-2<1/Lambda(LL)**2 <0.095 TeV**-2 (95%CL) in a model independent analysis allowing all of Lambda(LL), Lambda(LR), Lambda(RL), Lambda(RR) to coexist.


pdgid: S054CTH
text:
AABOUD 2017AT limits are from p p collisions at sqrt(s) = 13 TeV. The quoted limit uses  a uniform positive prior in 1/Lambda^2.


pdgid: S054CTH
text:
AAD 2021AU search for new phenomena in final states with e+ e- and one or no b-tagged  jets in p p collisions at sqrt(s) = 13 TeV. The quoted limits assume g_{{*}}^2 = 4 pi.


pdgid: S054CTH
text:
AAD 2021Q limits are from p p collisions at sqrt(s) = 13 TeV. A frequentist statistical  framework  is used to remove the prior dependence.


pdgid: S054CTH
text:
AABOUD 2016U limits are from p p collisions at sqrt(s) = 13 TeV. The quoted limit uses a  uniform positive prior in 1/Lambda^2.


pdgid: S054CTH
text:
AAD 2014BE limits are from p p collisions at sqrt(s) = 8 TeV. The quoted limit uses a uniform positive prior in 1/Lambda^2.


pdgid: S054CTH
text:
ABDALLAH 2011 limit is from e+ e- --> t cbar cross section. Lambda_{{LL}} = Lambda_{{LR}} = Lambda_{{RL}} = Lambda_{{RR}} is assumed.


pdgid: S054CTS
text:
AAD 2021AU search for new phenomena in final states with mu+ mu- and one or no  b-tagged jets in p p collisions at sqrt(s) = 13 TeV. The quoted limits assume g_{{*}}^2 =  4 pi.


pdgid: S054CTS
text:
AAD 2021Q limits are from p p collisions at sqrt(s) = 13 TeV. A frequentist statistical  framework is used to remove the prior dependence.


pdgid: S054CTN
text:
JODIDIO 1986 limit is from mu+ --> nubar_mu e+ nu_e. Chirality invariant interactions L = (g**2/Lambda**2) [eta(LL) (nubar_{{mu L}}gamma**alphamu_{{L}}) (ebar_{{L}}gamma(alpha)nu_{{e L}}) + eta_{{LR}} (nubar_{{mu L}}gamma**alphanu_{{e L}} (ebar_{{R}}gamma_{{alpha}}mu_{{R}})] with g**2/4pi = 1 and (eta(LL),eta(LR)) = (0,+-1) are taken. No limits are given for Lambda(LL)**+- with (eta(LL),eta(LR)) = (+-1,0).  For more general constraints with right-handed neutrinos and chirality nonconserving contact interactions, see their text.


pdgid: S054CTN
text:
DIAZCRUZ 1994 limits are from Gamma(tau --> e nu nu) and assume flavor-dependent contact interactions with Lambda(tau nu_tau e nu_e)<<Lambda(mu nu_mu e nu_e).


pdgid: S054CTN
text:
DIAZCRUZ 1994 limits are from Gamma(tau --> mu nu nu) and assume flavor-dependent contact interactions with Lambda(tau nu_tau mu nu_mu)<<Lambda(mu nu_mu e nu_e).


pdgid: S054CTQ
text:
AABOUD 2017AK limit is from dijet angular distribution in p p collisions at sqrt(s) = 13  TeV. u, d, and s quarks are assumed to be composite.


pdgid: S054CTQ
text:
AABOUD 2018AV obtain limit on t_{{R}} compositeness  2pi/Lambda_{{RR}}^2 < 1.6  TeV**-2 at 95% CL from t tbar t tbar production in the p p collisions at  Ecm = 13 TeV.


pdgid: S054CTQ
text:
SIRUNYAN 2017F limit is from dijet angular cross sections in p p collisions at Ecm  = 13 TeV. All quarks are assumed to be composite.


pdgid: S054CTQ
text:
AAD 2016S limit is from dijet angular selections in p p collisions  at Ecm = 13 TeV. u, d, and s quarks are assumed to be composite.


pdgid: S054CTQ
text:
AAD 2015AR obtain limit on the t_{{R}} compositeness 2pi/Lambda_{{RR}}^2() <  6.6 TeV**-2 at 95% CL from the t tbar t tbar production in the p p collisions at Ecm = 8 TeV.


pdgid: S054CTQ
text:
AAD 2015BY obtain limit on the t_{{R}} compositeness  2pi/Lambda(RR)**2 < 15.1 TeV**-2 at 95% CL from the t tbar t tbar production in the p p collisions at Ecm = 8 TeV.


pdgid: S054CTQ
text:
AAD 2015L limit is from dijet angular distribution in p p collisions at Ecm = 8 TeV.  u, d, and s quarks are assumed to be composite.


pdgid: S054CTQ
text:
KHACHATRYAN 2015J limit is from dijet angular distribution in p p  collisions at Ecm = 8 TeV. u, d, s, c, and b quarks are assumed to be composite.


pdgid: S054CTQ
text:
FABBRICHESI 2014 obtain bounds on chromoelectric  and chromomagnetic form factors of the top-quark using p p --> t tbar and p pbar --> t tbar cross sections. The quoted limit on the q qbar t tbar contact interaction is derived from their bound on the chromoelectric form factor.


pdgid: S054CTD
text:
AAD 2024AC limit is from the measurement of the t tbar production cross section with  large missing notET in p p collisions at sqrt(s) = 13 TeV.


pdgid: S054EXP
text:
From e+ e- collisions at sqrt(s) = 189 -- 209 GeV. f = f^' is assumed. ACHARD 2003B also obtain limit for f = -f^': mass(e^*)>96.6 GeV.


pdgid: S054EXS
text:
SIRUNYAN 2020AJ search for e^* production in 2e 2j final states in p p collisions  at sqrt(s) = 13 TeV. The quoted limit assumes Lambda = mass(e^*), f = f^' = 1. The  contact interaction is included. See their Fig.11 for exclusion limits in  mass(e^*)-Lambda plane.


pdgid: S054EXS
text:
AABOUD 2019AZ search for single e^* production in p p collisions at sqrt(s) = 13  TeV. The limit quoted above is from e^* --> e q qbar and e^* --> nu W decays assuming f  = f^' = 1 and mass(e^*) = Lambda. The contact interaction is included in e^*  production and decay amplitudes. See their Fig.6 for exclusion limits in  mass(e^*)-Lambda plane.


pdgid: S054EXS
text:
SIRUNYAN 2019Z search for e^* production in lepton lepton gamma final states in p p  collisions at sqrt(s) = 13 TeV. The quoted limit assumes Lambda = mass(e^*), f =  f^' = 1. The contact interaction is included in the e^* production and decay amplitudes.


pdgid: S054EXS
text:
KHACHATRYAN 2016AQ search for single e^* production in p p collisions at sqrt(s) = 8  TeV. The limit above is from the e^* --> e gamma search channel assuming f = f^' = 1,  mass(e^*) = Lambda. See their Table 7 for limits in other search channels or with  different assumptions.


pdgid: S054EXS
text:
AAD 2015AP search for e^* production in  evens with three or more charged leptons in p p collisions  at sqrt(s) = 8 TeV. The quoted limit assumes Lambda = mass(e^*),  f = f^' = 1. The contact interaction is included in the e^* production and decay amplitudes.


pdgid: S054EXS
text:
AAD 2013BB search for single e^* production in p p collisions with e^* --> e gamma decay. f = f^' = 1, and e^* production via  contact interaction with Lambda = mass(e^*) are assumed.


pdgid: S054EXS
text:
CHATRCHYAN 2013AE search for single e^* production in p p collisions with e^* --> e gamma decay. f = f^' = 1, and e^* production via  contact interaction with Lambda = mass(e^*) are assumed.


pdgid: S054EXS
text:
AAD 2012AZ search for e^* production via four-fermion contact  interaction in p p collisions with e^* --> e gamma decay. The quoted limit assumes Lambda = mass(e^*). See their Fig. 8 for the exclusion plot in the mass-coupling plane.


pdgid: S054EXG
text:
ABDALLAH 2004N also obtain a limit on the excited electron mass with e e^* chiral coupling, mass(e^*)>295 GeV at 95% CL.


pdgid: S054EXI
text:
DORENBOSCH 1989 obtain the limit lambda(gamma)**2Lambda(cut)**2/mass**2(e^*) < 2.6 (95% CL), where Lambda(cut) is the cutoff scale, based on the one-loop calculation by GRIFOLS 1986.  If one assumes that Lambda(cut) = 1 TeV and lambda_{{gamma}} = 1, one obtains mass(e^*) > 620 GeV.  However, one generally expects lambda_{{gamma}} ~~ mass(e^*)/Lambda(cut) in composite models.


pdgid: S054EXI
text:
GRIFOLS 1986 uses nu_mu e --> nu_mu e and nubar_mu e --> nubar_mu e data from CHARM Collaboration to derive mass limits which depend on the scale of compositeness.


pdgid: S054EXI
text:
RENARD 1982 derived from g-2 data limits on mass and couplings of e^* and mu^*.  See figures 2 and 3 of the paper.


pdgid: S054MXP
text:
From e+ e- collisions at sqrt(s) = 189 -- 209 GeV. f = f^' is assumed. ACHARD 2003B also obtain limit for f = -f^': mass(mu^*)>96.6 GeV.


pdgid: S054MXS
text:
SIRUNYAN 2020AJ search for mu^* production in 2mu 2j final states in p p  collisions at sqrt(s) = 13 TeV. The quoted limit assumes Lambda = mass(mu^*), f = f^'  = 1. The contact interaction is included. See their Fig.11 for exclusion limits in  mass(mu^*)-Lambda plane.


pdgid: S054MXS
text:
SIRUNYAN 2019Z search for mu^* production in lepton lepton gamma final states in p p  collisions at sqrt(s) = 13 TeV. The quoted limit assumes Lambda = mass(mu^*), f =  f^' = 1. The contact interaction is included in the mu^* production and decay amplitudes.


pdgid: S054MXS
text:
AAD 2016BM search for mu^* production in mu mu j j events in p p collisions at  sqrt(s) = 8 TeV. Both the production and decay are assumed to occur via a contact interaction with  Lambda = mass(mu^*).


pdgid: S054MXS
text:
KHACHATRYAN 2016AQ search for single mu^* production in p p collisions at sqrt(s) =  8  TeV. The limit above is from the mu^* --> mu gamma search channel assuming f = f^' =  1,  mass(mu^*) = Lambda. See their Table 7 for limits in other search channels or with   different assumptions.


pdgid: S054MXS
text:
AAD 2015AP search for mu^* production in  evens with three or more charged leptons in p p collisions  at sqrt(s) = 8 TeV. The quoted limit assumes Lambda = mass(mu^*),  f = f^' = 1. The contact interaction is included in the mu^* production and decay amplitudes.


pdgid: S054MXS
text:
AAD 2013BB search for single mu^* production in p p collisions with mu^* --> mu gamma decay. f = f^' = 1, and mu^* production via  contact interaction with Lambda = mass(mu^*) are assumed.


pdgid: S054MXS
text:
CHATRCHYAN 2013AE search for single mu^* production in p p collisions with mu^* --> mu gamma decay. f = f^' = 1, and mu^* production via  contact interaction with Lambda = mass(mu^*) are assumed.


pdgid: S054MXS
text:
AAD 2012AZ search for mu^* production via four-fermion contact  interaction in p p collisions with mu^* --> mu gamma decay. The quoted limit assumes Lambda = mass(mu^*). See their Fig. 8 for the exclusion plot in the mass-coupling plane.


pdgid: S054TXP
text:
From e+ e- collisions at sqrt(s) = 189 -- 209 GeV. f = f^' is assumed. ACHARD 2003B also obtain limit for f = -f^': mass(tau^*)>96.6 GeV.


pdgid: S054TXS
text:
AAD 2023BJ search for tau^* produced in association with tau and decaying into tau q qbar  via a contact interaction with g(contact)**2 = (4pi)**2. The limit  quoted above assumes Lambda = mass(tau^*).


pdgid: S054TXS
text:
AAD 2015AP search for tau^* production in  events with three or more charged leptons in p p collisions  at sqrt(s) = 8 TeV. The quoted limit assumes Lambda = mass(tau^*), f = f^' = 1. The contact interaction is included in the tau^* production and decay amplitudes.


pdgid: S054TXS
text:
ACHARD 2003B result is from e+ e- collisions at sqrt(s) = 189 -- 209 GeV. f = f^' = Lambda/mass(tau^*) is assumed. See their Fig.4 for the exclusion plot in the mass-coupling plane.


pdgid: S054TXS
text:
ABBIENDI 2002G result is from e+ e- collisions at sqrt(s) = 183 -- 209 GeV. f = f^' = Lambda/mass(tau^*) is assumed for tau^* coupling. See their Fig.4c for the exclusion limit in the mass-coupling plane.


pdgid: S054EXN
text:
AAD 2015AP search for nu^* pair production in  evens with three or more charged leptons in p p collisions  at sqrt(s) = 8 TeV. The quoted limit assumes Lambda = mass(nu^*), f = f^' = 1. The contact interaction is included in the nu^* production and decay amplitudes.


pdgid: S054EXN
text:
From e+ e- collisions at sqrt(s) = 192 -- 209 GeV, ABBIENDI 2004N obtain limit on CS(e+ e- --> nu^* nu^*) B**2(nu^* --> nu gamma). See their Fig.2. The limit ranges from 20 to 45 fb for mass(nu^*) > 45 GeV.


pdgid: S054EXN
text:
From e+ e- collisions at sqrt(s) = 189 -- 209 GeV. f = -f^' is assumed. ACHARD 2003B also obtain limit for f = f^': mass(nu_{{e}}^*)>101.7 GeV, mass(nu_{{mu}}^*)>101.8 GeV, and mass(nu_{{tau}}^*)>92.9 GeV. See their Fig.4 for the exclusion plot in the mass-coupling plane.


pdgid: S054EXO
text:
AARON 2008 search for single nu^*() production in e p collisions with the decays nu^*() --> nu gamma, nu Z, e W. The quoted limit assumes f = -f^'() = Lambda/mass(nu^*()). See their Fig. 3 and Fig. 4  for the exclusion plots in the mass-coupling plane.


pdgid: S054EXO
text:
TUMASYAN 2023AL search for Majorana excited neutrino nu^* produced and decaying via gauge  and contact interactions. The limit quoted above is for lepton = e with Lambda =  M(nu^*). The limit  becomes M(nu^*) > 6.1 TeV for lepton = mu.


pdgid: S054EXO
text:
ACHARD 2003B result is from e+ e- collisions at sqrt(s) = 189 -- 209 GeV. The quoted limit is for nu_{{e}}^*. f = -f^' = Lambda/mass(nu^*) is assumed. See their Fig.4 for the exclusion plot in the mass-coupling plane.


pdgid: S054EXO
text:
ADLOFF 2002 search for single nu^* production in e p collisions with the decays nu^* --> nu gamma, nu Z, e W. The quoted limit assumes f = -f^' = Lambda/mass(nu^*). See their Fig.1 for the exclusion plots in the mass-coupling plane.


pdgid: S054EXO
text:
CHEKANOV 2002D search for single nu^* production in e p collisions with the decays nu^* --> nu gamma, nu Z, e W. f = -f^' = Lambda/mass(nu^*) is assumed for the e^* coupling. CHEKANOV 2002D also obtain limit for f = f^' = Lambda/mass(nu^*): mass(nu^*)>135 GeV. See their Fig.5c and Fig.5d for the exclusion plot in the mass-coupling plane.


pdgid: S054EQP
text:
AALTONEN 2010H obtain limits on the q^*() q^*() production cross section in p pbar collisions. See their Fig.3.


pdgid: S054EQP
text:
SIRUNYAN 2018V search for pair production of spin 3/2 excited top quarks. B(t_3/2^*() --> t g) =  1 is assumed.


pdgid: S054EQP
text:
BARATE 1998U obtain limits on the form factor. See their Fig.16 for limits in mass-form factor plane.


pdgid: S054EQS
text:
TUMASYAN 2023AF limit quoted above assumes b g --> b^* production. The limit becomes  mass(b^*) >   4TeV if contact interaction is included in the b^* production  cross section. See  their  Fig. 5 for limits on .


pdgid: S054EQS
text:
TUMASYAN 2023BC search for excited light flavor quark q^* in p p collisions at  sqrt(s) = 13 TeV. f = 1.0 is assumed.


pdgid: S054EQS
text:
TUMASYAN 2023BC search for excited b quark b^* in p p collisions at sqrt(s) = 13  TeV. $b^*$ production via gauge interactions and f = 1.0 are assumed.  The limit becomes  $m_{b^*}>3.8$TeV if contact interaction is included in the $b^*$ production cross section.


pdgid: S054EQS
text:
AAD 2020T search for resonances decaying into dijets in p p collisions at sqrt(s) = 13  TeV. Assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1.


pdgid: S054EQS
text:
SIRUNYAN 2020AI search for resonances decaying into dijets in p p collisions at sqrt(s)  = 13 TeV. Assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1.


pdgid: S054EQS
text:
AABOUD 2018AB assume  Lambda = mass(b^*), f_{{s}} = f = f^' = 1. The contact  interactions are not included in b^* production  and decay amplitudes.


pdgid: S054EQS
text:
AABOUD 2018BA search for first-generation excited quarks  (u^* and d^*) with  degenerate mass, assuming Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The contact  interactions are not included in q^* production and decay amplitudes.


pdgid: S054EQS
text:
SIRUNYAN 2018AG search for first-generation excited quarks  (u^* and d^*) with  degenerate mass, assuming  Lambda = mass(q^*), f_{{s}} = f = f^' = 1.


pdgid: S054EQS
text:
SIRUNYAN 2018BO assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The contact  interactions are not included in q^* production and decay amplitudes.


pdgid: S054EQS
text:
AABOUD 2017AK assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The contact  interactions are not included in q^* production and decay amplitudes. Only the decay of q^* --> g u  and q^* --> g d is simulated as the benchmark signals in the analysis.


pdgid: S054EQS
text:
HAYRAPETYAN 2024G search for singly produced narrow resonances decaying to j j j in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 3 for limits on .


pdgid: S054EQS
text:
TUMASYAN 2022O search for b^* decaying to t W in p p collisions at sqrt(s) = 13   TeV. The limit quoted above assumes kappa_{{L}}^b = g_{{L}} = 1, kappa_{{R}}^b = g_{{R}} = 0. The   limit becomes mass(b^*) > 3.0 TeV (>3.2 TeV) if we assume kappa_{{L}}^b = g_{{L}} = 0,   kappa_{{R}}^b = g_{{R}} = 1 (kappa_{{L}}^b = g_{{L}} = 1, kappa_{{R}}^b = g_{{R}} = 1). See their   Fig. 3 for limits on .


