# pdgfootnote

pdgid: S126W
text:
TUMASYAN 2022AM use up to 140 fb**-1 at Ecm = 13 TeV. The off-shell Higgs boson   production in the Z Z --> 4 lepton and Z Z --> 2 lepton 2 nu decay channels and the   on-shell production in the Z Z^* --> 4 lepton (lepton = e , mu) decay channels are used  to measure the  total width. The off-shell Higgs signal strength is measured to be 0.62+0.68-0.45  without the  constraint on the ratio of the off-shell signal strengths for gluon-fusion and  gauge-boson modes.  The scenario of no off-shell contribution is excluded at 3.6 sigma. The  results are shown  in their Table 1 with other constraint scenarios and the decay widths assuming  the same coupling  modifiers for on- and off-shell couplings (g_{{p}} and g_{{d}} in their  notation). The measurement  of anomalous H V V couplings is shown in their Extended Data Table  1 and Fig. 8.


pdgid: S126W
text:
SIRUNYAN 2019BL measure the width and anomalous H V V couplings from on-shell and  off-shell production in the 4 lepton final state. Data of 80.2 fb**-1 at 13 TeV, 19.7  fb**-1 at 8 TeV, and 5.1 fb**-1 at 7 TeV are used. The total width for the SM-like  couplings is measured to be also [0.08, 9.16] MeV with 95% CL, assuming SM-like couplings for  on- and off-shells (see their Table VIII). Constraints on the total width for anomalous H V V  interaction cases are found in their Table IX. See their Table X for the Higgs boson signal  strength in the off-shell region.


pdgid: S126W
text:
AABOUD 2018BP use 36.1 fb**-1 at Ecm = 13 TeV. An observed upper limit on the  off-shell Higgs signal strength of 3.8 is obtained at 95% CL using off-shell Higgs boson  production in the Z Z --> 4 lepton and Z Z --> 2 lepton 2 nu decay channels (lepton =  e , mu). Combining with the on-shell signal strength measurements, the quoted upper limit on  the Higgs boson total width is obtained, assuming the ratios of the relevant Higgs-boson couplings  to the SM predictions are constant with energy from on-shell production to the high-mass range.


pdgid: S126W
text:
SIRUNYAN 2017AV obtain an upper limit on the width from the  distribution  in Z Z^* --> 4 lepton (lepton = e , mu) decays. Data of 35.9 fb**-1 p p  collisions at Ecm = 13 TeV is used. The expected limit is 1.60 GeV.


pdgid: S126W
text:
KHACHATRYAN 2016BA derive constraints on the total width from comparing W W^(*)()  production via on-shell and off-shell H using 4.9 fb**-1 of p p collisions at  Ecm = 7 TeV and 19.4 fb**-1 at 8 TeV.


pdgid: S126W
text:
KHACHATRYAN 2016BA combine the W W^(*)() result with Z Z^(*)() results of  KHACHATRYAN 2015BA and KHACHATRYAN 2014D.


pdgid: S126W
text:
AAD 2015BE derive constraints on the total width from comparing Z Z^(*)() and W W^(*)()  production via on-shell and off-shell H using 20.3 fb**-1 of p p collisions at  Ecm = 8 TeV.  The K factor for the background processes is assumed to be equal to that for  the signal.


pdgid: S126W
text:
KHACHATRYAN 2015AM combine gamma gamma and Z Z^* --> 4 lepton results. The expected limit is 2.3 GeV.


pdgid: S126W
text:
KHACHATRYAN 2015BA derive a lower limit on the total width from an upper limit on the decay  flight distance tau < 1.9E-13 s. 5.1 fb**-1 of p p collisions at  Ecm = 7 TeV and 19.7 fb**-1 at 8 TeV are used.


pdgid: S126W
text:
KHACHATRYAN 2015BA derive constraints on the total width from comparing Z Z^(*)()  production via on-shell and off-shell H with an unconstrained anomalous coupling. 4lepton  final states in 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at  Ecm = 8 TeV are used.


pdgid: S126W
text:
AAD 2014W use 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1 at 8 TeV.  The expected limit is 6.2 GeV.


pdgid: S126W
text:
CHATRCHYAN 2014AA use 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. The expected limit is 2.8 GeV.


pdgid: S126W
text:
KHACHATRYAN 2014D derive constraints on the total width from comparing Z Z^(*)() production via on-shell and off-shell H. 4lepton and lepton lepton nu nu final states in 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV are used.


pdgid: S126W
text:
KHACHATRYAN 2014P use 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. The expected limit is 3.1 GeV.


pdgid: S126R20
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139  fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV. SM values for the   production cross-sections are assumed. See their Fig. 2b.


pdgid: S126R21
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139  fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV. SM values for the  production cross-sections are assumed. See their Fig. 2b.


pdgid: S126R03
text:
AAD 2020F use 139 fb**-1 of p p collisions at Ecm = 13 TeV. The best-fit value  of the H --> e e branching fraction is 0.0+-1.7+-0.6E-4 for mass(H) = 125 GeV.


pdgid: S126R26
text:
AAD 2024D report combined results of ATLAS (AAD 2020AG) and CMS (TUMASYAN 2023F).  SM values for the production cross-sections are assumed.


pdgid: S126R16
text:
SIRUNYAN 2020BK search for H --> Z rho, Z --> e+ e-/mu+ mu-, rho --> pi+ pi-  with 137 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted branching fraction  is for the unpolarized decay. See their Table 3 for different polarizations.


pdgid: S126R17
text:
SIRUNYAN 2020BK search for H --> Z phi, Z --> e+ e-/mu+ mu-, phi --> K+ K-  with 137 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted branching fraction  is for the unpolarized decay. See their Table 4 for different polarizations.


pdgid: S126R18
text:
AAD 2020AE search for H --> Z eta_c with two-leptons (e+ e-/mu+ mu-) plus jet  events using 139 fb**-1 of p p collision data at Ecm = 13 TeV. The upper limit of  sigma(p p --> H).B(H --> Z eta_c) is 110 pb at 95% CL.


pdgid: S126R19
text:
TUMASYAN 2023C search for H --> Z J/psi, Z --> e+ e- or mu+ mu-, J/psi --> mu+ mu-  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted value is for the  Higgs decays for longitudinally polarized mesons. See their Table 1 for other cases.


pdgid: S126R19
text:
AAD 2020AE search for H --> Z J/psi with two-leptons (e+ e-/mu+ mu-) plus jet  events using 139 fb**-1 of p p collision data at Ecm = 13 TeV. The upper limit of  sigma(p p --> H).B(H --> Z J/psi) is 100 pb at 95% CL.


pdgid: S126R27
text:
TUMASYAN 2023C search for H --> Z psi(2S), Z --> e+ e- or mu+ mu-, psi(2S) --> mu+ mu-  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted value is for the  Higgs decays for longitudinally polarized mesons. See their Table 1 for other cases.


pdgid: S126R04
text:
AAD 2023CD search for H --> J/psi gamma, J/psi --> mu+ mu- with 138 fb**-1 of  p p collision data at Ecm = 13 TeV. SM values for the production cross-sections are  assumed.


pdgid: S126R04
text:
SIRUNYAN 2019AJ search for H --> J/psi gamma, J/psi --> mu+ mu- with 35.9 fb**-1  of p p collision data at Ecm = 13 TeV. The upper limit corresponds to 260 times the SM  prediction and by combining the KHACHATRYAN 2016B, it is 220 times the SM prediction.


pdgid: S126R04
text:
AABOUD 2018BL search for H --> J/psi gamma, J/psi --> mu+ mu- with 36.1 fb**-1  of p p collision data at Ecm = 13 TeV.


pdgid: S126R13
text:
TUMASYAN 2023C search for H --> J/psi J/psi, J/psi --> mu+ mu- with 138 fb**-1  of p p collision data at Ecm = 13 TeV. The quoted value is for the Higgs decays for  longitudinally polarized mesons. See their Table 1 for other cases.


pdgid: S126R13
text:
SIRUNYAN 2019BR search for H --> J/psi J/psi, J/psi --> mu+ mu- with 37.5 fb**-1  of p p collision data at Ecm = 13 TeV. J/psis from the Higgs decay are assumed to be  unpolarized. For fully longitudinal (transverse) polarized J/psis, limits change by  -22% (+10%).


pdgid: S126R12
text:
AAD 2023CD search for H --> psi(2S) gamma, psi(2S) --> mu+ mu- with 138 fb**-1 of  p p collision data at Ecm = 13 TeV. SM values for the production cross-sections are  assumed.


pdgid: S126R12
text:
AABOUD 2018BL search for H --> psi(2S) gamma, psi(2S) --> mu+ mu- with 36.1  fb**-1 of p p collision data at Ecm = 13 TeV.


pdgid: S126R28
text:
TUMASYAN 2023C search for H --> psi(2S) J/psi, psi(2S) --> mu+ mu-, J/psi --> mu+ mu- with  138 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted value is for the Higgs  decays for longitudinally polarized mesons. See their Table 1 for other cases.


pdgid: S126R29
text:
TUMASYAN 2023C search for H --> psi(2S) psi(2S), psi(2S) --> mu+ mu- with 138  fb**-1 of p p collision data at Ecm = 13 TeV. The quoted value is for the Higgs  decays for longitudinally polarized mesons. See their Table 1 for other cases.


pdgid: S126R05
text:
AAD 2023CD search for H --> Upsilon(1S) gamma, Upsilon(1S) --> mu+ mu- with 138  fb**-1 of p p collision data at Ecm = 13 TeV. SM values for the production cross-sections are assumed.


pdgid: S126R05
text:
AABOUD 2018BL search for H --> Upsilon(1S) gamma, Upsilon(1S) --> mu+ mu- with 36.1  fb**-1 of p p collision data at Ecm = 13 TeV.