pdgid: S054EQS
text:
SIRUNYAN 2021AG search for b^* decaying to t W in p p collisions at sqrt(s) = 13  TeV. The limit  quoted above assumes kappa_{{L}}^b = g_{{L}} = 1, kappa_{{R}}^b = g_{{R}} = 0. The  limit becomes mass(b^*) > 2.8 TeV (> 3.1 TeV) if we assume kappa_{{L}}^b = g_{{L}} =  0, kappa_{{R}}^b = g_{{R}} = 1 (kappa_{{L}}^b = g_{{L}} = kappa_{{R}}^b = g_{{R}} = 1). See their  Fig. 5 for limits on .


pdgid: S054EQS
text:
KHACHATRYAN 2017W assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The  contact interactions are not included  in q^* production and decay amplitudes.


pdgid: S054EQS
text:
AABOUD 2016 assume Lambda = mass(b^*), f_{{s}} = f = f^' = 1. The contact  interactions are not included in the b^* production and decay amplitudes.


pdgid: S054EQS
text:
AAD 2016AH search for b^* decaying to t W in p p collisions at sqrt(s) = 8 TeV.  f_{{g}} = f_{{L}} = f_{{R}} = 1 are assumed. See their Fig. 12b for limits on  sigma.B.


pdgid: S054EQS
text:
AAD 2016AV search for single production of vector-like quarks decaying to W b in p p  collisions. See their Fig. 8 for the limits on couplings and mixings.


pdgid: S054EQS
text:
AAD 2016S assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The contact  interactions are not included in q^* production and decay amplitudes.


pdgid: S054EQS
text:
KHACHATRYAN 2016I search for b^* decaying to t W in p p collisions at sqrt(s) = 8 TeV.  kappa_{{L}}^b() = g_{{L}} = 1, kappa_{{R}}^b() = g_{{R}} = 0 are  assumed. See their Fig. 8 for limits on sigma B.


pdgid: S054EQS
text:
KHACHATRYAN 2016K assume Lambda = mass(q^*), f_{{s}} = f = f^'= 1. The contact  interactions are not included in q^* production and decay amplitudes.


pdgid: S054EQS
text:
KHACHATRYAN 2016L search for resonances decaying to dijets in p p collisions at sqrt(s)  = 8 TeV using the data scouting technique which increases the sensitivity to the low mass  resonances.


pdgid: S054EQS
text:
AAD 2015V assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The contact   interactions are not included in q^* production and decay amplitudes.


pdgid: S054EQS
text:
KHACHATRYAN 2015V assume Lambda = mass(q^*), f_{{s}} = f = f^' = 1. The contact interactions are not included in q^* production and decay amplitudes.


pdgid: S054CQ
text:
ABE 1989D look for pair production of unit-charged particles which leave the detector before decaying. In the above limit the color sextet quark is assumed to fragment into a unit-charged or neutral hadron with equal probability and to have long enough lifetime not to decay within the detector.  A limit of 121 GeV is obtained for a color decuplet.


pdgid: S054CL
text:
ABE 1989D look for pair production of unit-charged particles which leave the detector before decaying. In the above limit the color octet lepton is assumed to fragment into a unit-charged or neutral hadron with equal probability and to have long enough lifetime not to decay within the detector.  The limit improves to 99 GeV if it always fragments into a unit-charged hadron.


pdgid: S054CL
text:
ABT 1993 search for e_{{8}} production via e-gluon fusion in e p collisions with e_8 --> e g.  See their Fig.3 for exclusion plot in the mass(e_{{8}})--Lambda plane for mass(e_{{8}}) = 35 -- 220 GeV.


pdgid: S054CN
text:
BARGER 1989 used ABE 1989B limit for events with large missing transverse momentum.  Two-body decay nu_8 --> nu g is assumed.


pdgid: S054CN
text:
BARTEL 1987B is at Ecm = 46.3-46.78 GeV. The limit assumes the nu_{{8}} pair production cross section to be eight times larger than that of the corresponding heavy neutrino pair production.  This assumption is not valid in general for the weak couplings, and the limit can be sensitive to its SU(2)(L)xU(1)(Y) quantum numbers.


pdgid: S071DGF
text:
BLAKEMORE 2021 obtain constraints on non-Newtonian forces with strengths |alpha|  ~> E8 and length scales R > 10 mum. See their Fig. 4 for more details  including comparison with previous searches.


pdgid: S071DGF
text:
HEACOCK 2021 obtain constraints on non-Newtonian forces with strengths E18~<  |alpha|~< E25 and length scales R ~= 0.02 -- 10 nm. See  their Figure 3 for more details. This improves the results of HADDOCK 2018. These constraints  do not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
LEE 2020 search for new forces probing a range of |alpha| ~=   and length scales R ~= 7 -- 90 mum. For  delta = 1 the bound on R is 30 mum. See their Fig. 5 for details on the  bound.


pdgid: S071DGF
text:
TAN 2020A search for new forces probing a range of |alpha| ~=  4E-3 -- 1E2 and length scales R ~= 40 -- 350 mum. See their  Fig. 6 for details on the bound.


pdgid: S071DGF
text:
BERGE 2018 uses results from the MICROSCOPE experiment to obtain constraints on non-Newtonian  forces with strengths E-11~< |alpha|~< E-7 and length scales R  ~>E5 m. See their Figure 1 for more details. These constraints do not place limits on the  size of extra flat dimensions.


pdgid: S071DGF
text:
FAYET 2018A uses results from the MICROSCOPE experiment to obtain constraints on an  EP-violating force possibly arising from a new U(1) gauge boson. For R ~>E7 m  the limits are |alpha| ~< a few E-13 to a few E-11 depending on the coupling,  corresponding to |epsilon| ~< E-24 for the coupling of the new spin-1 or spin-0  mediator. These constraints do not place limits on the size of extra flat dimensions. This extends  the results of FAYET 2018.


pdgid: S071DGF
text:
KLIMCHITSKAYA 2017A uses an experiment that measures the difference of Casimir forces to  obtain bounds on non-Newtonian forces with strengths |alpha| ~= E5 -- E17 and  length scales R = 0.03 -- 10 mum. See their Fig. 3. These constraints do  not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
XU 2013 obtain constraints on non-Newtonian forces with strengths |alpha| ~= 10**34 -- 10**36 and length scales R ~= 1 -- 10 fm. See their  Fig. 4 for more details. These constraints do not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
BEZERRA 2011 obtain constraints on non-Newtonian forces with strengths E11~< |alpha|~< E18 and length scales R = 30 -- 1260 nm. See their Fig. 2 for more details. These constraints do not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
SUSHKOV 2011 obtain improved limits on non-Newtonian forces with strengths E7~< |alpha| ~< E11  and length scales 0.4 mum < R < 4 mum (95% CL). See their Fig. 2. These bounds do not place limits  on the size of extra flat dimensions. However, a model dependent bound of M_{{*}} > 70 TeV is obtained assuming gauge  bosons that couple to baryon number also propagate in (4 + delta) dimensions.


pdgid: S071DGF
text:
BEZERRA 2010 obtain improved constraints on non-Newtonian forces with strengths E19~< |alpha|~< E29 and length scales R = 1.6 -- 14 nm (95% CL). See their Fig.1. This bound does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
MASUDA 2009 obtain improved constraints on non-Newtonian forces with strengths E9~<|alpha|~<E11 and length scales R = 1.0 -- 2.9 mum (95% CL). See their Fig.3. This bound does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
GERACI 2008 obtain improved constraints on non-Newtonian forces with strengths |alpha| > 14,000 and length scales R = 5 -- 15 micrometers. See their Fig. 9. This bound does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
TRENKEL 2008 uses two independent measurements of Newton's constant G to constrain new forces with strength |alpha|~=E-4 and length scales R = 0.02 -- 1 m. See their Fig. 1. This bound does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
DECCA 2007A search for new forces and obtain bounds in the region with strengths  |alpha| ~= E13 -- E18 and length scales R = 20 -- 86 nm.  See their Fig. 6. This bound does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
KAPNER 2007 search for new forces, probing a range of |alpha| ~=  10**-3 -- 10**5 and length scales R ~= 10 -- 1000 mum. For  delta = 1 the bound on R is 44 mum. For delta = 2, the bound is  expressed in terms of M_{{*}}, here translated to a bound on the radius. See their Fig. 6 for  details on the bound.


pdgid: S071DGF
text:
TU 2007 search for new forces probing a range of |alpha| ~= E-1 -- E5 and length scales R ~= 20 -- 1000 mum. For delta = 1  the bound on R is 53 mum. See their Fig. 3 for details on the bound.


pdgid: S071DGF
text:
SMULLIN 2005 search for new forces, and obtain bounds in the region with strengths alpha ~= 10**3 -- 10**8 and  length scales R = 6 -- 20 mum. See their Figs.1 and 16 for details on the bound. This work does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
HOYLE 2004 search for new forces, probing alpha down to 10**-2 and distances down to 10mum. Quoted bound on R is for delta = 2. For delta = 1, bound goes to 160 mum. See their Fig. 34 for details on the bound.


pdgid: S071DGF
text:
CHIAVERINI 2003 search for new forces, probing alpha above 10**4 and lambda down to 3mum, finding no signal.  See their Fig.4 for details on the bound. This bound does not place limits on the size of extra flat dimensions.


pdgid: S071DGF
text:
LONG 2003 search for new forces, probing alpha down to 3, and distances down to about 10mum. See their Fig.4 for details on the bound.


pdgid: S071DGF
text:
HOYLE 2001 search for new forces, probing alpha down to 10**-2 and distances down to 20mum.  See their Fig.4 for details on the bound.  The quoted bound is for alpha >= 3.


pdgid: S071DGF
text:
HOSKINS 1985 search for new forces, probing distances down to 4mm. See their Fig.13 for details on the bound.  This bound does not place limits on the size of extra flat dimensions.


pdgid: S071OS6
text:
AAD 2021F search for p p --> j G, using 139 fb**-1 of data at sqrt(s) = 13 TeV to  place lower limits on M_{{D}} for two to six extra dimensions (see their Table X), from which this  bound on R is derived. This limit supersedes that in AABOUD 2018I.


pdgid: S071OS6
text:
HANNESTAD 2003 obtain a limit on R from the heating of old neutron stars by the surrounding cloud of trapped KK gravitons. Limits for all delta<=7 are given in their TablesV and VI. These limits supersede those in HANNESTAD 2002.


pdgid: S071OS6
text:
SIRUNYAN 2021A search for p p --> Z G, using 137 fb**-1 of data at sqrt(s) = 13 TeV  to place lower limits on M_{{D}} for two to seven extra dimensions (see their Figure 12), from  which this bound on R is derived. These limits supersede those obtained in SIRUNYAN 2018BV.


pdgid: S071OS6
text:
TUMASYAN 2021D search for p p --> j G, using 137 fb**-1 of data at sqrt(s) = 13 TeV   to place lower limits on M_{{D}} for two to seven extra dimensions (see their Table 3), from which   this bound on R is derived. This limit supersedes that in SIRUNYAN 2018S.


pdgid: S071OS6
text:
SIRUNYAN 2017AQ search for p p --> gamma G, using 12.9 fb**-1 of data at sqrt(s) =  13 TeV to place limits on M_{{D}} for three to six extra dimensions (see their Table 3).


pdgid: S071OS6
text:
AABOUD 2016F search for p p --> gamma G, using 3.2 fb**-1 of data at sqrt(s) = 13  TeV to place limits on M_{{D}} for two to six extra dimensions (see their Figure 9), from which  this bound on R is derived.


pdgid: S071OS6
text:
KHACHATRYAN 2016N search for p p --> gamma G, using 19.6 fb**-1 of data at sqrt(s) =  8 TeV to place limits on M_{{D}} for three to six extra dimensions (see their Table 5).


pdgid: S071OS6
text:
AAD 2015CS search for p p --> gamma G, using 20.3 fb**-1 of data at sqrt(s) = 8 TeV    to place lower limits on M_{{D}} for two to six extra dimensions (see their Fig. 18).


pdgid: S071OS6
text:
AAD 2013C search for p p --> gamma G, using 4.6 fb**-1 of data at sqrt(s) = 7 TeV to place bounds on M_{{D}} for two to six extra dimensions, from which this bound on R is derived.


pdgid: S071OS6
text:
AAD 2013D search for the dijet decay of quantum black holes in 4.8 fb**-1 of data produced in p p collisions  at sqrt(s) = 7 TeV to place bounds on M_{{D}} for two to seven extra dimensions, from which these bounds on R are derived. Limits on M_{{D}} for all delta <= 7 are given in their Table 3.


pdgid: S071OS6
text:
AJELLO 2012 obtain a limit on R from the gamma-ray emission of point gamma sources that arise from the photon decay of KK gravitons which are gravitationally bound around neutron stars. Limits for all delta <= 7 are given in their Table 7.


pdgid: S071OS6
text:
AALTONEN 2008AC search for p pbar --> gamma G and p pbar --> j G at sqrt(s) = 1.96 TeV with 2.0 fb**-1 and 1.1 fb**-1 respectively, in order to place bounds on the fundamental scale and size of the extra dimensions. See their Table III for limits on all delta<= 6.


pdgid: S071OS6
text:
ABAZOV 2008S search for p pbar --> gamma G, using 1 fb**-1 of data at sqrt(s) = 1.96 TeV to place bounds on M_{{D}} for two to eight extra dimensions, from which these bounds on R are derived. See their paper for intermediate values of delta.


pdgid: S071OS6
text:
DAS 2008 obtain a limit on R from Kaluza-Klein graviton cooling of SN1987A due to plasmon-plasmon annihilation.


pdgid: S071OS6
text:
ABULENCIA,A 2006 search for p pbar --> j G using 368 pb**-1 of data at sqrt(s) = 1.96 TeV. See their Table II for bounds for all delta <= 6.


pdgid: S071OS6
text:
ABDALLAH 2005B search for e+ e- --> gamma G at sqrt(s) = 180 -- 209~GeV to place bounds on the size of extra dimensions and the fundamental scale.  Limits for all delta <= 6 are given in their Table~6. These limits supersede those in ABREU 2000Z.


pdgid: S071OS6
text:
ACHARD 2004E search for e+ e- --> gamma G at sqrt(s) = 189 -- 209~GeV to place bounds on the size of extra dimensions and the fundamental scale.  See their Table~8 for limits with delta <= 8. These limits supersede those in ACCIARRI 1999R.


pdgid: S071OS6
text:
ACOSTA 2004C search for pbar p --> j G at sqrt(s) = 1.8~TeV to place bounds on the size of extra dimensions and the fundamental scale. See their paper for bounds on delta~=~4,~6.


pdgid: S071OS6
text:
CASSE 2004 obtain a limit on R from the gamma-ray emission of point gamma sources that arises from the photon decay of gravitons around newly born neutron stars, applying the technique of HANNESTAD 2003 to neutron stars in the galactic bulge. Limits for all delta<=7 are given in their Table~I.


pdgid: S071OS6
text:
ABAZOV 2003 search for p pbar --> j G at sqrt(s)=1.8 TeV to place bounds on M(D) for 2 to 7 extra dimensions, from which these bounds on R are derived.  See their paper for bounds on intermediate values of delta. We quote results without the approximate NLO scaling introduced in the paper.


pdgid: S071OS6
text:
HANNESTAD 2003 obtain a limit on R from graviton cooling of supernova SN1987a.  Limits for all delta<=7 are given in their TablesV and VI.


pdgid: S071OS6
text:
HANNESTAD 2003 obtain a limit on R from gravitons emitted in supernovae and which subsequently decay, contaminating the diffuse cosmicgamma background. Limits for all delta<=7 are given in their TablesV and VI. These limits supersede those in HANNESTAD 2002.


pdgid: S071OS6
text:
HANNESTAD 2003 obtain a limit on R from gravitons emitted in two recent supernovae and which subsequently decay, creating pointgamma sources. Limits for all delta<=7 are given in their TablesV and VI. These limits are corrected in the published erratum.


pdgid: S071OS6
text:
HEISTER 2003C use the process e+ e- --> gamma G at sqrt(s) = 189 -- 209 GeV to place bounds on the size of extra dimensions and the scale of gravity. See their Table4 for limits with delta<=6 for derived limits on M(D).


pdgid: S071OS6
text:
FAIRBAIRN 2001 obtains bounds on R from over production of KK gravitons in the early universe. Bounds are quoted in paper in terms of fundamental scale of gravity. Bounds depend strongly on temperature of QCD phase transition and range from R<0.13mum to 0.001mum for delta=2; bounds for delta=3,4 can be derived from Table1 in the paper.


pdgid: S071OS6
text:
HANHART 2001 obtain bounds on R from limits on graviton cooling of supernova SN1987a using numerical simulations of proto-neutron star neutrino emission.


pdgid: S071OS6
text:
CASSISI 2000 obtain rough bounds on M(D) (and thus R) from red giant cooling for delta=2,3. See their paper for details.


pdgid: S071OS6
text:
ACCIARRI 1999S search for e+ e- --> Z G at sqrt(s)=189 GeV. Limits on the gravity scale are found in their Table2, for delta<=4.


pdgid: S071GEX
text:
SIRUNYAN 2018DD use dijet angular distributions in 35.9 fb**-1 of data from p p  collisions at sqrt(s) = 13 TeV to place a lower bound on Lambda_{{T}}, here converted to M_{{TT}}.  This updates the results of SIRUNYAN 2017F.


pdgid: S071GEX
text:
GIUDICE 2003 place bounds on Lambda(6), the coefficient of the gravitationally-induced dimension-6 operator (2pilambda/Lambda(6)**2)(Sumfbargamma(mu)gamma**5f)(Sumfbargamma**mugamma**5f), using data from a variety of experiments.  Results are quoted for lambda=+-1 and are independent of delta.


pdgid: S071GEX
text:
HAYRAPETYAN 2024AJ use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  place lower limits on M_{{TT}}() (equivalent to their M_{{S}}). This updates the results of  SIRUNYAN 2018DU.


pdgid: S071GEX
text:
SIRUNYAN 2021N use 137 (140) fb**-1 of data from p p collisions at sqrt(s) = 13 TeV  in the dielectron (dimuon) channels to place a lower limit on Lambda_{{T}}, here converted to  M_{{TT}}. Bounds on individual channels can be found in their Table 7.