pdgid: S126R30
text:
TUMASYAN 2023C search for H --> Upsilon(1S) Upsilon(1S), Upsilon(1S) --> mu+ mu-  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted value is for the  Higgs decays for longitudinally polarized mesons. See their Table 1 for other cases.


pdgid: S126R06
text:
AAD 2023CD search for H --> Upsilon(2S) gamma, Upsilon(2S) --> mu+ mu- with 138  fb**-1 of p p collision data at Ecm = 13 TeV. SM values for the production cross-sections are assumed.


pdgid: S126R06
text:
AABOUD 2018BL search for H --> Upsilon(2S) gamma, Upsilon(2S) --> mu+ mu- with 36.1  fb**-1 of p p collision data at Ecm = 13 TeV.


pdgid: S126R07
text:
AAD 2023CD search for H --> Upsilon(3S) gamma, Upsilon(3S) --> mu+ mu- with 138  fb**-1 of p p collision data at Ecm = 13 TeV. SM values for the production cross-sections are assumed.


pdgid: S126R07
text:
AABOUD 2018BL search for H --> Upsilon(3S) gamma, Upsilon(3S) --> mu+ mu- with 36.1  fb**-1 of p p collision data at Ecm = 13 TeV.


pdgid: S126R14
text:
TUMASYAN 2023C search for H --> Upsilon(nS) Upsilon(mS) with   Upsilon(nS) , Upsilon(mS) --> mu+ mu- (n, m = 1, 2, 3) with 138 fb**-1 of p p   collision data at Ecm = 13 TeV. The quoted value is for the Higgs decays for longitudinally   polarized mesons. See their Table 1 for other cases.


pdgid: S126R14
text:
SIRUNYAN 2019BR search for H --> Upsilon(nS) Upsilon(mS) with  Upsilon(nS),Upsilon(mS) --> mu+ mu- (n, m = 1, 2, 3) for 37.5 fb**-1 of p p  collision data at Ecm = 13 TeV. Upsilons from the Higgs decay are assumed to be  unpolarized. For fully longitudinal (transverse) polarized Upsilons, limits change by  -22% (+10%). The three Upsilon states selected in a mass range of 8.5 -- 11 GeV  are not distinguished.


pdgid: S126R33
text:
AAD 2024R use 136.3 fb**-1 of p p collision data at 13 TeV. The 95% CL upper  limit on the cross section times the branching ratio is 58 fb. The SM Higgs production cross  section of mass(H) = 125.09 GeV is assumed. See their Table 3.


pdgid: S126R09
text:
HAYRAPETYAN 2023C use 138 fb**-1 of p p collisions at Ecm = 13 TeV. The limit  constrains the Y(e mu) Yukawa coupling to sqrt(|Y(e mu)|**2 + |Y(mu e)|**2)  < 1.9E-4 at 95% CL (see their Fig. 6).


pdgid: S126R09
text:
AAD 2020F use 139 fb**-1 of p p collisions at Ecm = 13 TeV. The best-fit value  of the H --> e mu branching fraction is 0.4+-2.9+-0.3E-5 for mass(H) = 125 GeV.


pdgid: S126R09
text:
KHACHATRYAN 2016CD search for H --> e mu in 19.7 fb**-1 of p p collisions at  Ecm = 8 TeV. The limit constrains the Y(e mu) Yukawa coupling to  sqrt(|Y(e mu)|**2 + |Y(mu e)|**2) < 5.4E-4 at 95% CL  (see their Fig. 6).


pdgid: S126R10
text:
AAD 2023Q search for H --> e tau in 138 fb**-1 of p p collisions at Ecm =  13 TeV. The result is obtained from a simultaneous fit of possible H --> e tau and H --> mu tau  signals (see their Figs. 13 and 14). The limit constrains the Y(e tau) Yukawa coupling  to sqrt(|Y(e tau)|**2 + |Y(tau e)|**2) < 1.3E-3 at  95% CL (see their Fig. 15).


pdgid: S126R10
text:
AAD 2023Q search for H --> e tau in 138 fb**-1 of p p collisions at Ecm =  13 TeV. The limit constrains the Y(e tau) Yukawa coupling to sqrt(|Y(e tau)|**2 + |Y(tau e)|**2)  < 1.4E-3 at 95% CL (see their Fig. 12).


pdgid: S126R10
text:
SIRUNYAN 2021Z search for H --> e tau in 137 fb**-1 of p p collisions at  Ecm = 13 TeV. The limit constrains the Y(e tau) Yukawa coupling to  sqrt(|Y(e tau)|**2 + |Y(tau e)|**2) < 1.35E-3 at 95%  CL (see their Fig. 8).


pdgid: S126R10
text:
AAD 2020A search for H --> e tau in 36.1 fb**-1 of p p collisions at Ecm =  13 TeV. The limit constrains the Y(e tau) Yukawa coupling to sqrt(|Y(e tau)|**2 + |Y(tau e)|**2)  < 2.0E-3 at 95% CL (see their Fig. 5).


pdgid: S126R10
text:
SIRUNYAN 2018BH search for H --> e tau in 35.9 fb**-1 of p p collisions at  Ecm = 13 TeV. The limit constrains the Y(e tau) Yukawa coupling to  sqrt(|Y(e tau)|**2 + |Y(tau e)|**2) < 2.26E-3 at 95%  CL (see their Fig. 10).


pdgid: S126R10
text:
KHACHATRYAN 2016CD search for H --> e tau in 19.7 fb**-1 of p p collisions at  Ecm = 8 TeV. The limit constrains the Y(e tau) Yukawa coupling to  sqrt(|Y(e tau)|**2 + |Y(tau e)|**2) < 2.4E-3 at 95%  CL (see their Fig. 6).


pdgid: S126R02
text:
SIRUNYAN 2021Z search for H --> mu tau in 137 fb**-1 of p p collisions at  Ecm = 13 TeV. The limit constrains the Y(mu tau) Yukawa coupling to  sqrt(|Y(mu tau)|**2 + |Y(tau mu)|**2) < 1.11E-3 at  95% CL (see their Fig. 8).


pdgid: S126R02
text:
AAD 2023Q search for H --> mu tau in 138 fb**-1 of p p collisions at Ecm =   13 TeV. The result is obtained from a simultaneous fit of possible H --> e tau and H --> mu tau   signals (see their Figs. 13 and 14). The limit constrains the Y(mu tau) Yukawa coupling   to sqrt(|Y_{{mu tau}}|**2 + |Y_{{tau mu}}|**2) < 1.2E-3 at  95% CL (see  their Fig. 15).


pdgid: S126R02
text:
AAD 2023Q search for H --> mu tau in 138 fb**-1 of p p collisions at Ecm =  13 TeV. The limit constrains the Y(mu tau) Yukawa coupling to  sqrt(|Y(mu tau)|**2 + |Y(tau mu)|**2) < 1.2E-3 at 95%  CL (see their Fig. 12).


pdgid: S126R02
text:
AAD 2020A search for H --> mu tau in 36.1 fb**-1 of p p collisions at Ecm  = 13 TeV. The limit constrains the Y(mu tau) Yukawa coupling to  sqrt(|Y(mu tau)|**2 + |Y(tau mu)|**2) < 1.5E-3 at 95%  CL (see their Fig. 5).


pdgid: S126R02
text:
AAIJ 2018AM search for H --> mu tau in 2.0 fb**-1 of p p collisions at Ecm  = 8 TeV. The limit constrains the Y(mu tau) Yukawa coupling to  sqrt(|Y(mu tau)|**2 + |Y(tau mu)|**2) < 1.7E-2 at 95%  CL assuming SM production cross sections.


pdgid: S126R02
text:
SIRUNYAN 2018BH search for H --> mu tau in 35.9 fb**-1 of p p collisions at  Ecm = 13 TeV. The limit constrains the Y(mu tau) Yukawa coupling to  sqrt(|Y(mu tau)|**2 + |Y(tau mu)|**2) < 1.43E-3 at  95% CL (see their Fig. 10).


pdgid: S126R02
text:
KHACHATRYAN 2015Q search for H --> mu tau with tau decaying electronically or hadronically in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. The fit gives B(H --> mu tau) = (0.84+0.39-0.37)% with a significance of 2.4 sigma.


pdgid: S126R01
text:
AAD 2023A report the combined results of 7, 8 (AAD 2015CX) and 13 TeV assuming the   Standard Model cross section (mass(H) = 125 GeV). See their Table 1 and Fig. 3.


pdgid: S126R01
text:
AAD 2023A report the combined results using 139 fb**-1 of data at Ecm = 13 TeV,    where H decaying to invisible final states in VBF (AAD 2022P), Z H, Z --> e e , mu mu    (AAD 2022D), p p --> t tbar H (AAD 2023AF), VBF+gamma (AAD 2022S) and    gluon-fusion production with an energetic jet (AAD 2021F) assuming the Standard Model cross    section (mass(H) = 125 GeV). See their Table 1 and Fig. 3.


pdgid: S126R01
text:
AAD 2023AF search for p p --> t tbar H with H decaying to invisible final states   using 139 fb**-1 of data. The quoted limit on the branching ratio is given for mass(H) = 125   GeV and assumes the Standard Model cross section. See their Table 3 for different decay topologies.


pdgid: S126R01
text:
TUMASYAN 2023BA search for H decaying to invisible final states produced in association  with a t tbar or a V, which decay to a fully hadronic final state. 138 fb**-1 of data  is used. The quoted limit on the branching ratio is given for mass(H) = 125 GeV and assumes the  Standard Model cross section. See their Fig. 6 for the results of individual topologies.