pdgid: S071GEX
text:
SIRUNYAN 2019AC use 35.9 (36.3) fb**-1 of data from p p collisions at sqrt(s) = 13  TeV in the dielectron (dimuon) channels to place a lower limit on Lambda_{{T}}, here converted to  M_{{TT}}. The dielectron and dimuon channels are combined with previous results in the diphoton  channel to set the best limit. Bounds on individual channels and different priors can be found in  their Table 2. This updates the results in KHACHATRYAN 2015AE.


pdgid: S071GEX
text:
AABOUD 2017AP use 36.7 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  place lower limits on M_{{TT}}() (equivalent to their M_{{S}}). This updates the results of AAD 2013AS.


pdgid: S071GEX
text:
AAD 2014BE use 20 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV in the dilepton channel to place lower limits on M_{{TT}}() (equivalent to their M_{{S}}).


pdgid: S071GEX
text:
AAD 2013E use 4.9 and 5.0 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV in the dielectron  and dimuon channels, respectively, to place lower limits on M_{{TT}}() (equivalent to their M_{{S}}). The dielectron  and dimuon channels are combined with previous results in the diphoton channel to set the best limit. Bounds on individual channels and different priors can be found in their Table VIII.


pdgid: S071GEX
text:
BAAK 2012 use electroweak precision observables to place bounds on the ratio Lambda_{{T}}/M_{{D}} as a function of M_{{D}}.  See their Fig. 22 for constraints with a Higgs mass of 120 GeV.


pdgid: S071GEX
text:
AARON 2011C search for deviations in the differential cross section of e()+- p --> e()+- X in 446 pb**-1 of data  taken at sqrt(s) = 301 and 319 GeV to place a bound on M_{{TT}}.


pdgid: S071GEX
text:
ABAZOV 2009AE use dijet angular distributions in 0.7 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to place lower bounds on Lambda(T) (equivalent to their M(S)), here converted to M(TT).


pdgid: S071GEX
text:
ABAZOV 2009D use 1.05 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to place lower bounds on Lambda_{{T}} (equivalent to their M_{{s}}), here converted to M_{{TT}}.


pdgid: S071GEX
text:
SCHAEL 2007A use e+ e- collisions at sqrt(s) = 189 -- 209 GeV to place lower  limits on Lambda_{{T}}, here converted to limits on M_{{TT}}.


pdgid: S071GEX
text:
ABDALLAH 2006C use e+ e- collisions at sqrt(s)~130 -- 207 GeV to place lower limits on M_{{TT}}, which is equivalent to their definition of M_{{s}}. Bound shown includes all  possible final state leptons, lepton = e, mu, tau. Bounds on individual leptonic final  states can be found in their Table 31.


pdgid: S071GEX
text:
GERDES 2006 use 100 to 110 pb**-1 of data from p pbar collisions at sqrt(s) = 1.8 TeV, as recorded by the CDF Collaboration during Run I of the Tevatron. Bound shown includes a K-factor  of 1.3. Bounds on individual e+ e- and gamma gamma final states are found in their Table I.


pdgid: S071GEX
text:
ABAZOV 2005V use 246 pb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV  to search for deviations in the differential cross section to mu+ mu- from graviton exchange.


pdgid: S071GEX
text:
CHEKANOV 2004B search for deviations in the differential cross section of e+- p --> e+- X with 130~pb^{-1} of combined data and Q^2 values up to 40,000~GeV**2 to place a bound on M(TT).


pdgid: S071GEX
text:
ABBIENDI 2003D use e+ e- collisions at sqrt(s)=181 -- 209 GeV to place bounds on the ultraviolet scale M(TT), which is equivalent to their definition of M(s).


pdgid: S071GEX
text:
ACHARD 2003D look for deviations in the cross section for e+ e- --> Z Z from sqrt(s) = 200 -- 209 GeV to place a bound on M(TT).


pdgid: S071GEX
text:
ADLOFF 2003 search for deviations in the differential cross section of e+- p --> e+- X at sqrt(s)=301 and 319 GeV to place bounds on M(TT).


pdgid: S071GEX
text:
HEISTER 2003C use e+ e- collisions at sqrt(s)= 189 -- 209 GeV to place bounds on the scale of dim-8 gravitational interactions.  Their M(s)**+- is equivalent to our M(TT) with lambda=+-1.


pdgid: S071GEX
text:
ACHARD 2002 search for s-channel graviton exchange effects in e+ e- --> gamma gamma at Ecm = 192 -- 209 GeV.


pdgid: S071GEX
text:
ABBOTT 2001 search for variations in differential cross sections to e+ e- and gamma gamma final states at the Tevatron.


pdgid: S071GEX
text:
ABREU 2000A search for s-channel graviton exchange effects in e+ e- --> gamma gamma at Ecm= 189 -- 202 GeV.


pdgid: S071GEX
text:
ABREU 2000S uses e+ e- collisions at sqrt(s)=183 and 189 GeV. Bounds on mu and tau individual final states given in paper.


pdgid: S071GEX
text:
CHANG 2000B derive 3sigma limit on M(TT) of (28,19,15) TeV for delta=(2,4,6) respectively assuming the presence of a torsional coupling in the gravitational action. Highly model dependent.


pdgid: S071GEX
text:
CHEUNG 2000 obtains limits from anomalous diphoton production at OPAL due to graviton exchange. Original limit for delta=4.  However, unknown UV theory renders deltadependence unreliable. Original paper works in HLZ convention.


pdgid: S071GEX
text:
GRAESSER 2000 obtains a bound from graviton contributions to g-2 of the muon through loops of 0.29 TeV for delta=2 and 0.38 TeV for delta=4,6.  Limits scale as lambda**1/2. However calculational scheme not well-defined without specification of high-scale theory. See the ``Extra Dimensions Review.''


pdgid: S071GEX
text:
HAN 2000 calculates corrections to gauge boson self-energies from KK graviton loops and constrain them using S and T. Bounds on M(TT) range from 0.5 TeV (delta=6) to 1.1 TeV (delta=2); see text. Limits have strong dependence, lambda**delta+2, on unknown lambda coefficient.


pdgid: S071GEX
text:
MATHEWS 2000 search for evidence of graviton exchange in CDF and D0 dijet production data.  See their Table2 for slightly stronger delta-dependent bounds.  Limits expressed in terms of Mtilde(S)**4 = M(TT)**4/8.


pdgid: S071GEX
text:
MELE 2000 obtains bound from KK graviton contributions to e+ e- --> V V (V=gamma,W,Z) at LEP. Authors use Hewett conventions.


pdgid: S071GEX
text:
ABBIENDI 1999P search for s-channel graviton exchange effects in e+ e- --> gamma gamma at Ecm=189 GeV.  The limits G(+)>660 GeV  and G(-)>634 GeV are obtained from combined Ecm=183 and 189 GeV data, where G(+-) is a scale related to the fundamental gravity scale.


pdgid: S071GEX
text:
ACCIARRI 1999M search for the reaction e+ e- --> gamma G and s-channel graviton exchange effects in e+ e- --> gamma gamma, W+ W-, Z Z, e+ e-, mu+ mu-, tau+ tau-, q qbar at Ecm=183 GeV.  Limits on the gravity scale are listed in their Tables1 and 2.


pdgid: S071GEX
text:
ACCIARRI 1999s search for the reaction e+ e- --> Z G and s-channel graviton exchange effects in e+ e- --> gamma gamma, W+ W-, Z Z, e+ e-, mu+ mu-, tau+ tau-, q qbar at Ecm=189 GeV.  Limits on the gravity scale are listed in their Tables1 and 2.


pdgid: S071GEX
text:
BOURILKOV 1999 performs global analysis of LEP data on e+ e- collisions at sqrt(s)=183 and 189 GeV. Bound is on Lambda(T).


pdgid: S071KK
text:
AAD 2012CC use 4.9 and 5.0 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV in the dielectron and dimuon  channels, respectively, to place a lower bound on the mass of the lightest KK Z/gamma boson  (equivalent to 1/R = M_{{c}}). The limit quoted here assumes a flat prior corresponding to when the pure Z/gamma KK cross section term dominates. See their Section 15 for more details.


pdgid: S071KK
text:
BARBIERI 2004 use electroweak precision observables to  place a lower bound on the compactification scale 1/R. Both the gauge bosons and the Higgs boson are assumed to propagate in the bulk.


pdgid: S071KK
text:
FLORES 2023 use a number of 13 TeV Run 2 searches at the LHC to place constraints on the    compactification scale 1/R and cutoff scale Lambda in the minimal universal extra   dimension model    with Standard Model fields propagating in the bulk (see their Fig.6).


pdgid: S071KK
text:
AVNISH 2021 perform a study on the ATLAS collaboration search for multiple jets plus missing  transverse energy from p p collisions at sqrt(s) = 13 TeV and integrated luminosity of 139  fb**-1, to place constraints on the compactification scale and cutoff scale Lambda in  universal extra dimension models with Standard Model fields propagating in the bulk.


pdgid: S071KK
text:
AABOUD 2018AV use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV in  final states with multiple b-jets, to place a lower bound on the compactification scale in a model  with two universal extra dimensions. Assuming the radii of the two extra dimensions are equal, a  lower limit of 1.8 TeV for the Kaluza-Klein mass is obtained.


pdgid: S071KK
text:
AABOUD 2018CE use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV in  final states with same-charge leptons and b-jets, to place a lower bound on the compactification  scale in a model with two universal extra dimensions. Assuming the radii of the two extra  dimensions are equal, a lower limit of 1.45 TeV for the Kaluza-Klein mass is obtained.


pdgid: S071KK
text:
ACCOMANDO 2015 use electroweak precision observables to place a lower bound on the compactification scale 1/R.  See their Fig. 2 for the bound as a function of   sin(beta),  which parametrizes the VEV contribution from brane and bulk Higgs fields.  The   quoted value is for  the minimum bound which occurs at sin(beta) = 0.45.


pdgid: S071KK
text:
KHACHATRYAN 2015T use 19.7 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV  to place a lower bound on the compactification  scale 1/R.


pdgid: S071KK
text:
CHATRCHYAN 2013AQ use 5.0 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV  and a  further 3.7 fb**-1 of data at sqrt(s) = 8 TeV to place a lower bound on the compactification  scale 1/R,  in models with universal extra dimensions and Standard Model fields  propagating in the bulk.  See  their Fig. 5 for the bound  as a function of the universal bulk fermion mass parameter mu.


pdgid: S071KK
text:
CHATRCHYAN 2013W use diphoton events with large missing transverse momentum in 4.93 fb**-1 of data produced from p p collisions at sqrt(s) = 7 TeV to place a lower bound on the compactification scale in a universal extra dimension model  with gravitational decays. The bound assumes that the cutoff scale Lambda, for the radiative corrections  to the Kaluza-Klein  masses, satisfies Lambda/M_{{c}} = 20. The model parameters are chosen such that the decay gamma^* --> G gamma occurs with an appreciable branching fraction.


pdgid: S071KK
text:
EDELHAUSER 2013 use 19.6 and 20.6 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV analyzed by the CMS Collaboration in the dielectron and dimuon  channels, respectively, to place a lower bound on the mass of  the second lightest Kaluza-Klein Z/gamma boson (converted  to a limit on 1/R = M_{{c}}). The  bound assumes Standard Model fields propagating in the bulk and that the cutoff scale Lambda, for the radiative corrections  to the Kaluza-Klein  masses, satisfies  Lambda/M_{{c}} = 20.


pdgid: S071KK
text:
AAD 2012CP use diphoton events with large missing transverse momentum in 4.8 fb**-1 of data produced from p p collisions at sqrt(s) = 7 TeV to place a lower bound on the compactification scale in a universal extra dimension model  with gravitational decays. The bound assumes that the cutoff scale Lambda, for the radiative corrections  to the Kaluza-Klein masses, satisfies Lambda/M_{{c}} = 20. The model parameters are chosen such that the decay gamma^* --> G gamma occurs with an appreciable branching fraction.


pdgid: S071KK
text:
AAD 2012X use diphoton events with large missing transverse momentum in 1.07 fb**-1 of data produced from p p collisions at sqrt(s) = 7 TeV to place a lower bound on the compactification scale in a universal extra dimension model with gravitational decays. The bound assumes that the cutoff scale Lambda, for the radiative corrections to the Kaluza-Klein  masses, satisfies Lambda/M_{{c}} = 20. The model parameters are chosen such that the decay gamma^* --> G gamma  occurs with an appreciable branching fraction.


pdgid: S071KK
text:
ABAZOV 2012M use same-sign dimuon events in 7.3 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV  to place a lower bound on the compactification scale 1/R, in models with universal extra dimensions where  all Standard Model fields propagate in the bulk.


pdgid: S071KK
text:
BAAK 2012 use electroweak precision observables to place a lower bound on the compactification scale 1/R,  in models with universal extra dimensions and Standard Model fields propagating in the bulk. Bound assumes a 125 GeV Higgs mass. See their Fig. 25 for the bound as a function of the Higgs mass.


pdgid: S071KK
text:
FLACKE 2012 use electroweak precision observables to place a lower bound on the compactification scale 1/R,  in models with universal extra dimensions and Standard Model fields propagating in the bulk.  See their Fig. 1 for the bound  as a function of the universal bulk fermion mass parameter mu.


pdgid: S071KK
text:
NISHIWAKI 2012 use up to 2 fb**-1 of data from the ATLAS and CMS experiments that constrains the production cross section of a Higgs-like particle to place a lower bound on the compactification scale 1/R in universal extra dimension models.  The quoted bound assumes Standard Model fields propagating in the bulk and a 125 GeV Higgs mass. See their Fig. 1 for the bound  as a function of the Higgs mass.


pdgid: S071KK
text:
AAD 2011F use diphoton events with large missing transverse energy in 3.1 pb**-1 of data produced from p p  collisions at sqrt(s) = 7 TeV to place a lower bound on the compactification scale in a universal extra dimension model with gravitational decays. The bound assumes that the cutoff scale Lambda, for the radiative corrections to the Kaluza-Klein  masses, satisfies Lambda/M(c) = 20. The model parameters are chosen such that the decay gamma^*() --> G gamma  occurs with an appreciable branching fraction.


pdgid: S071KK
text:
AAD 2011X use diphoton events with large missing transverse energy in 36 pb**-1 of data produced from p p collisions at sqrt(s) = 7 TeV to place a lower bound on the compactification scale in a universal extra dimension model with gravitational decays. The bound assumes that the cutoff scale Lambda, for the radiative corrections to the Kaluza-Klein masses, satisfies Lambda/M_{{c}} = 20. The model parameters are chosen such that the decay gamma^*() --> G gamma occurs with an appreciable  branching fraction.


pdgid: S071KK
text:
ABAZOV 2010P use diphoton events with large missing transverse energy in 6.3 fb**-1 of data produced  from p pbar collisions at sqrt(s) = 1.96 TeV to place a lower bound on the compactification scale in a universal extra dimension model with gravitational decays. The bound assumes that the cutoff scale Lambda, for the radiative corrections to the Kaluza-Klein masses, satisfies Lambda/M(c)=20. The model parameters are chosen such that the decay gamma^*() --> G gamma occurs with an appreciable branching fraction.


pdgid: S071KK
text:
ABAZOV 2009AE use dijet angular distributions in 0.7 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to place a lower bound on the compactification scale.


pdgid: S071KK
text:
HAISCH 2007 use inclusive Bbar-meson decays to place a Higgs mass independent bound  on the compactification scale 1/R in the minimal universal extra dimension model.


pdgid: S071KK
text:
GOGOLADZE 2006 use electroweak precision observables to place a lower bound on the compactification scale in models with universal extra dimensions. Bound assumes a 115 GeV Higgs mass. See their Fig. 3 for the bound as a function of the Higgs mass.


pdgid: S071KK
text:
CORNET 2000 translates a bound on the coefficient of the 4-fermion operator (leptonbar gamma_mu tau^a lepton)(leptonbar gamma^mu tau^a lepton) derived by Hagiwara and Matsumoto into a limit on the mass scale of KK Wbosons.


pdgid: S071KK
text:
RIZZO 2000 obtains limits from global electroweak fits in models with a Higgs in the bulk (3.8 TeV) or on the standard brane (3.3 TeV).


pdgid: S071RSG
text:
SIRUNYAN 2021N use 137 (140) fb**-1 of data from p p collisions at sqrt(s) = 13 TeV  to search for dilepton resonances in the dielectron (dimuon) channel. See Table 6 for other limits  with warp parameter values k/Mbar_{{P}} = 0.01 and 0.05. This updates the results of  SIRUNYAN 2018BB.


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HAYRAPETYAN 2024AE use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the b bbar W W final state. See their Figure 19 for  limits on the cross section times branching fraction as a function of the KK graviton mass for  k/Mbar_{{P}} = 0.3, 0.5 and 1.


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HAYRAPETYAN 2024AJ use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV,  in the diphoton channel to place a lower limit on the mass of the lightest KK graviton. See their  paper for limits with other warp parameter values k/Mbar_{{P}} = 0.01 and 0.2. This  updates the results of SIRUNYAN 2018DU.


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TUMASYAN 2024B use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the gamma gamma b bbar final state. See their Figure  6 for limits on the cross section times branching fraction as a function of the KK graviton mass  assuming k/Mbar_{{P}} = 0.5 and 1. This updates the result of SIRUNYAN 2019.


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TUMASYAN 2023AP use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for W W , Z Z diboson resonances in q qbar q qbar final states. See their Figure 7  for the limit on the cross section times branching fraction as a function of the KK graviton mass.  Assuming k/Mbar_{{P}} = 0.5, a graviton mass is excluded below 1400 GeV. This updates the  result of SIRUNYAN 2020Q.


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AAD 2022F use 126 -- 139 fb**-1 of data from p p collisions at sqrt(s) = 13  TeV to search for Higgs boson pair production in the b bbar b bbar final state. See their  Figure 14 for limits on the cross section times branching fraction as a function of the KK graviton  mass. Assuming k/Mbar_{{P}} = 1, gravitons in the mass range 298 -- 1460 GeV are  excluded. This updates the results of AABOUD 2019A.


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TUMASYAN 2022D use 137 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for W W resonances in lepton nu q q final states (lepton = e, mu). See  their Figure 6 for the limit on the KK graviton mass as a function of the cross section times  branching fraction, including theoretical values for k/Mbar_{{P}} = 0.5. This updates the  results of SIRUNYAN 2018AX.


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TUMASYAN 2022J use 137 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Z Z resonances in the nu nubar q qbar final state. See their Figure 10 for the  limit on the KK graviton mass as a function of the cross section times branching fraction, assuming  k/Mbar_{{P}} = 0.5 . This updates the result of SIRUNYAN 2018BK.


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TUMASYAN 2022R use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Z Z resonances in 2 lepton 2 q final states (lepton = e, mu). See  their Figure 8 for the limit on the KK graviton mass as a function of the cross section times  branching fraction. Assuming k/Mbar_{{P}} = 0.5, a graviton mass is excluded below 1200  GeV. This updates the result of SIRUNYAN 2018DJ.


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TUMASYAN 2022U use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to   search for Higgs boson pair production in the b bbar q qbar^' lepton nu, b bbar lepton nu lepton nu   and b bbar lepton nu nu lepton nu nu final states (lepton = e, mu). See their   Figure 7 for limits on the cross section times branching fraction as a function of the KK graviton   mass, including theoretical values for k/Mbar_{{P}} = 0.3 and 0.5. This updates the   results of SIRUNYAN 2019CF and SIRUNYAN 2018F.


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AAD 2021AF use 139 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to search  for Z Z resonances in the lepton lepton lepton lepton and lepton lepton nu nubar final  states (lepton=e, mu). See their Figure 8 for the limit on the cross section times  branching fraction as a function of the KK graviton mass, including theoretical values for  k/Mbar_{{P}} = 1. This updates the results of AAD 2015AU and AABOUD 2018BF.


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AAD 2021AY use 139 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV in the  diphoton channel to place a lower limit on the mass of the lightest KK graviton. This updates the  results of AABOUD 2017AP.


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AAD 2020AT use 139 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to search  for diboson resonances in semileptonic final states (lepton nu q q,lepton lepton q q, nu nu q q).  See their Figure 15 for the limit on the cross section times branching fraction as a function of  the KK graviton mass. Lower limits on the graviton mass are also given for k/Mbar_{{P}} =  1. This updates the results of AABOUD 2018AK and AABOUD 2018AL.


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AAD 2020C use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to search  for Higgs boson pair production in the b bbar b bbar, b bbar W+ W-, and b bbar tau+ tau- final  states. See their Figure 5(b)(c) for limits on the cross section as a function of the KK graviton  mass. In the case of k/Mbar_{{P}} = 1 and 2, gravitons are excluded in the mass range  260 -- 3000 GeV and 260 -- 1760 GeV, respectively.


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AAD 2020T use 139 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to search  for narrow resonances decaying to bottom quark pairs. See their Figure 7 for the limit on the  product of the cross section, branching fraction, acceptance and b-tagging efficiency as a  function of the KK graviton mass. In the case of k/Mbar_{{P}} = 0.2, KK gravitons in the  mass range 1.25 -- 2.8 TeV are excluded.


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SIRUNYAN 2020AI use 137 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for dijet resonances. See their Figure 6 for the limit on the product of the cross section,  branching fraction and acceptance as a function of the KK graviton mass. This updates the results  of SIRUNYAN 2018BO.


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SIRUNYAN 2020F use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the b bbar Z Z final state. See their Figure 4 for  limits on the cross section times branching fraction as a function of the KK graviton mass, and  Figure 5 for limits as a function of k/Mbar_{{P}}.


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AABOUD 2019O use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the b bbar W W final state. See their Figure 12 for  limits on the cross section times branching fraction as a function of the KK graviton mass for  k/Mbar_{{P}} = 1 and k/Mbar_{{P}} = 2.


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AAD 2019D use 139 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to search  for diboson resonances in the all-hadronic final state. See their Figure 9(b) for the limit on the  cross section times branching fraction as a function of the KK graviton mass, including theoretical  values for k/Mbar_{{P}} = 1. This updates the results of AABOUD 2018F.


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SIRUNYAN 2019BE use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production by combining the results from four final states: b bbar gamma gamma, b bbar tau taubar, b bbar b bbar, and  b bbar V V. See their Figure 7 for limits on the cross section times branching fraction as a  function of the KK graviton mass.


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AABOUD 2018BI use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for top-quark pairs decaying into the lepton-plus jets topology. See their Figure 16 for the  limit on the KK graviton mass as a function of the cross section times branching fraction,  including theoretical values for k/Mbar_{{P}} = 1.


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AABOUD 2018CJ combine the searches for heavy resonances decaying into bosonic and leptonic  final states from 36.1 fb**-1 of p p collision data at sqrt(s) = 13 TeV. The lower limit  on the KK graviton mass, with k/Mbar_{{P}} = 1, is 2.3 TeV.


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AABOUD 2018CQ use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the b bbar tau+ tau- final state. See their Figure 2  for limits on the cross section times branching fraction as a function of the KK graviton mass.  Assuming k/Mbar_{{P}} = 1, gravitons in the mass range 325 -- 885 GeV are excluded.


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AABOUD 2018CW use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the gamma gamma b bbar final state. See their Figure  7 for limits on the cross section times branching fraction as a function of the KK graviton mass.


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SIRUNYAN 2018AF use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the b bbar b bbar final state. See their Figure 9 for  limits on the cross section times branching fraction as a function of the KK graviton mass,  including theoretical values for k/Mbar_{{P}} = 0.5. This updates the results of  KHACHATRYAN 2015R.


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SIRUNYAN 2018AS use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Z Z resonances in the lepton lepton nu nubar final state (lepton=e,  mu). See their Figure 5 for the limit on the KK graviton mass as a function of the cross  section times branching fraction, including theoretical values for k/Mbar_{{P}} = 0.1,  0.5, and 1.0.


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SIRUNYAN 2018CW use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for Higgs boson pair production in the b bbar b bbar final state. See their Figure 8 for  limits on the cross section times branching fraction as a function of the KK graviton mass,  including theoretical values for k/Mbar_{{P}} = 0.5.


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SIRUNYAN 2018I use 19.7 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV to  search for narrow resonances decaying to bottom quark pairs. See their Figure 3 for the limit on  the KK graviton mass as a function of the cross section times branching fraction in the mass range  of 325 -- 1200 GeV.


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AAD 2016R use 20.3 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV to place a  lower bound on the mass of the lightest KK graviton. See their Figure 4 for the limit on the KK  graviton mass as a function of the cross section times branching fraction.


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AAD 2015AZ use 20.3 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV to place a  lower bound on the mass of the lightest KK graviton.  See their Figure 2 for limits on the KK graviton mass as a function of the cross section times  branching ratio.


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AAD 2015CP use 20.3 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV to place a  lower bound on the mass of the lightest KK graviton.  See their Figures 6b and 6c for the limit on the KK graviton mass as a function of the cross  section times branching fraction.


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AAD 2014V use 20.3 (20.5) fb**-1 of data from p p collisions at sqrt(s) = 8 TeV in  the dielectron (dimuon) channels to place a lower bound on the mass of the lightest KK graviton.  This updates the results of AAD 2012CC .


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AAD 2013A use 4.7 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV in the lepton nu lepton nu channel,  to place a lower bound on the mass of the lightest KK graviton.


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AAD 2013AO use 4.7 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV in the  lepton nu j j channel, to place a lower bound on the mass of the lightest KK graviton.


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AAD 2013AS use 4.9 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV in the diphoton channel to place lower limits on the mass of the lightest KK graviton. The diphoton channel is combined with previous results in the dielectron and  dimuon channels to set the best limit. See their Table 2 for warp parameter values k/Mbar_{{P}} between 0.01 and 0.1. This updates the results of AAD 2012Y .


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AAD 2012AD use 1.02 fb**-1 of data from p p collisions at sqrt(s) = 7 TeV to search for KK gravitons in a warped extra dimension decaying to Z Z dibosons in the l l j j and l l l l channels (lepton=e, mu). The limit is quoted for the combined l l j j + l l l l channels. See their Figure 5 for limits on the cross section CS(G --> Z Z) as a function of the graviton mass.


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AALTONEN 2012V use 6 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in a warped extra dimension decaying to Z Z dibosons in the l l j j and l l l l channels (lepton=e, mu). It provides improved limits over the previous analysis in AALTONEN 2011G. See their Figure 16 for limits from all  channels combined on the cross section times branching ratio CS(p pbar --> G^* --> Z Z) as a function of the graviton mass.


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BAAK 2012 use electroweak precision observables to place a lower bound on the compactification scale  k e**-pi k R, assuming Standard Model fields propagate in the bulk and the Higgs is confined to the IR brane. See their Fig. 27 for more details.


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AALTONEN 2011G use 2.5 -- 2.9 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to search  for KK gravitons in a warped extra dimension decaying to Z Z dibosons via the e e e e, e e mu mu, mu mu mu mu, e e j j, and mu mu j j channels. See their Fig. 20 for limits on the cross section  CS(G --> Z Z) as a function of the graviton mass.


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AALTONEN 2011R uses 5.7 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV in the dielectron channel to place a lower bound on the mass of the lightest graviton. It provides combined limits with the diphoton channel analysis  of AALTONEN 2011U. For warp parameter values k/Mbar_{{P}} between 0.01 to 0.1 the lower limit on the mass  of the lightest graviton is between 612 and 1058 GeV. See their Table I for more details.


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ABAZOV 2011H use 5.4 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96  TeV to place a lower bound on the mass of the lightest graviton. Their 95% C.L. exclusion limit does not include masses less than 300 GeV.


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AALTONEN 2010N use 2.9 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to place a lower bound on the mass of the lightest graviton.


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ABAZOV 2010F use 5.4 fb**-1 of data from p pbar collisions at sqrt(s) = 1.96 TeV to place a lower bound on the mass of the lightest graviton. For warp parameter values of  k/Mbar_{{P}} between 0.01 and 0.1 the lower limit on the mass of the lightest graviton is between 560 and 1050 GeV. See their Fig. 3 for more details.


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AALTONEN 2008S use p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to four electrons via two Z bosons using 1.1 fb**-1 of data. See their Fig. 8 for limits on sigma.B(G --> Z Z) versus the graviton mass.


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ABAZOV 2008J use p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to electrons and photons using 1 fb**-1 of data. For warp parameter values of k/Mbar_{{P}} between 0.01 and 0.1 the lower limit on the mass of the lightest excitation is between 300 and 900 GeV. See their Fig. 4 for more details.


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AALTONEN 2007G use p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in warped extra  dimensions. They search for graviton resonances decaying to photons using 1.2 fb**-1 of data.  For warp parameter values of k/Mbar_{{P}} = 0.1, 0.05, and 0.01 the bounds on the graviton  mass are 850, 694, and 230 GeV, respectively. See their Fig. 3 for more details. See also AALTONEN 2007H.


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AALTONEN 2007H use p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in warped extra  dimensions. They search for graviton resonances decaying to electrons using 1.3 fb**-1 of data.  For a warp parameter value of k/Mbar_{{P}} = 0.1 the bound on the graviton mass is 807 GeV.  See their Fig. 4 for more details. A combined analysis with the diphoton data of AALTONEN 2007G yields for k/Mbar_{{P}} = 0.1 a graviton mass lower bound of 889 GeV.


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ABAZOV 2005N use p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to muons, electrons or photons, using 260~pb**-1 of data. For warp parameter values of k/Mbar_{{P}} = 0.1, 0.05, and 0.01, the bounds on the graviton mass are 785, 650 and 250GeV respectively. See their Fig.3 for more details.


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ABULENCIA 2005A use p pbar collisions at sqrt(s) = 1.96 TeV to search for KK gravitons in warped extra dimensions. They search for graviton resonances decaying to muons or electrons, using 200~pb**-1 of data. For warp parameter values of k/Mbar_{{P}} = 0.1, 0.05, and 0.01, the bounds on the graviton mass are 710, 510 and 170 GeV respectively.


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AABOUD 2018BI use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV. This  result updates AAD 2013AQ.


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HAYRAPETYAN 2024G use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  place limits on a KK gluon decaying to gluons via a spin-0 radion, R. See their Figure 3 for  limits on the cross section times branching fraction as a function of the KK gluon mass and various  values of the radion mass. This updates the results of TUMASYAN 2022C.


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AABOUD 2019AS use 36.1 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV. An  upper bound of 3.4 TeV is placed on the KK gluon mass for Gamma/m = 30%.


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SIRUNYAN 2019AL use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  place limits on a KK gluon decaying to a top quark and a heavy vector-like fermion, T. KK gluon  masses between 1.5 and 2.3 TeV and between 2.0 and 2.4 TeV are excluded for T masses of 1.2 and 1.5  TeV, respectively.


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CHATRCHYAN 2013BM use 19.7 fb**-1 of data from p p collisions at sqrt(s) = 8 TeV. Bound is for a width of approximately 15 -- 20% of the KK gluon mass.


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CHEN 2013A place limits on the KK mass scale for a specific warped model with custodial symmetry  and bulk fermions. See their Figures 4 and 5.


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SIRUNYAN 2018DA use 35.9 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to  search for semiclassical black holes decaying to multijet final states. No excess of events above  the expected level of standard model background was observed. Exclusions at 95% CL are set on  the mass threshold for black hole production as a function of the higher-dimensional Planck scale  for rotating and nonrotating black holes under several model assumptions (ADD, 2, 4, 6 extra  dimensions model) in the 7.1 -- 10.3 TeV range. These limits supersede those in SIRUNYAN 2017CP.


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AAD 2016N use 3.6 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to search  for semiclassical black hole decays to multijet final states. No excess of events above the  expected level of Standard Model background was observed. Exclusion contours at 95% C.L. are  set on the mass threshold for black hole production versus higher-dimensional Planck scale for  rotating black holes (ADD, 6 extra dimensions model).


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AAD 2016O use 3.2 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to search  for semiclassical black hole decays to high-mass final states with leptons and jets.  No excess of  events above the expected level of Standard Model background was observed. Exclusion contours at  95% C.L. are set on the mass threshold for black hole production versus higher-dimensional  Planck scale for rotating black holes (ADD, 2 to 6 extra dimensions).


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AAD 2013AW use 20.3 fb^{-1} of data from p p collisions at sqrt(s) = 8 TeV to search  for semiclassical black hole decays to like-sign dimuon final states using large track  multiplicity. No excess of events above the expected level of Standard Model background was  observed. Exclusion contours at 95% C.L. are set on the mass threshold for black hole  production versus higher-dimensional Planck scale in various extra dimensions, rotating and  non-rotating models.


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AAD 2024S use 140 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to search  for quantum black hole decays to final states with high-invariant-mass lepton + jet. No excess of  events above the expected level of Standard Model background was observed. Exclusion limits at  95% C.L. are set on mass thresholds for black hole production in an ADD (6 extra dimensions)  model and the Randall-Sundrum (one extra dimension) model. The resulting lower mass threshold  limits in the ADD (RS) models are 9.2 (6.8) TeV. The ADD limit supersedes that in AAD 2014AL.


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AAD 2023CB use 139 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to search  for quantum black hole decays with different-flavor high-mass dilepton final states. No excess of  events above the expected level of Standard Model background was observed. Exclusion limits at  95% C.L. are set on mass thresholds for black hole production in ADD (6 extra dimensions) and  RS1 models. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale,  mass thresholds below 5.9 (3.8), 5.2 (3.0), and 5.1 (3.0) TeV are excluded in the e mu, e tau and  mu tau channels for the ADD (RS1) models, respectively. These limits supersede those in  AABOUD 2018CM.


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TUMASYAN 2023AW use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for quantum black hole decays in the tau lepton plus missing transverse momentum final  state. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale,  threshold masses below 6.6 TeV are excluded in the ADD model with four extra dimensions (see their  Figure 8).


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TUMASYAN 2023BC use 138 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for quantum black hole decays to final states with a photon and a jet. No excess of events  above the expected level of Standard Model background was observed. Exclusion limits at 95%  C.L. are set on mass thresholds for black hole production in ADD (6 extra dimensions) and RS1  models. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale,  mass thresholds below 7.5 TeV and 5.2 TeV are excluded for the ADD and RS1 models, respectively  (see their Figure 9).


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TUMASYAN 2023H use 138 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to    search for quantum black hole decays with different-flavor high-mass dilepton final states. No    excess of events above the expected level of Standard Model background was observed. Exclusion    limits at 95% C.L. are set on mass thresholds for black hole production in the ADD model  (with 4 extra dimensions). Assuming the black hole mass threshold is equal to the  higher-dimensional   Planck scale, mass thresholds below 5.6, 5.2, and 5.0 TeV are excluded in the  e mu, e tau   and mu tau channels, respectively.


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AAD 2020T use 139 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to search  for quantum black hole decays to final states with dijets. No excess of events above the expected  level of Standard Model background was observed. Exclusion limits at 95% C.L. are set on mass  thresholds for black hole production in an ADD (6 extra dimensions) model. Assuming the black hole  mass threshold is equal to the higher-dimensional Planck scale, mass thresholds below 9.4 TeV are  excluded. This limit supersedes AABOUD 2017AK.


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AABOUD 2018BA use 36.7 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for quantum black hole decays to final states with a photon and a jet. No excess of events  above the expected level of Standard Model background was observed. Exclusion limits at 95%  C.L. are set on mass thresholds for black hole production in ADD (6 extra dimensions) and RS1  models. Assuming the black hole mass threshold is equal to the Planck scale, mass thresholds below  7.1 TeV and 4.4 TeV are excluded for the ADD and RS1 models, respectively. These limits supersede  those in AAD 2016AI.


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SIRUNYAN 2018AT use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for quantum black hole decays to e mu final states. In Figure 4, lower mass limits of  5.3, 5.5 and 5.6 TeV are placed in a model with 4, 5 and 6 extra dimensions, respectively, and a  lower mass limit of 3.6 TeV is found for a single warped dimension.


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SIRUNYAN 2018DD use 35.9 fb**-1 of data from p p collisions at sqrt(s) = 13 TeV to  search for quantum black hole decays in dijet angular distributions. A lower mass limit of 5.9  (8.2) TeV is placed in the RS (ADD) model with one (six) extra dimension(s).


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SIRUNYAN 2017CP use 2.3 fb^{-1} of data from p p collisions at sqrt(s) = 13 TeV to  search for quantum black holes decaying to dijet final states. No excess of events above the  expected level of standard model background was observed. Limits on the quantum black hole mass  threshold are set as a function of the higher-dimensional Planck scale, under the assumption that  the mass threshold must exceed the above Planck scale. Depending on the model, mass thresholds in  the range up to 5.1 -- 9.0 TeV are excluded.


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KHACHATRYAN 2016BE use 19.7 fb^{-1} of data from p p collisions at sqrt(s) = 8 TeV to  search for quantum black holes undergoing lepton flavor violating decay to the e mu final  state. No excess of events above the expected level of standard model background was observed.  Exclusion limits at 95% CL are set on mass thresholds for black hole production in the ADD  (2 -- 6 flat extra dimensions), RS1 (1 warped extra dimension), and a model with a Planck  scale at the TeV scale from a renormalization of the gravitational constant (no extra dimensions).  Limits on the black hole mass threshold are set assuming that it is equal to the higher-dimensional  Planck scale. Mass thresholds for quantum black holes in the range up to 3.15 -- 3.63 TeV  are excluded in the ADD model. In the RS1 model, mass thresholds below 2.81 TeV are excluded in the  PDG convention for the Schwarzschild radius. In the model with no extra dimensions, mass thresholds  below 1.99 TeV are excluded.