pdgid: S126R01
text:
TUMASYAN 2023BA report the combined results of 7, 8, and 13 TeV assuming the Standard Model  cross section (mass(H) = 125 GeV). They combine results from TUMASYAN 2022G, SIRUNYAN 2021A,  SIRUNYAN 2021B, TUMASYAN 2021D, SIRUNYAN 2020AH, KHACHATRYAN 2017F,  CHATRCHYAN 2014B as shown in their Table 8. See their Fig. 7 and Table 9 for the results of  individual topologies.


pdgid: S126R01
text:
AAD 2022D search for H decaying to invisible final states associated with a Z  decaying e e / mu mu using 139 fb**-1 at 13 TeV. The limit is obtained for mass(H) = 125  GeV and assuming the SM Z H production cross section. The branching ratio is obtained to be  (0.3+-9.0)%.


pdgid: S126R01
text:
AAD 2022P search for p p --> q q H X (VBF) with H decaying to invisible final  states using 139 fb**-1 of data. The quoted limit on the branching ratio is given for mass(H)  = 125 GeV and assumes the Standard Model cross section.


pdgid: S126R01
text:
AAD 2022S observe electroweak Z(--> nu nu)gamma+2jets production process with 139  fb**-1 of data. This result is applicable to search for p p --> q q H gamma X  (VBF+gamma) with H decaying to invisible final states. The quoted limit on the branching  ratio is given for mass(H) = 125 GeV and assumes the Standard Model cross section.


pdgid: S126R01
text:
ATLAS 2022 report the combined results using 139 fb**-1 of data at Ecm = 13 TeV,  where H decaying to invisible final states in VBF (AAD 2022P), and Z H, Z --> e e , mu mu    (AAD 2022D), assuming kappa(V) <= 1 and B(undetected) >= 0.


pdgid: S126R01
text:
CMS 2022 report the combined results using (a part of) 138 fb**-1 of data at Ecm =  13 TeV, where H decaying to invisible final states in VBF (SIRUNYAN 2019BO),    associated  with an energetic jet or a V(--> q qbar ) (TUMASYAN 2021D), and Z H,    Z --> e e , mu mu   (SIRUNYAN 2021A) and assuming kappa(V) <= 1 and  B(undetected) >= 0.


pdgid: S126R01
text:
TUMASYAN 2022G combine 13 TeV 101 fb**-1 results with 8 TeV (KHACHATRYAN 2017F) and  other 13 TeV (KHACHATRYAN 2017F for 2015 and SIRUNYAN 2019BO for 2016) for H    decaying to invisible final states with VBF topology. The quoted limit on the branching ratio is    given for mass(H) = 125.38 GeV and assumes the Standard Model production rates. The branching    ratio is obtained to be 0.086+0.054-0.052. See their Figs. 11 and 12.


pdgid: S126R01
text:
TUMASYAN 2022G search for p p --> q q H X (VBF) with H decaying to invisible final   states using 101 fb**-1 of data (2017 and 2018). The quoted limit on the branching ratio is   given for mass(H) = 125.38 GeV and assumes the Standard Model cross section. See their Figs. 11  and 12.


pdgid: S126R01
text:
AAD 2021F search for an invisibly decaying Higgs boson with an energetic jet (pT  > 150 GeV) and missing transverse momentum (> 200 GeV) in 139 fb**-1 at Ecm =  13 TeV. The quoted limit on the branching ratio is given for mass(H) = 125 GeV.


pdgid: S126R01
text:
SIRUNYAN 2021A search for H decaying to invisible final states associated with a Z  decaying e e/mu mu using 137 fb**-1 at 13 TeV. The limit is obtained for mass(H) =  125 GeV and assuming the SM Z H production cross section.


pdgid: S126R01
text:
TUMASYAN 2021D search for H decaying to invisible final states associated with an  energetic jet or a V, V --> q qbar using 101 fb**-1 at 13 TeV and the result is  combined with SIRUNYAN 2018S.


pdgid: S126R01
text:
AABOUD 2019AI search for p p --> q q H X (VBF) with H decaying to invisible final  states using 36.1 fb**-1 of data. The quoted limit on the branching ratio is given for  mass(H) = 125 GeV and assumes the Standard Model rates for VBF and gluon-fusion production.


pdgid: S126R01
text:
AABOUD 2019AL combine results of H decaying to invisible final states with  VBF(AABOUD 2019AI), Z H, and W H productions (AABOUD 2018, AABOUD 2018CA), which  use 36.1 fb**-1 of data at 13 TeV. The quoted limit is given for mass(H) = 125 GeV and  assumes the Standard Model rates for gluon fusion, VBF, Z H, and W H productions.


pdgid: S126R01
text:
AABOUD 2019AL combine results of 7, 8 (AAD 2015CX), and 13 TeV for H decaying to  invisible final states.