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KHACHATRYAN 2015V use 19.7 fb^{-1} of data from p p collisions at sqrt(s) = 8 TeV to  search for quantum black holes decaying to dijet final states. No excess of events above the  expected level of standard model background was observed. Exclusion limits at 95% CL are set  on mass thresholds for black hole production in the ADD (2 -- 6 flat extra dimensions) and  RS1 (1 warped extra dimension) model. Limits on the black hole mass threshold are set as a function  of the higher-dimensional Planck scale, under the assumption that the mass threshold must exceed  the above Planck scale. Depending on the model, mass thresholds in the range up to 5.0 -- 6.3 TeV are  excluded. This paper supersedes CHATRCHYAN 2013AD.


pdgid: S071BHQ
text:
AAD 2014V use 20.3 (20.5) fb^{-1} of data in the dielectron (dimuon) channels from p p  collisions at sqrt(s) = 8 TeV to search for quantum black hole decays involving high-mass dilepton  resonances. No excess of events above the expected level of Standard Model background was observed.  Exclusion limits at 95% C.L. are set on mass thresholds for black hole production in ADD (6  extra dimensions) and RS1 models. Assuming the black hole mass threshold is equal to the  higher-dimensional Planck scale, mass thresholds below 3.65 TeV and 2.24 TeV are excluded for the  ADD and RS1 models, respectively.


pdgid: S071BHQ
text:
CHATRCHYAN 2013A use 5 fb^{-1} of data from p p collisions at sqrt(s) = 7 TeV to  search for quantum black holes decaying to dijet final states. No excess of events above the  expected level of standard model background was observed. Exclusion limits at 95% CL are set  on mass thresholds for black hole production in the ADD (2 -- 6 flat extra dimensions) and  RS (1 warped extra dimension) model. Limits on the black hole mass threshold are set as a function  of the higher-dimensional Planck scale, under assumption that the mass threshold must exceed the  above Planck scale. Depending on the model, mass thresholds in the range up to 4.0 -- 5.3  TeV are excluded.


pdgid: S030DI5
text:
ANGLOHER 2024 search for spin-independent light WIMP (mass between 0.16 and 6 GeV) scatter on  diamond target. No signal observed. Limits placed in sigma^SI vs mass plane for sub-GeV WIMPs.  Quoted limit is for m(WIMP) = 0.2 GeV.


pdgid: S030DI5
text:
ANGLOHER 2024B search for low mass m(wimp) ~100 MeV. No signal observed. Limits placed  in cross section vs. mass plane. Quoted limit for m(wimp) = 100 MeV.


pdgid: S030DI5
text:
AALBERS 2023A search for e recoil events from GeV scale WIMP scatter on Xe. No  signal observed. Limits placed on 6 different models including sigma^SI < 3E-3 for  m(chi) ~ 1 GeV via Migdal scattering.


pdgid: S030DI5
text:
AGNES 2023 for for light DM via e recoil/Migdal effect. No signal observed.  sigma^SI(chiN) < 4E-7 pb for m(chi) = 3 GeV.


pdgid: S030DI5
text:
AGNES 2023B search for GeV-scale DM scatter on nucleons in Ar. No signal observed.  Limit sigma^SI(chi N) < 6E-7 pb for m(chi) = 3 GeV.


pdgid: S030DI5
text:
ALBAKRY 2023 search for light DM via Migdal effect. No signal observed. Allow sigma^SI  < 0.5 pb for m(chi)=1 GeV (see e.g. Fig. 7).


pdgid: S030DI5
text:
AMBROSONE 2023 derive limits on sigma(chi p) due to possible DM distortion of cosmic  ray spectra in starburst galaxies. Limits placed in sigma vs. mass (E-3 -- 10 MeV)  plane, the most stringent given above being at 1 keV.


pdgid: S030DI5
text:
ANGLOHER 2023 search for light DM using Si target. No signal observed. Require  sigma^SI < 70 pb for m(chi) = 0.3 GeV (see e.g. Fig. 5).


pdgid: S030DI5
text:
LI 2023F searches for SI light DM scatter from Xe. No signal observed. The quoted  limit for m(chi) = 4 GeV.


pdgid: S030DI5
text:
MA 2023A search for GeV-scale DM using PandaX-4T. No signal observed. sigma(chi p)  < 5E-10 pb for m(chi) = 10 GeV.


pdgid: S030DI5
text:
ADHIKARI 2022B search for sub-GeV WIMPs via SI and SD detection; no signal detected; limits  placed in m(chi) vs. sigma plane for m(chi): 0.2 -- 3 GeV; quoted limit is for  m(chi) = 1 GeV.


pdgid: S030DI5
text:
ARMENGAUD 2022 search for GeV-scale DM scatter on Ge at EDELWEISS via Migdal   effect; no signal observed; limits placed in sigma^SI(chi N) vs. m(DM) plane; quoted limit   is for m(DM) = 100 MeV.


pdgid: S030DI5
text:
CUI 2022 search for sub-GeV boosted DM at PandaX-II at CJPL; no signal detected; limits set  in sigma^SI(chi p) vs. m(chi) plane; quoted limit for m(chi) = 0.1 GeV.


pdgid: S030DI5
text:
XU 2022 search for sub-GeV boosted DM in CDEX; no signal observed; limits placed in  CS(chi N) vs. m(DM) plane; quoted limit is for m(DM) = 0.1 GeV.


pdgid: S030DI5
text:
AKERIB 2021A present new technique for low mass WIMP detection. Require sigma^SI(p chi) <  2E-7 pb for m(WIMP) 10 GeV.


pdgid: S030DI5
text:
ALKHATIB 2021 search for light DM using SuperCDMS; require sigma^SI(p chi) <  5E6  for m(DM) = 0.1 GeV.


pdgid: S030DI5
text:
ANDRIAMIRADO 2021A search for upscattered (boosted) sub-GeV DM interacting with proton in  PROSPECT detector. No signal observed. Limits placed in  sigma(chi N) vs. m(DM) plane for  m(DM) ~ 1   keV - 0.5 GeV. The listed limit is for m(DM) = 1 keV.


pdgid: S030DI5
text:
APRILE 2021 search for low recoil energy GeV-scale DM in XENON1T with 1.6 keV threshold. No  signal in 0.6 t y exposure. Limits placed in sigma^SI(chi N) vs. m(DM) plane for m(DM)  between 3 -- 12 GeV. The listed limit is for m(DM) = 5 GeV.


pdgid: S030DI5
text:
AGUILAR-AREVALO 2020C search for WIMP SI scatter on Si using DAMIC at SNOLab; some  excess; limits placed in sigma vs m(DM) for m(DM) in 1.2 -- 10 GeV; quoted limit for  m(WIMP) = 2 GeV.


pdgid: S030DI5
text:
AKERIB 2020A search for GeV-scale WIMPs via WIMP-nucleon scatter with single photon emission;  no signal; limits placed in m(WIMP) vs sigma^SI plane: for example sigma^SI(chi n)  < 8E-4 pb for m(WIMP) = 2.5 GeV.


pdgid: S030DI5
text:
ABDELHAMEED 2019A search for GeV scale dark matter SI scatter on  CaWO(4); no signal, limits placed in sigma vs. mass plane for m(DM) ~  0.1 -- 10 GeV. The listed limit is for m(DM) = 1 GeV.


pdgid: S030DI5
text:
AGNESE 2019A search for 1.5 -- 10 GeV WIMP scatter on Ge in CDMSlite  dataset. Limits set in a likelihood analysis. No signal was observed. Limit reported for m(chi)  = 5 GeV.


pdgid: S030DI5
text:
AKERIB 2019 search for 0.4 -- 5 GeV DM using bremsstrahlung photons and "Migdal"  electrons; 1.4E4 kg d exposure of liquid Xe; constraint sigma^SI(chi N)  < 1 pb for m(chi) = 5 GeV in light scalar mediator model.


pdgid: S030DI5
text:
AMOLE 2019 search for SI WIMP scatter on C(3)F(8) in PICO-60  bubble chamber; no signal: set limit for spin independent coupling sigma^SI(chi N) <  1E-6 pb for m(chi) = 5 GeV.


pdgid: S030DI5
text:
APRILE 2019C search for light DM scatter on Xe via atomic excitation, ionization  (Migdal effect) or bremsstrahlung; no signal, limits placed in sigma vs. m(DM) plane for m(DM)  ~ 0.085 -- 2 GeV. The listed limit is for m(DM) = 1 GeV.


pdgid: S030DI5
text:
APRILE 2019D search for light DM scatter on Xe via ionization to probe SI, SD, and  chi e cross sections; with 22 t d exposure, limits placed in various sigma vs. m(DM)  planes. Quoted limit is for m(DM) = 5 GeV.


pdgid: S030DI5
text:
ARMENGAUD 2019search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 0.045 -- 10 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
KOBAYASHI 2019 search for sub-GeV WIMP annual modulation in Xe via brems; no  signal; limits placed in sigma^SI(chi N) vs. m(chi) plane for m ~ 0.3 -- 1  GeV; quoted limit is for m(chi) = 0.5 GeV.


pdgid: S030DI5
text:
LIU 2019B seach for sub-GeV DM using Migdal effect on Ge at CDEX-IB; no signal,  require sigma^SI(chi N) < 7E2  pb for m(chi) = 0.1 GeV.


pdgid: S030DI5
text:
AGNESE 2018 search for GeV scale WIMPs using CDMSlite; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m ~ 1.5 -- 20 GeV; quoted limit is  for m(chi) = 5 GeV.


pdgid: S030DI5
text:
APRILE 2018 search for WIMP scatter on 1 t yr Xe; no signal, limits set in  sigma(chi N) vs. m(chi) plane for m(chi) ~ 6 -- 1000 GeV; quoted limit  is for m = 6 GeV.


pdgid: S030DI5
text:
ARNAUD 2018 search for low mass WIMP scatter on Ne via SPC at NEWS-G; limits set  in sigma^SI(chi N) vs. m(chi) plane for m ~ 0.5 -- 20 GeV; quoted limit is  for m = 5 GeV.


pdgid: S030DI5
text:
JIANG 2018 search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 3 -- 10 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
YANG 2018 search for WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 2 -- 10 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
AKERIB 2017 search for WIMP scatter on Xe; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
ANGLOHER 2017A search for GeV scale WIMP scatter on Al(2)O(3)  crystal; limits placed in sigma^SI(chi N) vs. m(chi) plane for m(chi) ~  0.15 -- 10 GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
ANGLOHER 2016 search for GeV scale WIMP scatter on  CaWO(4); limits placed in sigma^SI(chi N) vs. m(chi) plane for  m(chi) ~ 0.5 -- 30 GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
APRILE 2016 search for low mass WIMPs via ionization at XENON100; limits placed in  sigma**SI(chi N) vs m(chi) plane for m ~ 3.5 -- 20 GeV; quoted limit  is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
ARMENGAUD 2016 search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 30 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
HEHN 2016 search for low mass WIMPs via SI scatter on Ge target using profile  likelihood analysis; limits placed in sigma^SI(chi N) vs. m(chi) plane for m(chi)  ~ 4 -- 30 GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
ZHAO 2016 search for GeV-scale WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 30 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
AMOLE 2015 search for WIMP scatter on C(3)F(8) in PICO-2L;  limits placed in sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 25  GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
XIAO 2015 search for WIMP scatter on Xe with PandaX-I; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 5 -- 100 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
AGNESE 2014 search for GeV scale WIMPs SI scatter at SuperCDMS; no signal, limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 3.5 -- 30 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
AKERIB 2014 search for WIMP scatter on Xe; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 5 -- 5000 GeV. Limit  given for m(chi) = 5 GeV.


pdgid: S030DI5
text:
LI 2013B search for WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 100 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
ARCHAMBAULT 2012 search for low mass WIMP scatter on C(4)F(10);  limits set in sigma^SI(chi N) vs. m(chi) plane for m ~ 4 -- 12 GeV; quoted  limit is for m = 5 GeV.


pdgid: S030DI5
text:
AALSETH 2011 search for GeV-scale SI WIMP scatter on Ge; limits placed on  sigma**SI(chi N) for m(chi) ~ 3.5 -- 100 GeV; quoted limit is for  m(chi) = 5 GeV.


pdgid: S030DI5
text:
AHMED 2011B search for GeV scale WIMP scatter on Ge in CDMS II; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m ~ 4 -- 12 GeV.


pdgid: S030DI5
text:
ANGLE 2011 search for GeV scale WIMPs in Xenon-10; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 20 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DI5
text:
AKERIB 2010 search for WIMP scatter on Ge/Si in CDMS II; limits place  in sigma_{{SI}}(chi N) vs. m(chi) plane for m ~ 3 -- 100 GeV. Limit given for  m(DM) = 5 GeV.


pdgid: S030DI1
text:
ANGLOHER 2024A search for WIMP scatter on NaI target. No signal observed. Limits  placed in sigma^SI vs m plane.


pdgid: S030DI1
text:
AALBERS 2023 present first limits for WIMP scatter on Xe. sigma^SI(chi p)  < 1E-11 pb for m(chi) = 20 GeV.


pdgid: S030DI1
text:
ABE 2023E search for WIMP scatter on Xe in XMASS. No signal observed. Require  sigma^SI < 2E-7 pb for m(chi) = 20 GeV.


pdgid: S030DI1
text:
APRILE 2023A present first results from Xe-nton SI WIMP search. No signal observed. Quoted  limit is for m(chi) = 20 GeV.


pdgid: S030DI1
text:
MENG 2021B search for SI WIMP interaction with 3.7 t Xe and 0.63 t yr exposure. No  signal observed. Limits  placed in m(DM) vs. sigma**SI plane.


pdgid: S030DI1
text:
ANGLOHER 2019 search for low mass WIMP scatter on  CaWO(4); no signal; limits placed on Wilson coefficients for  m(chi) = 0.6 -- 60 GeV.


pdgid: S030DI1
text:
KIM 2019A search for WIMP scatter in NaI KIMS experiment; no signal: require  sigma^SI(chi n) < 7E-5 pb for m(chi) = 20 GeV.


pdgid: S030DI1
text:
KOBAYASHI 2019 search for WIMP scatter in XMASS single-phase liquid Xe detector;  no signal; require sigma^SI(chi N) < 3E-7 pb for m(chi) = 20 GeV.


pdgid: S030DI1
text:
SEONG 2019 search for Upsilon --> gamma A, A --> chi chi via CP-odd Higgs; no signal;  limits on BF set; model dependent conversion to WIMP-nucleon scattering cross section limits sigma**SI < E-36 cm**2 for m(chi) = 0.01 -- 1 GeV.


pdgid: S030DI1
text:
YANG 2019 search for low mass wimps via annual modulation in Ge; no signal;  require sigma^SI(chi N) < 3.5E-5 pb for m(chi) = 20 GeV.


pdgid: S030DI1
text:
ABE 2018C search for WIMP annual modulation signal for m(WIMP): 6 -- 20 GeV; limits  set on SI WIMP-nucleon cross section: see Fig. 6.


pdgid: S030DI1
text:
ADHIKARI 2018 search for WIMP scatter on NaI; no signal; require sigma**SI  < 1.44E-5 pb for m(WIMP) = 20 GeV; inconsistent with DAMA/LIBRA result.


pdgid: S030DI1
text:
AGNES 2018 search low mass m(WIMP): 1.8 -- 20 GeV scatter on Ar; limits on  SI WIMP-nucleon cross section set in Fig. 8.


pdgid: S030DI1
text:
AGNESE 2018 give limits for sigma^SI(chi N) for m(WIMP) between 1.5 and 20 GeV using  CDMSlite mode data.


pdgid: S030DI1
text:
AGNESE 2018A search for WIMP scatter on Ge at SuperCDMS; 1 event, consistent with expected  background; set limit in sigma^SI(chi N) vs. m(chi) plane for m ~ 10 -- 250 GeV.


pdgid: S030DI1
text:
APRILE 2018 search for WIMP scatter on 1 t yr Xe; no signal, limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 6 -- 1000 GeV.


pdgid: S030DI1
text:
ARNAUD 2018 search for low mass WIMP scatter on Ne via SPC at NEWS-G; limits set  in sigma^SI(chi N) vs. m(chi) plane for m ~ 0.5 -- 20 GeV.


pdgid: S030DI1
text:
AKERIB 2017 search for WIMP scatter on Xe; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV.


pdgid: S030DI1
text:
BARBOSA-DE-SOUZA 2017 search for annual modulation of WIMP scatter on  NaI using an exposure of 61 kg yr of DM-Ice17 for recoil energy in the  4 -- 20 keV range (DAMA found modulation for recoil energy < 5 keV). No modulation  seen. Sensitivity insufficient to distinguish DAMA signal from null.


pdgid: S030DI1
text:
CUI 2017A search for SI WIMP scatter; limits placed in sigma^SI(chi N) vs. m(chi)  plane for  m ~ 10 -- 1E4 GeV using 54 ton-day exposure of Xe.


pdgid: S030DI1
text:
AGNESE 2016 CDMSlite excludes low mass WIMPs 1.6 -- 5.5 GeV and SI scattering cross  section depending on m(WIMP); see Fig. 4.


pdgid: S030DI1
text:
ANGLOHER 2016 search for GeV scale WIMP scatter on  CaWO(4); limits placed in sigma^SI(chi N) vs. m(chi) plane for  m(chi) ~ 0.5 -- 30 GeV.


pdgid: S030DI1
text:
APRILE 2016  search for low mass WIMPs via ionization at XENON100; limits placed in  sigma**SI(chi N) vs m(chi) plane for m ~ 3.5 -- 20 GeV.


pdgid: S030DI1
text:
ARMENGAUD 2016 search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 30 GeV.


pdgid: S030DI1
text:
HEHN 2016 search for low mass WIMPs via SI scatter on Ge target using profile  likelihood analysis; limits placed in sigma^SI(chi N) vs. m(chi) plane for m(chi)  ~ 4 -- 30 GeV.


pdgid: S030DI1
text:
ZHAO 2016 search for GeV-scale WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 30 GeV.


pdgid: S030DI1
text:
AGNESE 2015A reanalyse AHMED 2011B low threshold data.  See their Fig. 12 (left) for   improved limits extending down to 5 GeV.


pdgid: S030DI1
text:
XIAO 2015 search for WIMP scatter on Xe with PandaX-I; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 5 -- 100 GeV.