pdgid: S126R01
text:
SIRUNYAN 2019BO search for p p --> q q H X (VBF) with H decaying to invisible final  states using 35.9 fb**-1 of data. The quoted limit on the branching ratio is given for  mass(H) = 125.09 GeV and assumes the Standard Model production rates.


pdgid: S126R01
text:
SIRUNYAN 2019BO combine the VBF channel with results of other 13 TeV analyses: SIRUNYAN 2018BV  and SIRUNYAN 2018S. The quoted limit on the branching ratio is given for mass(H) = 125.09  GeV and assumes the Standard Model production rates.


pdgid: S126R01
text:
SIRUNYAN 2019BO combine 13 TeV 35.9 fb**-1 results with 7, 8, 13 TeV (KHACHATRYAN 2017F) for  H decaying to invisible final states. The quoted limit on the branching ratio is given for  mass(H) = 125.09 GeV and assumes the Standard Model production rates. The branching ratio is  obtained to be 0.05+-0.03 (stat) +-0.07(syst).


pdgid: S126R01
text:
AABOUD 2018 search for p p --> H Z X, Z --> e e , mu mu with H decaying to  invisible final states in 36.1 fb**-1 at Ecm = 13 TeV. The quoted limit on the branching  ratio is given for mass(H) = 125 GeV and assumes the Standard Model rate for H Z production.


pdgid: S126R01
text:
AABOUD 2018CA search for H decaying to invisible final states using W H, and Z H  productions, where W and Z hadronically decay. The data of 36.1 fb**-1 at Ecm =  13 TeV is used. The quoted limit assumes SM production cross sections with combining the  contributions from W H, Z H, ggF and VBF production modes.


pdgid: S126R01
text:
SIRUNYAN 2018BV search for H decaying to invisible final states associated with a Z,  Z --> lepton lepton using 35.9 fb**-1 at 13 TeV.The limit is obtained for mass(H) = 125  GeV and assuming the SM Z H production cross section.


pdgid: S126R01
text:
SIRUNYAN 2018S search for H decaying to invisible final states associated with an  energetic jet or a V, V --> q qbar using 35.9 fb**-1 at 13 TeV.


pdgid: S126R01
text:
AABOUD 2017BD search for H decaying to invisible final states with >=1 jet and VBF  events using 3.2 fb**-1 of p p collisions at Ecm = 13 TeV. A cross-section ratio  R**miss is used in the measurement. The quoted limit is given for mass(H) =  125 GeV.


pdgid: S126R01
text:
KHACHATRYAN 2017F search for H decaying to invisible final states with gluon fusion,  VBF, Z H, and W H productions using 2.3 fb**-1 of p p collisions at Ecm = 13  TeV, 19.7 fb**-1 at 8 TeV, and 5.1 fb**-1 at 7 TeV. The quoted limit is given for mass(H)  = 125 GeV and assumes the Standard Model rates for gluon fusion, VBF, Z H, and W H  productions.


pdgid: S126R01
text:
AAD 2016AF search for p p --> q q H X (VBF) with H decaying to invisible final  states in 20.3 fb**-1 at Ecm = 8 TeV. The quoted limit on the branching ratio is given  for mass(H) = 125 GeV and assumes the Standard Model rates for VBF and gluon-fusion production.


pdgid: S126R01
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The branching  fraction of decays into BSM particles that are invisible or into undetected decay modes is measured  for mass(0) = 125.09 GeV.


pdgid: S126R01
text:
AAD 2015BD search for p p --> H W X and p p --> H Z X with W or Z decaying  hadronically and H decaying to invisible final states using data at Ecm = 8 TeV. The  quoted limit is given for mass(H) = 125 GeV, assumes the Standard Model rates for the production  processes and is based on a combination of the contributions from H W, H Z and the  gluon-fusion process.


pdgid: S126R01
text:
AAD 2015CX search for H decaying to invisible final states with VBF, Z H, and W H  productions using 20.3 fb**-1 at 8 TeV, and 4.7 fb**-1 at 7 TeV. The quoted limit is given  for mass(H) = 125.36 GeV and assumes the Standard Model rates for gluon fusion, VBF, Z H, and  W H productions. The upper limit is improved to 0.23 by adding the measured visible decay rates.


pdgid: S126R01
text:
AAD 2014O search for p p --> H Z X, Z --> lepton lepton, with H decaying to invisible final states in 4.5 fb**-1 at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The quoted limit on the branching ratio is given for mass(H) = 125.5 GeV and assumes the Standard Model rate for H Z production.


pdgid: S126R01
text:
CHATRCHYAN 2014B search for p p --> H Z X, Z --> lepton lepton and Z --> b bbar, and also p p --> q q H X with H decaying to invisible final states using data at Ecm = 7 and 8 TeV. The quoted limit on the branching ratio is obtained from a combination of the limits from H Z and q q H. It is given for mass(H) = 125 GeV and assumes the Standard Model rates for the two production processes.