pdgid: S030DI1
text:
This limit value is provided by the authors. See their Fig. 4 for limits extending down to mass(X0) = 3.5 GeV.


pdgid: S030DI1
text:
This limit value is provided by the authors. AGNESE 2014A result is from CDMSlite mode operation with enhanced sensitivity to low mass mass(X0). See their Fig. 3 for limits extending down to mass(X0) = 3.5 GeV (see also Fig. 4 in AGNESE 2014).


pdgid: S030DI1
text:
LIU 2014A result is based on prototype CDEX-0 detector. See their Fig. 13 for limits extending down to mass(X0) = 2 GeV.


pdgid: S030DI1
text:
AARTSEN 2013 search for neutrinos from the Sun arising from the pair annihilation of X0  trapped by the sun in data taken between June 2010 and May 2011.


pdgid: S030DI1
text:
This limit value is provided by the authors. AGNESE 2013 use data taken between Oct. 2006 and July 2007. See their Fig. 4 for limits extending down to mass(X0) = 7 GeV.


pdgid: S030DI1
text:
This limit value is provided by the authors. AGNESE 2013A use data taken between July 2007 and Sep. 2008. Three candidate events are seen. Assuming these events are real, the best fit parameters are mass(X0) = 8.6 GeV and sigma = 1.9E-5 pb.


pdgid: S030DI1
text:
This limit value is provided by the authors. Limit from combined data of AGNESE 2013 and AGNESE 2013A. See their Fig. 4 for limits extending down to mass(X0) = 5.5 GeV.


pdgid: S030DI1
text:
BERNABEI 2013A search for annual modulation of counting rate in the 2 -- 6 keV recoil  energy interval, in a 14 yr live time exposure of 1.33 t yr. Find a modulation of  0.0112+-0.0012 counts/(day kg keV) with 9.3 sigma C.L. Find period and phase in agreement with  expectations from DM particles.


pdgid: S030DI1
text:
LI 2013B search for WIMP scatter on Ge; limits placed in  sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 4 -- 100 GeV.


pdgid: S030DI1
text:
ANGLOHER 2012 observe excess events above the expected background which are consistent with X0 with mass  ~ 25 GeV (or 12 GeV) and spin-independent X0-nucleon cross section of 2E-6 pb (or 4E-5 pb).


pdgid: S030DI1
text:
AALSETH 2011A find indications of annual modulation of the data, the energy spectrum being compatible with X0 mass around 8 GeV. See also AALSETH 2013.


pdgid: S030DI1
text:
AHMED 2011 search for X0 inelastic scattering. See their Fig. 8 -- 10 for limits. The inelastic cross section reduces to the elastic cross section at the limit of zero mass splitting (Fig. 8, left).


pdgid: S030DI1
text:
APRILE 2011A search for X0 inelastic scattering. See their Fig. 2 and 3 for limits. See also APRILE 2014A.


pdgid: S030DI2
text:
AALBERS 2023 present first LZ limits on SI WIMP-nucleon scatter from Xe.  sigma^SI(chi p) < 2.5E-11 pb for m(chi) = 100 GeV.


pdgid: S030DI2
text:
ABE 2023E search for WIMP scatter on Xe in XMASS. No signal observed. Require  sigma^SI < 2E-7 pb for m(chi) = 100 GeV.


pdgid: S030DI2
text:
APRILE 2023A present first results from Xe-nton SI WIMP search. No signal observed. Quoted  limit is for m(chi) = 100 GeV.


pdgid: S030DI2
text:
MENG 2021B search for SI WIMP interaction with 3.7 t Xe and 0.63 t yr exposure. No  signal observed. Limits placed in m(DM) vs. sigma**SI plane.


pdgid: S030DI2
text:
ADHIKARI 2020 search for SI WIMP scatter from Ar in AJAJ 2019 data. No  signal observed. Limits placed on sigma^p vs. m(WIMP) for various assumed operators and models.


pdgid: S030DI2
text:
ABE 2019 search for SI DD in single phase Xe; no signal; require  sigma^SI(chi p) < 4E-8 pb for m(chi) ~ 100 GeV.


pdgid: S030DI2
text:
AJAJ 2019 search for SI WIMP-nucleon scatter with 758 tonne day exposure of single phase  liquid Ar; no signal: require sigma^SI(chi N) < 3.9E-9 pb for  m(chi) = 100 GeV.


pdgid: S030DI2
text:
ADHIKARI 2018 search for WIMP scatter on NaI;limit set sigma**SI(chi p) <  2.3E-6 pb for m(chi) = 100 GeV.


pdgid: S030DI2
text:
AGNES 2018A search for WIMP scatter on 46.4 kg Ar; no signal; require  sigma^SI(chi N) < 1.14E-8 pb for m(chi) = 100 GeV.


pdgid: S030DI2
text:
AMAUDRUZ 2018 search for WIMP scatter on Ar with DEAP-3600; limits set:  sigma**SI(chip) < 1.2E-8 pb for m(WIMP) = 100 GeV.


pdgid: S030DI2
text:
APRILE 2018 search for WIMP scatter on 1.3 t liquid Xe; no signal; require  sigma^SI(chi p) < 9.12E-11 pb for m(chi) = 100 GeV.


pdgid: S030DI2
text:
REN 2018 search for self-interacting DM at Panda-X-II with a total exposure of 54 ton day;  limits set in m(DM) vs. m(mediator) plane.


pdgid: S030DI2
text:
AKERIB 2017 exclude SI cross section > 1.7E-10 pb for m(WIMP) = 100 GeV. Uses  complete LUX data set.


pdgid: S030DI2
text:
APRILE 2017G set limit sigma**SI(chi p) < 1.2 E-10 pb for m(WIMP) =  100 GeV using 1 ton fiducial mass Xe TPC. Exposure is 34.2 live days.


pdgid: S030DI2
text:
AKERIB 2016 re-analysis of 2013 data exclude SI cross section > 1E-9 pb for  m(WIMP) = 100 GeV on Xe target.


pdgid: S030DI2
text:
APRILE 2016B combined 447 live days using Xe target exclude  sigma(SI) > 1.1E-9 pb for m(WIMP) = 50 GeV.


pdgid: S030DI2
text:
AVRORIN 2014 search for neutrinos from the Sun arising from the pair annihilation of X0 trapped by the Sun in data taken between 1998 and 2003. See their Table 1 for limits assuming annihilation into neutrino pairs.


pdgid: S030DI2
text:
AARTSEN 2013 search for neutrinos from the Sun arising from the pair annihilation of X0 trapped by the sun in data taken between June 2010 and May 2011.


pdgid: S030DI2
text:
ADRIAN-MARTINEZ 2013 search for neutrinos from the Sun arising from the pair annihilation of X0 trapped by the sun in data taken between Jan. 2007 and Dec. 2008.


pdgid: S030DI2
text:
BOLIEV 2013 search for neutrinos from the Sun arising from the pair annihilation of X0 trapped by the sun in data taken from 1978 to 2009. See also SUVOROVA 2013 for an older analysis of the same data.


pdgid: S030DI2
text:
ABBASI 2012 search for neutrinos from the Sun arising from the pair annihilation of X0 trapped by the Sun. The amount of X0 depends on the X0-proton cross section.


pdgid: S030DI2
text:
AJELLO 2011 search for e+- flux from X0 annihilations in the Sun. Models in which X0 annihilates  into an intermediate long-lived weakly interacting particles or X0 scatters inelastically are constrained. See their Fig. 6 -- 8 for limits.


pdgid: S030DI2
text:
GIULIANI 2005 analyzes the spin-independent X0-nucleon cross section limits with both isoscalar and isovector couplings. See their Fig. 3 and 4 for limits on the couplings.


pdgid: S030DI3
text:
AALBERS 2023 give first LZ limits on WIMP-nucleon scatter from Xe. sigma^SI  < 2.8E-10 pb for m(chi) = 1 TeV.


pdgid: S030DI3
text:
ABE 2023E search for WIMP scatter on Xe in XMASS. No signal observed. Require  sigma^SI < 2E-7 pb for m(chi) = 1000 GeV.


pdgid: S030DI3
text:
ADHIKARI 2020 search for SI WIMP scatter from Ar in AJAJ 2019 data. No   signal observed. Limits placed on sigma^p vs. m(WIMP) for various assumed operators and models.


pdgid: S030DI3
text:
YAGUNA 2019 recasts DEAP-3600 single-phase liquid argon results in  limit for isospin  violating DM; for f_{{n}}/f_{{p}} = -0.69, requires sigma^SI(chi p) < 3E-6   pb for m(chi) = 1 TeV.


pdgid: S030DI3
text:
AGNES 2018A search for WIMP scatter on 46.4 kg Ar; no signal; require  sigma^SI(chi N) < 3.8E-8 pb for m(chi) = 1 TeV.


pdgid: S030DI3
text:
APRILE 2018 search for WIMP scatter on 1.3 t Xe; no signal seen; require  sigma^SI(chi p) < 8.24E-10 pb for m(chi) = 1 TeV.


pdgid: S030DI3
text:
AKERIB 2017 search for WIMP scatter on Xe using complete LUX data set; limits  placed in sigma^SI(chi N) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV.


pdgid: S030DI3
text:
CHEN 2017E search for inelastic WIMP scatter on Xe; require  sigma**SI(chi N) < 0.3 pb for m(chi) = 1 TeV and (mass difference) = 300 keV.


pdgid: S030DI3
text:
CUI 2017A search for WIMP scatter using 54 ton-day exposure of Xe; limits placed  in sigma^SI(chi N) vs. m(chi) plane for m ~ 10 -- 1E4 GeV.


pdgid: S030DI6
text:
AALBERS 2024A search for ultraheavy dark matter in range 10E8 -- 10E17 GeV via  multiple scatter. No signal observed. Limits placed in sigma^SI vs m plane for two different  nuclear scaling possibilities.


pdgid: S030DI6
text:
ABREU 2023 search for superheavy DM X decay to q qbar pairs via instanton, then   to  gammas. No signal detected. Exclude m(X) > 3E13 GeV for dark gauge coupling    alpha_{{X}} = 0.09.


pdgid: S030DI6
text:
ACEVEDO 2023 re-examine data from ancient mica to place limits on superheavy DM  in the mass range E7 -- E25 GeV. See Fig. 3 for sigma^SI and sigma^SD limits.


pdgid: S030DP5
text:
ANGLOHER 2024B search for low mass wimps. No signal observed. Limits placed in sigma vs.  m plane. Quoted limit for m = 100 MeV.


pdgid: S030DP5
text:
AALBERS 2023A search for GeV-scale WIMP scatter on Xe. No signal observed. Limits  placed in sigma^SD(chi p) vs. m(chi) plane. Quoted limit is for m(chi) = 1 GeV via  Migdal scattering.


pdgid: S030DP5
text:
ADHIKARI 2022B search for sub-GeV WIMPs via SI and SD detection; no signal detected; limits   placed in m(chi) vs. sigma plane for m(chi): 0.2 -- 3 GeV; quoted limit is for  SD  m(chi) = 1 GeV.


pdgid: S030DP5
text:
ANGLOHER 2022 search for SD WIMP-proton scatter from Li target; no signal  detected;  limits placed in sigma vs. m(WIMP) plane; limit quoted for m(WIMP) = 1 GeV.


pdgid: S030DP5
text:
ANGLOHER 2022A search for spin-dependent DM scatter on Li and Al for  m(DM) ~    0.2 -- 6 GeV; no signal observed; limits set in CS(chi p) vs. m(DM)  plane; quoted   limit is for m(DM) = 1 GeV.


pdgid: S030DP5
text:
ABDELHAMEED 2020A use LiAlO(2) target in CRESST to search for SD WIMP scatter  on p; no signal; quoted limit is for m(DM) = 1 GeV.


pdgid: S030DP5
text:
ABDELHAMEED 2019 search for SD WIMP scatter on Li7; limits placed on  sigma^SD(chi p) for m(chi) ~ 0.8 -- 20 GeV; quoted limit is for m(chi)  = 1 GeV.


pdgid: S030DP5
text:
AMOLE 2019 search for SD WIMP scatter on C(3)F(8) in PICO-60  bubble chamber; no signal: set limit for spin dependent coupling sigma^SD(chi p) <  2E-4 pb for m(chi) = 5 GeV.


pdgid: S030DP5
text:
APRILE 2019C search for light DM on Xe via Migdal/brem effect; no signal, require  sigma^SD(chi p) < 1.7E4 pb for m(chi) = 1 GeV.


pdgid: S030DP5
text:
ARMENGAUD 2019 search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 0.5 -- 10 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DP5
text:
XIA 2019A search for WIMP scatter on Xe in PandaX-II; limits placed in  sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DP5
text:
AGNESE 2018 search for GeV scale WIMPs with CDMSlite; limits placed in  sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 1.5 -- 20 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DP5
text:
AKERIB 2017A search for SD WIMP scatter on Xe using 129.5 kg yr exposure; limits placed in sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 6 -- 1E5 GeV.


pdgid: S030DP5
text:
FU 2017 search for SD WIMP scatter on Xe; limits set in sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 4 -- 1E3 GeV.; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DP5
text:
AMOLE 2015 search for WIMP scatter on C(3)F(8) in PICO-2L;  limits placed in sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 4 -- 1E4 GeV;  quoted limit is for m(chi) = 5 GeV.


pdgid: S030DP5
text:
ARCHAMBAULT 2012 search for SD WIMP scatter in F19 with PICASSO; limits set in  sigma^SD(chi p) vs. m(chi) plane for m ~ 4 -- 500 GeV; quoted limit is for  m(chi) = 5 GeV.


pdgid: S030DP1
text:
AALBERS 2023 yield first SD LZ limits on WIMP-p scatter using Xe.  sigma^SD(chi p) < 6E-5 pb for m(chi) = 20 GeV.


pdgid: S030DP1
text:
ABBASI 2022B search for WIMP annihilation to b bbar, tau taubar, nu nubar in Sun  with 7 years data; no signal; limits set in m(chi) vs. sigma^SD(chi p) plane for  m(chi): 10 -- 100 GeV; quoted limit for nu nubar channel.


pdgid: S030DP1
text:
ANGLOHER 2022 search for SD WIMP-proton scatter from Li target; no signal  detected; limits placed in sigma vs. m(WIMP) plane.


pdgid: S030DP1
text:
HUANG 2022 search for SD DM scatter on Xe; no signal observed; limits placed in  CS(chi n) vs. m(DM) plane; quoted limit is for m(DM) = 20 GeV.


pdgid: S030DP1
text:
AARTSEN 2020C place combined IceCube and Pico-60 velocity-independent limits on  spin-dependent WIMP-p scatter sigma^SD(chi p)< 9 -- 5 pb for m(WIMP) = 20  GeV assuming dominant annihilation to tau taubar.


pdgid: S030DP1
text:
ABDELHAMEED 2020A use LiAlO(2) target in CRESST to search for spin-dependent  WIMP scatter on p; limits set for m(WIMP): 0.3 -- 30 GeV in Fig. 8.  Quoted limit is for M(WIMP) = 30 GeV.


pdgid: S030DP1
text:
ABDELHAMEED 2019 uses Li(2)MoO(4) target to set limit for spin  dependent coupling sigma^SD(chi p) < 3.E5 pb for m(chi) = 20 GeV.


pdgid: S030DP1
text:
AMOLE 2019 search for SD WIMP scatter on C(3)F(8) in PICO-60  bubble chamber; no signal: set limit for spin dependent coupling sigma^SD(chi p) <  2.5E-5 pb for m(chi) = 20 GeV.


pdgid: S030DP1
text:
APRILE 2019A search for SD WIMP scatter on 1 t yr Xe; no signal, limits placed in  sigma^SD(chi p) vs. m(chi) plane for m ~ 6 -- 1000 GeV.


pdgid: S030DP1
text:
XIA 2019A search for WIMP scatter on Xe in PandaX-II; limits placed in  sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV.


pdgid: S030DP1
text:
AGNESE 2018 give limits for sigma^SD(p chi) for m(WIMP) between 1.5 and 20 GeV using  CDMSlite mode data.


pdgid: S030DP1
text:
BEHNKE 2017 show final Picasso results based on 231.4 kg d exposure at SNOLab for WIMP  scatter on C(4)F(10) search via superheated droplet; require  sigma(SD) < 1.32E-2 pb for m(WIMP) = 20 GeV.


pdgid: S030DP1
text:
FU 2017 search for SD WIMP scatter on Xe; limits set in  sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 4 -- 1E3 GeV.


pdgid: S030DP1
text:
AMOLE 2016A require SD WIMP-p scattering < 5E-4 pb for m(WIMP) = 20  GeV; bubbles from C(3)F(8) target.


pdgid: S030DP1
text:
KHACHATRYAN 2016AJ require SD WIMP-p < 2E-6 pb for m(WIMP) = 20 GeV  from p p --> Z + notET; Z --> lepton leptonbar signal.


pdgid: S030DP1
text:
The value has been provided by the authors. APRILE 2013 note that the proton limits on Xe are highly sensitive to the theoretical model used. See also APRILE 2014A.


pdgid: S030DP1
text:
ARCHAMBAULT 2012 search for WIMP scatter on C(4)F(10); limits  set in sigma^SD(chi p) vs. m(chi) plane for m ~ 4 -- 500 GeV.


pdgid: S030DP1
text:
TANAKA 2011 search for neutrinos from the Sun arising from the pair annihilation of X0 trapped by the Sun.  The amount of X0 depends on the X0-proton cross section.


pdgid: S030DP2
text:
AALBERS 2023 yield first SD LZ limits on WIMP-p scatter using Xe.  sigma^SD(chi p) < 1.5E-4 pb for m(chi) = 100 GeV.


pdgid: S030DP2
text:
ADHIKARI 2023C search for SD WIMP scatter on I. No signal observed. Require  sigma^SD(chi p) <  1 pb for m(chi) = 100 GeV.


pdgid: S030DP2
text:
SHIMADA 2023 search for WIMPs in NEWAGE directional detector. No signal observed. Limits  placed in sigma^SD(chi p) vs. mass plane. Quoted limit for m(chi) = 150 GeV.


pdgid: S030DP2
text:
HUANG 2022 search for SD DM scatter on Xe; no signal observed; limits placed in  CS(chi n) vs. m(DM) plane; quoted limit is for m(DM) = 100 GeV.


pdgid: S030DP2
text:
IKEDA 2021 use direction sensitive TPC NEWAGE to search for SD WIMPs. No signal observed.  Limits set in sigma^SD(chi p) vs. m plane; sigma^SD(chi p) < 50 pb for m(DM)  = 100 GeV.