pdgid: S126R01
text:
CHATRCHYAN 2014B search for p p --> H Z X with H decaying to invisible final states and Z --> lepton lepton in 4.9 fb**-1 at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV, and also with Z --> b bbar in 18.9 fb**-1 at Ecm = 8 TeV. The quoted limit on the branching ratio is given for mass(H) = 125 GeV and assumes the Standard Model rate for H Z production.


pdgid: S126R01
text:
CHATRCHYAN 2014B search for p p --> q q H X (vector boson fusion) with H decaying to invisible final states in 19.5 fb**-1 at Ecm = 8 TeV. The quoted limit on the branching ratio is given for mass(H) = 125 GeV and assumes the Standard Model rate for q q H production.


pdgid: S126R15
text:
AAD 2024BH search for H decaying to an invisible final state plus a gamma in the VBF  and H Z production using 139 fb**-1 data at Ecm = 13 TeV. The invisible state is  called a dark photon. The quoted limit on the branching ratio is given for mass(H) = 125 GeV  assuming the Standard Model rates. The 95% CL upper limits on the branching ratio for the VBF  and H Z production are 1.8% and 2.3%, respectively. See their Fig. 3(a).


pdgid: S126R15
text:
SIRUNYAN 2021L search for H decaying to an invisible final state plus a gamma in the   VBF production using 130 fb**-1 data at Ecm = 13 TeV. The invisible state is called a   dark photon. The quoted limit on the branching ratio is given for mass(H) = 125 GeV assuming the   Standard Model rates.


pdgid: S126R15
text:
SIRUNYAN 2019CG search for p p --> H Z, Z --> e e , mu mu with H decaying to     invisible final states plus a gamma in 137 fb**-1 at Ecm = 13 TeV. The quoted  limit    on the branching ratio is given for mass(H) = 125 GeV assuming the Standard Model rate  for  H Z   production and is obtained in the context of a theoretical model, where the  undetected  (invisible)  particle is massless.


pdgid: S126SA
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139   fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV. The Higgs production   cross-sections, branching fractions and several ratios are found in their Figs. 2 and 3.


pdgid: S126SA
text:
CMS 2022 report combined results (see their Extended Data Table 2) using 138 fb**-1 of   data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV. Signal strengths for production modes   and decay channels are found in their Fig. 2.


pdgid: S126SA
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The signal  strengths for individual production processes are 1.03+0.16-0.14 for gluon fusion, 1.18+0.25-0.23  for vector boson fusion, 0.89+0.40-0.38 for W H production, 0.79+0.38-0.36 for Z H  production, and 2.3+0.7-0.6 for t tbar H production.


pdgid: S126SA
text:
AAD 2016AN: The uncertainties represent statistics, experimental systematics, and added in quadrature theory  systematics on the background and  on the signal. The quoted signal strengths  are given for mass(H) = 125.09 GeV. In the fit, relative branching ratios and relative production  cross sections are fixed to those in the Standard Model.


pdgid: S126SA
text:
AALTONEN 2013M combine all Tevatron data from the CDF and D0 Collaborations with up to 10.0 fb**-1 and 9.7 fb**-1,  respectively, of p pbar collisions at Ecm = 1.96 TeV. The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126SA
text:
AAD 2020 combine results of up to 79.8 fb**-1 of data at Ecm = 13 TeV, assuming  mass(H) = 125.09 GeV: gamma gamma, Z Z^*, W W^*, tau tau, b bbar, mu mu,  invisible, and off-shell analyses (see their Table I). The signal strengths for individual  production processes are 1.04+-0.09 for gluon fusion, 1.21+0.24-0.22 for vector boson  fusion, 1.30+0.40-0.38 for W H production, 1.05+0.31-0.29 for Z H production,  and 1.21+0.26-0.24 for t tbar H+t H production (see their Fig. 2 and Table IV).  Several results with the simplified template cross section and kappa-frameworks are  presented: see their Figs. 9 -- 11, Figs 20, 21 and Table VIII for stage-1 simplified  template cross sections, their Figs. 12 -- 17 and Tables X-XII for the  kappa-framework.


pdgid: S126SA
text:
SIRUNYAN 2019AT combine results of 35.9 fb**-1 of data at Ecm = 13 TeV, assuming  mass(H) = 125.09 GeV. The signal strengths for individual production processes are 1.22+0.14-0.12 for  gluon fusion, 0.73+0.30-0.27 for vector boson fusion, 2.18+0.58-0.55 for W H  production, 0.87+0.44-0.42 for Z H production, and 1.18+0.30-0.27 for t tbar H  production. Several results with the simplified template cross section and kappa-frameworks  are presented: see their Fig. 8 and Table 5 for stage-0 simplified template cross sections, their  Figs. 9 -- 18 and Tables 7 -- 11 for the kappa-framework.