pdgid: S030DP2
text:
AARTSEN 2020C place combined IceCube and Pico-60 velocity-independent limits on  spin-dependent WIMP-p scatter sigma^SD(chi p) < 3.34E-4 pb for m(WIMP) = 100  GeV assuming dominant annihilation to tau taubar.


pdgid: S030DP2
text:
AMOLE 2019 search for SD WIMP scatter on C(3)F(8) in PICO-60  bubble chamber; no signal: set limit for spin dependent coupling sigma^SD(chi p) <  4E-5 pb for m(chi) = 100 GeV.


pdgid: S030DP2
text:
AKERIB 2017A search for SD WIMP scatter on Xe using 129.5 kg yr exposure; limits  placed in sigma^SD(chi p) vs. m(chi) plane for m(chi) ~ 6 -- 1E5 GeV.


pdgid: S030DP2
text:
AMOLE 2017 require CS(WIMP-p)**SD < 5E-5 pb for m(WIMP) = 100 GeV using  PICO-60 1167 kg-days exposure at SNOLab.


pdgid: S030DP2
text:
APRILE 2017A require require CS(WIMP-p)(inelastic)**SD < 3.3E-2 pb for  m(WIMP) = 100 GeV, based on 7640 kg day exposure at LNGS.


pdgid: S030DP2
text:
BATTAT 2017 use directional detection of CS(2) ions to require  CS(SD) < 2.8E-1 pb for 100 GeV WIMP with a 55 days exposure at the  Boulby  Underground  Science Facility.


pdgid: S030DP2
text:
FU 2017 from a 33000 kg d exposure at CJPL, PANDAX II derive for m(DM) = 100 GeV,  sigma^SD(WIMP-p) <2E-3 pb.


pdgid: S030DP2
text:
AABOUD 2016D use ATLAS 13 TeV 3.2 fb^{-1} of data to search for monojet plus missing  E(T); agree with SM rates; present limits on large extra dimensions, compressed SUSY spectra  and wimp pair production.


pdgid: S030DP2
text:
AABOUD 2016F search for monophoton plus missing E(T) events at ATLAS with 13 Tev and 3.2  fb**-1; signal agrees with SM background; place limits on SD WIMP-proton scattering vs.  mediator mass and large extra dimension models.


pdgid: S030DP2
text:
AARTSEN 2016C search for high energy nus from WIMP annihilation in solar core; limits set  on SD WIMP-p scattering (Fig. 8).


pdgid: S030DP2
text:
ADRIAN-MARTINEZ 2016 search for WIMP annihilation into nus from solar core; exclude SD  cross section < few E-4 depending on m(WIMP).


pdgid: S030DP2
text:
AMOLE 2016 use bubble technique on CF(3)I target to exclude SD WIMP-p scattering  > 5E-4 pb for m(WIMP) = 100 GeV.


pdgid: S030DP3
text:
AALBERS 2023 yield first SD LZ limits on WIMP-p scatter using Xe.  sigma^SD(chi p) < 2E-3 pb for m(chi) = 1 TeV.


pdgid: S030DP3
text:
ADHIKARI 2023C search for SD WIMP scatter on I. No signal observed. Require  sigma^SD(chi p) < 0.2 pb for m(chi) = 1 TeV.


pdgid: S030DP3
text:
HUANG 2022 search for SD DM scatter on Xe; no signal observed; limits placed in  CS(chi n) vs. m(DM) plane; quoted limit is for m(DM) = 1 TeV.


pdgid: S030DP3
text:
IKEDA 2021 use direction sensitive TPC NEWAGE to search for SD WIMPs. No signal observed.  Limits set in sigma^SD(chi p) vs. m plane; sigma^SD(chi p) < 200 pb for m(DM)  = 1000 GeV.


pdgid: S030DP3
text:
AARTSEN 2020C place combined IceCube and Pico-60 velocity-independent limits on  spin-dependent WIMP-p scatter sigma^SD(chi p) < 3E-3 pb for m(WIMP) = 1 TeV  assuming dominant annihilation to W W.


pdgid: S030DP3
text:
AMOLE 2019 search for SD WIMP scatter on C(3)F(8) in PICO-60  bubble chamber; no signal: set limit for spin dependent coupling sigma^SD(chi p) <  3E-4 pb for m(chi) = 1000 GeV.


pdgid: S030DP3
text:
ALBERT 2018C search for DM annihilation in Sun to long-lived mediator (LLM) which decays  outside Sun, for DM masses above 1 TeV; assuming LLM, limits set on sigma**SD(chi p).


pdgid: S030DP3
text:
AARTSEN 2017A search for neutrinos from solar WIMP annihilation into tau+ tau- in 532  days of live time.


pdgid: S030DP3
text:
ADRIAN-MARTINEZ 2016B search for secluded DM via WIMP annihilation in solar core into light  mediator which later decays to mu or nus; limits presented in Figures 3 and 4.


pdgid: S030DN5
text:
AALBERS 2023A search for GeV-scale WIMP scatter on Xe. No signal observed. Limits  placed in sigma^SD(chi n) vs. m(chi) plane. Quoted limit is for m(chi) = 1 GeV via  Migdal scattering.


pdgid: S030DN5
text:
ANGLOHER 2022 search for SD WIMP scatter on Li target; no signal detected; limits  placed on WIMP-neutron SD scatter versus m(WIMP); limit quoted for m(WIMP) = 1 GeV.


pdgid: S030DN5
text:
ANGLOHER 2022A search for spin-dependent DM scatter on Li and Al for  m(DM) ~    0.2 -- 6 GeV; no signal observed; limits set in CS(chi n) vs. m(DM)  plane; quoted    limit is for m(DM) = 1 GeV.


pdgid: S030DN5
text:
ABDELHAMEED 2020A use LiAlO(2) target in CRESST to search for SD WIMP scatter;  no signal; quoted limit is for m(DM) = 1 GeV.


pdgid: S030DN5
text:
ABDELHAMEED 2019 search for GeV-scale WIMP SD scatter on Li7 crystal; set limit  sigma^SD(chi n) for m(chi) ~ 0.8 -- 20 GeV; quoted limit for m(chi) =  1 GeV.


pdgid: S030DN5
text:
APRILE 2019C search for light DM on Xe via Migdal/bremsstrahlung effect; no  signal, require sigma^SD(chi n) <230 pb for m(chi) = 1 GeV.


pdgid: S030DN5
text:
APRILE 2019D search for light DM scatter on Xe via ionization; no signal, limits  placed in sigma vs. m(DM) ~ 3 -- 6 GeV; quoted limit is for m(DM) = 5 GeV.


pdgid: S030DN5
text:
ARMENGAUD 2019 search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 0.5 -- 10 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DN5
text:
XIA 2019A search for WIMP scatter on Xe in PandaX-II; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DN5
text:
AGNESE 2018 search for GeV scale WIMPs scatter at CDMSlite; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m ~ 1.5 -- 20 GeV; quoted limit is  for m(chi) = 5 GeV.


pdgid: S030DN5
text:
JIANG 2018 search for GeV scale WIMP scatter on Ge; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 3 -- 10 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DN5
text:
YANG 2018 search for WIMP scatter on Ge; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 2 -- 10 GeV;  quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DN5
text:
AKERIB 2017A search for SD WIMP scatter on Xe with 129.5 kg yr exposure; limits  placed in sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV; quoted limit is for m(chi) = 5 GeV.


pdgid: S030DN5
text:
FU 2017 search for SD WIMP scatter on Xe; limits set in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 4 -- 1E3 GeV.; quoted limit is for  m(chi) = 5 GeV.


pdgid: S030DN5
text:
ZHAO 2016 search for GeV-scale WIMP scatter on Ge; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 4 -- 30 GeV; quoted  limit is for m(chi) = 5 GeV.


pdgid: S030DN5
text:
AHMED 2011B search for GeV scale WIMP scatter on Ge in CDMS II; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m ~ 4 -- 12 GeV. Limit given for  m(chi) = 5 GeV.


pdgid: S030DN1
text:
AALBERS 2023 yield first LZ limits on SD WIMP-n scatter using Xe.   sigma^SD(chi n)< 2E-6 pb for m(chi) = 20 GeV.


pdgid: S030DN1
text:
ANGLOHER 2022 search for SD WIMP-neutron scatter from Li target; no signal  detected; limits placed in sigma vs. m(WIMP) plane.


pdgid: S030DN1
text:
ABDELHAMEED 2020A use LiAlO(2) target in CRESST to search for SD WIMP scatter  on n; limits placed for m(WIMP): 0.3 -- 30 GeV in Fig. 8.  Quoted limit is for M(WIMP) = 30 GeV.


pdgid: S030DN1
text:
APRILE 2019A search for SD WIMP scatter on 1 t yr Xe; no signal: limits placed in  sigma^SD(chi n) vs. m(chi) plane for m ~ 6 -- 1000 GeV.


pdgid: S030DN1
text:
XIA 2019A search for WIMP scatter on Xe in PandaX-II; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV.


pdgid: S030DN1
text:
AGNESE 2018 give limits for sigma^SD(n chi) for m(WIMP) between 1.5 and 20 GeV using  CDMSlite mode data.


pdgid: S030DN1
text:
AKERIB 2017A search for SD WIMP scatter on Xe with 129.5 kg yr exposure; limits  placed in sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 5 -- 1E5 GeV.


pdgid: S030DN1
text:
FU 2017 search for SD WIMP scatter on Xe; limits set in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 4 -- 1E3 GeV.


pdgid: S030DN1
text:
ZHAO 2016 search for GeV-scale WIMP scatter on Ge; limits placed in  sigma^SD(chi n) vs. m(chi) plane for m(chi) ~ 4 -- 30 GeV.


pdgid: S030DN2
text:
AALBERS 2023 yield first LZ limits on SD WIMP-n scatter using Xe.  sigma(chi n) < 5E-6 pb for m(chi) = 100 GeV.


pdgid: S030DN2
text:
APRILE 2019A search for SD WIMP scatter on 1 t yr Xe; no signal, limits placed in  sigma^SD(chi n) vs. m(chi) plane for m ~ 6 -- 1000 GeV.


pdgid: S030DN2
text:
SUZUKI 2019 search in single phase liquid xenon detector for inelastic scattering  X0 +  ^129Xe --> X0 +  ^129Xe* (39.58 keV) ; no signal: require  CS(chi n)**SD < 4E-3 pb for m(chi) = 100 GeV.


pdgid: S030DN2
text:
UCHIDA 2014 derived limit from search for inelastic scattering X0 +  ^129Xe --> X0 +  ^129Xe(39.58  keV).


pdgid: S030DN2
text:
MIUCHI 2003 give model-independent limit for spin-dependent X0-proton and neutron cross sections. See their Fig. 5.


pdgid: S030DN3
text:
AALBERS 2023 yield first LZ SD limits on WIMP-n scatter on Xe.  sigma^SD(chi n) < 5E-5 pb for m(chi) = 1 TeV.


pdgid: S030DE5
text:
SHANG 2024 report on search for electron cosmic-ray boosted DM in keV range or below with  PandaX-4T. No signal observed. Limits plotted in sigma(chi e) vs m plane for m  ~E-2 -- E3 keV.


pdgid: S030DE5
text:
ZHANG 2024A examine detection of accelerated MeV-scale DM on e in Ge  semiconductor. Limits placed in sigma_{{e}} vs. m plane depending on various mediator assumptions.


pdgid: S030DE5
text:
AGNES 2023A search for MeV-scale DM scatter from e using Ar. No signal  observed. sigma(chi e) < 3E-3 pb for m(chi) = 30 MeV.


pdgid: S030DE5
text:
ARNQUIST 2023A search for LDM scatter on e using CCDs. No signal observed. Require    sigma(chi e) < 0.3 pb for m(chi) = 10 MeV and F(DM) = 1 (Fig. 3b).


pdgid: S030DE5
text:
LI 2023F search for light DM in MeV range via scatter from e. No signal observed. Limits  set. The quoted limit is for m(chi) = 0.2 GeV with F(DM) = 1.


pdgid: S030DE5
text:
AGOSTINI 2022 search for superWIMP particles using GERDA detector; no  signal observed;  limits placed in mass vs coupling plane for m(DM) 0.06 -- 1 MeV.


pdgid: S030DE5
text:
APRILE 2022 place new limits on WIMP-e scatter for dark photon and various multipole  moments vs. WIMP mass for various DM models; quoted limit for m(WIMP) = 1 GeV in light mediator  model.


pdgid: S030DE5
text:
BATTAGLIERI 2022 search for light MeV scale DM particles produced in JLAB beam dump; no   signal observed; limits set in kinetic mixing vs. m(DM) plane for m(DM) ~ 1 -- 200  MeV .


pdgid: S030DE5
text:
BOSE 2022 theoretically derive limits on WIMP-e scatter from solar gamma rays using data  of Fermi-LAT; limit quoted for m(WIMP) = 5 GeV.


pdgid: S030DE5
text:
GHOSH 2022 derive limits on sub-GeV boosted DM scatter from e or nu using   SuperK/XENON1T  data; quoted limit for m(chi) = 1 MeV.


pdgid: S030DE5
text:
HOCHBERG 2022 search for sub-eV or sub-MeV scale DM scatter/absorption on e in  superconducting nanowire; no signal observed; limits set in m(DM) vs. cross section plane for  sub-MeV-scale DM and in m(DM) vs. kinetic mixing plane for sub-eV-scale DM.


pdgid: S030DE5
text:
ZHANG 2022A search for DM scatter on e using CDEX-10; no signal observed; limits placed  on CS(chi e) vs. m(DM) plane for m(DM) ~ 0.07 -- 10 GeV for various simplified  models.


pdgid: S030DE5
text:
CHENG 2021 search for MeV-scale DM scatter from e in PANDAX-II. No signal detected.  Limits set in sigma(chi e) vs. m(DM) plane for two choices of form factors;  sigma(chi e) < 10 pb for m(chi) = 10 MeV and F(DM) = 1.


pdgid: S030DE5
text:
AKERIB 2020 search for mirror DM with LUX 95 d x 118 kg data for mirror e  scatter from Xe; no signal, limits placed in kinetic mixing parameter vs. mirror e  temperature T ~ 0.1 -- 0.9 keV plane.


pdgid: S030DE5
text:
AMARAL 2020 search SuperCDMS data for low mass DM scatter from e in Si; no  signal; quoted limit sigma_{{e}} < 8.7E2 pb for m(DM) = 10 MeV with form factor  F(DM) = 1.


pdgid: S030DE5
text:
APRILE 2020 report excess at electron recoil around 2 -- 3 keV in Xe; data  compared to unforeseen tritium background, and various signal models (bosonic DM, solar axion, and  neutrino magnetic moment).


pdgid: S030DE5
text:
ARNAUD 2020 search for MeV DM scattering from e in Ge; no signal; quoted limit  is for m(DM) = 10 MeV with form factor F(DM) = 1.


pdgid: S030DE5
text:
BARAK 2020 report search for MeV scale DM scatter from e in Si; limits placed  in sigma_{{e}} vs. m(DM) plane; quoted limit is for m(DM) = 10 MeV and form factor F(DM) = 1.


pdgid: S030DE5
text:
ABRAMOFF 2019 search for MeV-scale WIMP scatter from Si skipper-CCD; limits placed  on sigma(chi e) for m(chi) ~ 0.5 -- 100 MeV depending on DM form factors.  Limit given for m(DM) = 1 MeV.


pdgid: S030DE5
text:
AGUILAR-AREVALO 2019A search for MeV scale DM scatter from e in Si CCDs at  SNOLAB; no signal, limits placed in CS(e) vs. m(DM) plane for m(DM) ~ 0.6 -- 100 MeV.


pdgid: S030DE5
text:
APRILE 2019D search for light DM scatter on Xe via ionization; no signal, limits  placed in sigma on nucleus vs. m(DM) plane for m(DM) ~ 0.02 -- 10 GeV; quoted  limit is for m(DM) = 0.2 GeV.


pdgid: S030DE5
text:
AGNES 2018B search for MeV scale WIMP scatter from e in Ar; no signal, limits  set in sigma_{{e}} vs. m(chi) plane for m ~ 20 -- 1000 MeV and two choices of form  factor F(DM); quoted limit for m(chi) = 100 MeV and F = 1.


pdgid: S030DE5
text:
AGNESE 2018B search for e chi scatter in SuperCDMS; limits placed in sigma(e chi)  vs. m(chi) plane for m ~ 0.3 -- 1E4 MeV for two assumed form factors and also in  m(dark photon) vs. kinetic mixing plane. Limit given for m(chi) = 1 GeV and F=1.


pdgid: S030DE5
text:
CRISLER 2018 search for chi e --> chi e scatter in Si CCD; place limits on MeV  DM in sigma_{{e}} vs. m(chi) plane for m ~ 0.5 -- 1000 MeV for different form  factors; quoted limit is for F(DM) = 1 and m(chi) = 10 MeV.


pdgid: S030DE5
text:
APRILE 2017 search for WIMP-e annual modulation signal for recoil energy in the  2.0 -- 5.8 keV interval using 4 years data with Xe. No significant effect seen.


pdgid: S030DM5
text:
AKIMOV 2022 use COHERENT CsI(Na) detector to search for sub GeV DM particles produced by the   Spallation Neutron Source; no signal  observed; limits placed in mediator mass vs. coupling plane   for leptophobic DM models.


pdgid: S030DM1
text:
BENOIT 2000 find four event categories in Ge detectors and suggest that low-energy surface nuclear recoils can explain anomalous events reported by UKDMC and Saclay NaI experiments.


pdgid: S030DM1
text:
BELLI 1996C use background subtraction and obtain sigma<150pb (<1.5fb) (90% CL) for spin-dependent (independent) X0-proton cross section. The confidence level is from R. Bernabei, private communication, May 20, 1999.


pdgid: S030DM1
text:
BERNABEI 1996 use pulse shape discrimination to enhance the possible signal.  The limit here is from R.Bernabei, private communication, September 19, 1997.


pdgid: S030DM1
text:
SARSA 1996 search for annual modulation of WIMP signal. See SARSA 1997 for details of the analysis. The limit here is from M.L.Sarsa, private communication, May 26, 1997.


pdgid: S030DM1
text:
SMITH 1996 use pulse shape discrimination to enhance the possible signal.  A dark matter density of 0.4GeVcm**-3 is assumed.


pdgid: S030DM1
text:
GARCIA 1995 limit is from the event rate.  A weaker limit is obtained from searches for diurnal and annual modulation.


pdgid: S030DM1
text:
REUSSER 1991 limit here is changed from published (0.04) after reanalysis by authors. J.L.Vuilleumier, private communication, March 29, 1996.


pdgid: S030DM2
text:
APRILE 2021A search for inelastic DM scatter off Xe129 nuclei with 0.83 t yr    exposure. No signal obseved. Limits placed in sigma(chiXe) vs. m(DM) plane for  WIMP  mass  between 20 GeV and 10 TeV.


pdgid: S030DM2
text:
BELLI 2002 discuss dependence of the extracted WIMP cross section on the assumptions of the galactic halo structure.


pdgid: S030DM2
text:
BERNABEI 2002C analyze the DAMA data in the scenario in which X0 scatters into a slightly heavier state as discussed by SMITH 2001.


pdgid: S030DM2
text:
GREEN 2002 discusses dependence of extracted WIMP cross section limits on the assumptions of the galactic halo structure.


pdgid: S030DM2
text:
ULLIO 2001 disfavor the possibility that the BERNABEI 1999 signal is due to spin-dependent WIMP coupling.


pdgid: S030DM2
text:
AMBROSIO 1999 search for upgoing muon events induced by neutrinos originating from WIMP annihilations in the Sun and Earth.


pdgid: S030DM2
text:
BRHLIK 1999 discuss the effect of astrophysical uncertainties on the WIMP interpretation of the BERNABEI 1999 signal.


pdgid: S030DM2
text:
BELLI 1996C use background subtraction and obtain sigma<0.35pb (<0.15fb) (90% CL) for spin-dependent (independent) X0-proton cross section. The confidence level is from R. Bernabei, private communication, May 20, 1999.


pdgid: S030DM2
text:
REUSSER 1991 limit here is changed from published (0.3) after reanalysis by authors. J.L.Vuilleumier, private communication, March 29, 1996.


pdgid: S030DM3
text:
BERNABEI 1999D search for SIMPs (Strongly Interacting Massive Particles) in the mass range 10**3 -- 10**16 GeV.  See their Fig.3 for cross-section limits.


pdgid: S030DM3
text:
DERBIN 1999 search for SIMPs (Strongly Interacting Massive Particles) in the mass range 10**2 -- 10**14 GeV.  See their Fig.3 for cross-section limits.


pdgid: S030DM3
text:
BELLI 1996C use background subtraction and obtain sigma<0.7pb (<0.7fb) (90% CL) for spin-dependent (independent) X0-proton cross section. The confidence level is from R. Bernabei, private communication, May 20, 1999.


pdgid: S030DM3
text:
SNOWDEN-IFFT 1995 look for recoil tracks in an ancient mica crystal.  Similar limits are also given for Al27 and Si28.


pdgid: S030DM3
text:
REUSSER 1991 limit here is changed from published (5) after reanalysis by authors. J.L.Vuilleumier, private communication, March 29, 1996.


pdgid: S030UDM
text:
ABE 2024A report Kamland-Zen search for de-excitation of WIMP DM bound to nucleus due to  small mass splitting with charged WIMP partner. No signal observed. Limits placed in several  parameter planes such as charged WIMP decay width vs. mass splitting (e.g. Fig. 7).


pdgid: S030UDM
text:
ARNQUIST 2024A report DAMIC-M search for MeV-scale DM scatter on e via mediator. No  signal observed. Limits placed in sigma(e) vs m plane.


pdgid: S030UDM
text:
ABE 2023A search for boosted sub-GeV DM using 0.37 Mt.y exposure of SuperK data. No  signal observed. Model dependent limits set, see Fig. 3 corrected in ABE 2023G erratum.


pdgid: S030UDM
text:
ADAMS 2023 search for inelastic DM scatter in fluorocarbons. No signal observed. Limits  placed in sigma vs. m(chi) mass splitting plane.


pdgid: S030UDM
text:
ADHIKARI 2023B search for boosted heavy photon DM in MeV range using Cosine-100. No signal  observed. Limits placed in coupling vs. mass plane for masses 1 -- 100 MeV.


pdgid: S030UDM
text:
AL-KHARUSI 2023 search for absorption of MeV-scale DM with 234.1 kg.y exposure of   Xe136, triggering beta decay. No signal observed. Limit placed in cross section vs.  mass  plane for m(chi) = 1.7 -- 11.6 MeV (see Fig. 5).


pdgid: S030UDM
text:
APRILE 2023 search for multiple scatter events from Planck scale-DM particles. No signal  observed. Limits set on sigma^SI and sigma^SD on n and p.


pdgid: S030UDM
text:
HUANG 2023 search for MeV-scale scalar DM interacting via GeV-scale dark mediator. Limits  placed on cross section vs. mass plane.


pdgid: S030UDM
text:
NING 2023A search for boosted LDM arising from eta decays which are produced in CR   events with 0.63 t.y exposure. No signal observed. Limits placed in sigma(chi N)   vs. m(chi) plane for various mediator models and branching fraction assumptions (see Fig. 2).


pdgid: S030UDM
text:
ADHIKARI 2022 search for multiple scatter of Planck scale DM on Ar using DEAP  detector. No signal observed. Limits placed in mass vs. cross section plane for m(DM): E7 -- E19 GeV.


pdgid: S030UDM
text:
ADHIKARI 2022D report search for annual modulation signal of DM in a 173 kg.yr  exposure of NaI; result consistent with both the modulation amplitude reported by  DAMA/LIBRA and no-modulation .


pdgid: S030UDM
text:
DAI 2022A search for MeV-scale exotic DM interaction with Ge; no signal observed;  limits set in m(DM) vs. cross section plane for m(DM) ~ 5 -- 60 MeV in simplified  model.


pdgid: S030UDM
text:
GU 2022 use PANDAX to search for absorption of fermionic DM in MeV range in Xe; no   signal observed; limits set in m(DM) vs. cross section plane for m(DM) ~ 30 -- 125  MeV.


pdgid: S030UDM
text:
ZHANG 2022 search for light DM scatter on e; no signal observed; limits placed in   vs. m(DM) plane for m(DM) ~ 10 -- 180 keV.


pdgid: S030UDM
text:
AKERIB 2021B place limits on 15 WIMP non-relativistic EFT couplings for m(DM): 10 -- 4000 GeV   using 3.14 kg d exposure.


pdgid: S030UDM
text:
AMARE 2021 search for WIMP annual modulation signal on NaI target in the Canfranc  Underground Laboratory (LSC). With an effective exposure of 313.95 kg y, and a sensitivity of 2.5  sigma no signal is observed. Incompatible with DAMA/LIBRA at 3.3 sigma level.


pdgid: S030UDM
text:
WANG 2021K use CDEX detector to search for WIMP dark matter scatter on Ge; no  signal observed; limits placed on 14 non-relativistic effective operators along with WIMP-pion  coupling for m(WIMP) ~ 3 -- 20 GeV.


pdgid: S030UDM
text:
AGOSTINI 2020 search for keV-MeV scale super-WIMP absorption in Ge in  GERDA; no signal; limits placed on keV-MeV scale bosonic superWIMPs in coupling vs. mass  plane.


pdgid: S030UDM
text:
ANDRIANAVALOMAHEFA 2020 search for hidden photon DM in eV range; place limits in m(DM) vs  ln(chi) plane: exclude coupling chi ~< 1E-12 for m(DM) ~ 2.5 -- 7  eV.


pdgid: S030UDM
text:
CLARK 2020 use Majorana and Xe-1-ton data to constrain superheavy multply interacting dark  matter (MIMP) in range m~ E8 -- E17 GeV depending on interaction cross section.


pdgid: S030UDM
text:
ABRAMOFF 2019 search for MeV scale DM via DM-e scattering and dark photon DM via  absorption in Si; limits set in coupling vs. m(chi) plane and on dark photon in  m(A) vs. kinetic mixing parameter plane.


pdgid: S030UDM
text:
ADHIKARI 2019 search for annual modulation signal from WIMP scatter on  NaI with 1.7 yr exposure; result consistent with both DAMA/LIBRA and null  hypothesis.


pdgid: S030UDM
text:
AMARE 2019 is ANAIS-112 search for WIMP scatter annual modulation on NaI; 157.55  kg yr exposure; result compatible with null hypothesis; confirm goal of reaching sensitivity at  3sigma to DAMA/LIBRA result in 5 years.


pdgid: S030UDM
text:
APRILE 2019 search for WIMP-pion scattering in Xe; no signal: require  sigma(chi pi) < 6.4E-10 pb for m(chi) = 30 GeV.


pdgid: S030UDM
text:
BRINGMANN 2019 derive theoretically limits on GeV and sub-GeV mass dark matter, in its high  energy component generated by interaction with cosmic rays; place limits on sigma^SI and  sigma^SD < E5 pb.


pdgid: S030UDM
text:
BRUNE 2019 examine possibility of Majoron dark matter; limits placed on Majoron mass vs.  coupling from SN1987a and nu-less double beta decay.


pdgid: S030UDM
text:
CHOI 2019 from multimessenger observation finds limit on  sigma(nu chi)/m(DM) < 5.1E-23 cm**2/GeV based on 290 TeV IceCube neutrino  event.


pdgid: S030UDM
text:
HA 2019 search for inelastic boosted MeV scale dark photon using COSINE-100 data; limits  placed in m vs. epsilon plane for various mediators.


pdgid: S030UDM
text:
KLOPF 2019 search for DM via n --> chi e+ e-; no signal: limits placed in branching  fraction vs. m(e+ e-) plane.


pdgid: S030UDM
text:
AARTSEN 2018D search for long-lived DM particles decaying chi --> nu X; no excess seen;  for DM masses above 10 TeV, excluding lifetimes shorter than E28 s.


pdgid: S030UDM
text:
ABE 2018F search for keV mass ALPs and hidden photons (HP) scatter on electrons; limits set  on mass vs. coupling.


pdgid: S030UDM
text:
AGNES 2018B search for MeV-scale DM scatter on electrons in Ar; no signal; require  sigma(chi e) < 9E-3 pb for DM form factor F(DM) = 1 and < 300 pb for F(DM)  proportional to 1/q**2 for m(chi) = 100 MeV.


pdgid: S030UDM
text:
AGNESE 2018B search for MeV scale DM via DM-e scattering and dark photon DM via  absorption in Si; limits set on MeV DM in coupling vs. m(chi) plane and on dark  photon in m(A^') vs. kinetic mixing plane.


pdgid: S030UDM
text:
AKERIB 2018A search for annual and diurnal  modulation of DM scattering rate on electrons for  recoil energy between 2 and 6 keVee; no signal found.


pdgid: S030UDM
text:
ARMENGAUD 2018 search for ALP from the Sun and galactic bosonic DM, interacting in Ge; no signal; limits set for 0.8 -- 500 keV DM particles.


pdgid: S030UDM
text:
KACHULIS 2018 search  for an excess of elastically scattered electrons above the atmospheric  neutrino background in Super-K; limits placed for simple annihilation or decay in the Sun or  galactic center producing "boosted" dark matter.


pdgid: S030UDM
text:
AGUILAR-AREVALO 2017 search for hidden photon DM scatter on Si target CCD; limit  kinetic mixing kappa < 1E-12 for m = 10 eV.


pdgid: S030UDM
text:
APRILE 2017D set limits on 14 WIMP-nucleon different interaction operators. No deviations  found using 225 live days in the 6.6 -- 240 keV recoil energy range.


pdgid: S030UDM
text:
APRILE 2017H search for keV bosonic DM via e chi --> e, looking for electronic recoils  with 224.6 live days of data and 34 kg of LXe. Limits set on chi e e coupling for m(chi) =  8 -- 125 keV.


pdgid: S030UDM
text:
APRILE 2017K search for magnetic inelastic DM via chi N --> chi^* --> chi gamma. Limits  set in DM magnetic moment vs. mass splitting plane for two DM masses corresponding to the  DAMA/LIBRA best fit values.


pdgid: S030UDM
text:
ANGLOHER 2016A require q**2 dependent scattering < 8E-3 pb for asymmetric DM  m(WIMP) = 3 GeV on CaWO(4) target. It uses a local dark matter density of 0.38 GeV/cm**3.


pdgid: S030UDM
text:
APRILE 2015 search for periodic variation of electronic recoil event rate in the data between  Feb. 2011 and Mar. 2012. No significant modulation is found for periods up to 500 days.


pdgid: S030UDM
text:
APRILE 2015A search for X0 scattering off electrons.  See their Fig. 4 for limits on  cross section through axial-vector coupling for mass(X0) between 0.6 GeV and 1 TeV.  For mass(X0)  = 2 GeV, sigma< 60 pb (90%CL) is obtained.


pdgid: S030DMA
text:
ACHARYYA 2024 search for TeV-scale wimp annihilation in dwarf spheroidals. No signal  observed. Limits placed on <> vs. m(wimp) in various annihilation channels. Quoted  limit for chi chi --> W W.


pdgid: S030DMA
text:
CAO 2024 search for superheavy WIMP annihilation in dwarf spheroidals to b bbar or tau taubar.  No signal observed. Limits set in <> vs. m(WIMP) plane. Quoted limit for b bbar  with m(WIMP) = 1 TeV.


pdgid: S030DMA
text:
CHOLIS 2024 derive limits on wimp annihilation contribution to Fermi-LAT observation of  isotropic gamma ray background. Limits set in <> vs m plane for various chi chi  annihilation channel.


pdgid: S030DMA
text:
CRNOGORCEVIC 2024 interpret published Fermi-LAT data aimed at Ursa-Major III to derive limits  on WIMP annihilation in high J-factor dwarf spheroidal. Fermi-LAT limits are recast in  <> vs m plane depend on J and on assumed annihilation channel.


pdgid: S030DMA
text:
DE-LA-TORRE-LUQUE 2024 analyze 15 years Fermi-LAT data for m(WIMP) 10 -- 300 GeV  annihilation to photons. No signal observed. Limits placed in <> vs m plane for  several models motivated by galactic center excess.


pdgid: S030DMA
text:
MANNA 2024 analyze SPT-SZ survay for 1 -- 300 GeV gamma rays from wimp annihilation in  galaxy clusters. Some slight signals observed in conflict with dwarf spheroidal searches. Limits in  <> vs m plane; quoted limit is for m(wimp) = 10 GeV in b bbar annihilation  channel.


pdgid: S030DMA
text:
MCDANIEL 2024 combined 14.3 years Fermi-LAT data from multiple dwarf spheroidals to gain  updated bounds on WIMP annihilation rates with some 2sigma excesses claimed. Reported limit is for 100 GeV WIMP mass.


pdgid: S030DMA
text:
MCDANIEL 2024 perform combined 14 year Fermi-LAT analysis of gammas from dwarf spheroidals.  New limits obtained from Fig. 6. Quoted value for m(WIMP) = 100 GeV in  b bbar and tau taubar  annihilation channels.


pdgid: S030DMA
text:
SONG 2024 use Fermi-LAT data to constrain heavy E3 -- E11 GeV DM annihilation and  decay. Limits placed in <> vs. m and lifetime vs. m planes.


pdgid: S030DMA
text:
SONG 2024A examine Fermi-LAT gamma ray data from superheavy WIMP annihilation/decay in galaxy  clusters. Limits placed in <> vs m and lifetime vs m planes for a variety of  annihilation/decay modes.


pdgid: S030DMA
text:
ZAKHAROV 2024A derive limits DM annihilation to X-rays  in the 4 -- 15 keV particle  mass range via SRG/ART-XC telescope. Limits placed in <> vs m plane. Quoted limit is  from MW halo for m = 10 keV, see Fig. 10.


pdgid: S030DMA
text:
ABBASI 2023A search for WIMP-WIMP annihilation to nu's. No signal observed. Require  <> < E-24 cm**3/s for m(chi) ~ 10 -- 10E4 GeV for  various halo profiles.


pdgid: S030DMA
text:
ABBASI 2023B search for PeV-scale WIMP-WIMP annihilation to mu or b pairs. No signal  observed. Require <> < E-22 cm**3/s for chi chi --> b bbar with  m(chi) about 1 PeV or <> < E-23 cm**3/s for chi chi --> mu+ mu- with  m(chi) about 1 PeV.


pdgid: S030DMA
text:
ABE 2023B search for WMP-WIMP annihilation to gamma in GC. No signal observed. Require  <> < 5E-28 cm**3/s for m(chi) = 1 TeV or <> <  1E-25 cm**3/s for m(chi) = 100 TeV.


pdgid: S030DMA
text:
ALBERT 2023 search for WIMP pair annihilation to gamma in galactic halo. No signal  observed. Limits placed in <> vs. mass (10 -- 100 TeV) plane for various  annihilation channels.


pdgid: S030DMA
text:
CHENG 2023A provide updated combined Fermi-LAT/DAMPE search for gamma line from WIMP  annihilation. No signal observed. Limits placed in <> vs. mass (6 -- 200 GeV)  plane for various halo profiles.


pdgid: S030DMA
text:
FOSTER 2023 search for gamma ray line in Fermi-LAT data. No signal observed. Limits placed in  <> vs. m(chi) plane. For Higgsino DM limit see Fig. 12.


pdgid: S030DMA
text:
GUO 2023 search with Five-hundred-meter Aperture Spherical Radio Telescope for synchrotron  emission radio signal of DM annihilation from dwarf spheroidal galaxy. No signal observed. Limits  set in <> vs. m(chi) plane for various annihilation final states.


pdgid: S030DMA
text:
GUO 2023A search in public IceCube data for DM annihilation to neutrinos. No signal observed.  Limits  placed in  <> vs m(chi) plane for various annihilation assumptions.


pdgid: S030DMA
text:
LAVIS 2023 search for 2HDM+S DM and generic spectra using MeerKAT. No signal observed. Limits  placed in <> vs. mass (10 -- 1000 GeV) plane for various annihilation  channels.


pdgid: S030DMA
text:
ABDALLA 2022 search for WIMP annihilation in galactic center to gamma rays using HESS; no    signal observed; limits set in mass vs <> plane for dominant annihilation to W W or    tau taubar. Limit here for tau taubar channel 0.7 TeV mass.


pdgid: S030DMA
text:
ALBERT 2022A search for secluded PeV-scale DM annihilation to four final states; no signal  detected; limits placed in <> vs. m(chi) plane for m(chi): 6 -- 6000  TeV for m(mediator) = 50, 250, and 1000 GeV.


pdgid: S030DMA
text:
CHAN 2022 derive a variety of limits on DM annihilation to various channels resulting in  X-rays from dwarf galaxy Omega Centauri. Limits are very dependent on assumed DM density and  diffusion coefficient. Quoted limit is for m(WIMP) = 100 GeV annihilating to W W with  parameters as in Fig. 4.


pdgid: S030DMA
text:
EGOROV 2022 derives limits on DM annihlation to b bbar or tau taubar via radio    signals from M31; quoted limit from b bbar channel with LOFAR telescope as main data source,  using  parameters as in Fig. 10 (green   curve) for m(chi) = 100 GeV.