pdgid: S126SA
text:
SIRUNYAN 2019BA measure differential cross sections for the Higgs boson transverse momentum,  the number of jets, the rapidity of the Higgs boson and the transverse momentum of the leading jet  using 35.9 fb**-1 of data at Ecm = 13 TeV with H --> gamma gamma, H --> Z Z^*,  and H --> b bbar. The total cross section for Higgs boson production is measured to be 61.1+-6.0+-3.7 pb  using H --> gamma gamma and H --> Z Z^* channels. Several coupling measurements in the  kappa-framework are performed.


pdgid: S126SA
text:
AAD 2016K use up to 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and up to 20.3  fb**-1 at Ecm = 8 TeV.  The third uncertainty in the measurement is theory systematics.   The signal strengths for individual production modes are 1.23+-0.14+0.09-0.08+0.16-0.12 for  gluon fusion, 1.23+0.28-0.27+0.13-0.12+0.11-0.09  for vector boson fusion, 0.80+0.31-0.30+-0.17+0.10-0.05  for W / Z H production, and  1.81+0.52-0.50+0.58-0.55+0.31-0.12 for t tbar H  production. The quoted signal strengths are given for mass(H) = 125.36 GeV.


pdgid: S126SA
text:
AAD 2015P measure total and differential cross sections of the process p p --> H X at  Ecm = 8 TeV with 20.3 fb**-1. gamma gamma and 4lepton final states are used.  CS(p p --> H X) = 33.0+-5.3+-1.6 pb is given. See their Figs. 2 and 3 for  data on  differential cross sections.


pdgid: S126SA
text:
KHACHATRYAN 2015AM use up to 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and up  to 19.7 fb**-1 at Ecm = 8 TeV.  The third uncertainty in the measurement is theory  systematics.  Fits to each production mode give the value of 0.85+0.19-0.16 for gluon fusion,  1.16+0.37-0.34 for  vector boson fusion, 0.92+0.38-0.36 for W H, Z H   production, and 2.90+1.08-0.94 for  t tbar H production.


pdgid: S126SA
text:
AAD 2013AK use 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and 20.7 fb**-1 at Ecm = 8 TeV. The combined signal strength is based on the gamma gamma, Z Z^* --> 4 lepton, and W W^* --> lepton nu lepton nu channels. The quoted signal strength is given for mass(H) = 125.5 GeV. Reported statistical error value modified following private communication with the experiment.


pdgid: S126SA
text:
AALTONEN 2013L combine all CDF results with 9.45 -- 10.0 fb**-1 of p pbar collisions at Ecm = 1.96 TeV.  The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126SA
text:
ABAZOV 2013L combine all D0 results with up to 9.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV.  The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126SA
text:
AAD 2012AI obtain results based on 4.6 -- 4.8 fb**-1 of p p collisions at Ecm = 7 TeV and 5.8 -- 5.9 fb**-1 at Ecm = 8 TeV. An excess of events over background with a local significance of 5.9 sigma is observed at mass(H) = 126 GeV. The quoted signal strengths are given for mass(H) = 126 GeV. See also AAD 2012DA.


pdgid: S126SA
text:
CHATRCHYAN 2012N obtain results based on 4.9 -- 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 5.1 -- 5.3 fb**-1 at Ecm = 8 TeV. An excess of events over background with a local significance of 5.0sigma is observed at about mass(H) = 125 GeV. The combined signal strength is based on the gamma gamma, Z Z^*, W W^*, tau+ tau-, and b bbar channels.  The quoted signal strength is given for mass(H) = 125.5 GeV. See also CHATRCHYAN 2013Y.


pdgid: S126SWW
text:
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb**-1  of  data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV. See their Fig. 2 right.


pdgid: S126SWW
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The signal  strengths for individual production processes are 0.84+-0.17 for gluon fusion, 1.2+-0.4  for vector boson fusion, 1.6+1.2-1.0 for W H production, 5.9+2.6-2.2 for Z H  production, and 5.0+1.8-1.7 for t tbar H production.


pdgid: S126SWW
text:
AAD 2016AN:  In the fit, relative production cross sections are fixed to those in the  Standard Model. The quoted signal strength is given for mass(H) = 125.09 GeV.


pdgid: S126SWW
text:
HAYRAPETYAN 2024AG search for the anomalous couplings of the Higgs boson to vector bosons,  including CP violation effects using H --> W W^* --> e nu mu nu decay channel (lepton  = e , mu) with 138 fb**-1 at Ecm = 13 TeV. The anomalous HVV and Hgg coupling  parameters are given in their Table 7. The data constrain the SMEFT Higgs and Warsaw bases coupling  parameters as shown in their Tables 8, 9 and Fig. 12.


pdgid: S126SWW
text:
AAD 2023AP measure cross-sections times the H --> W W^* branching fraction in the H --> W W^* --> e nu mu nu   channel using 139 fb**-1 of p p collisions at Ecm = 13 TeV:   sigma(ggF)xB(H --> W W^*) = 12.0+-1.4 pb,   sigma(VBF)xB(H --> W W^*) = 0.75+0.19-0.16 pb, and   sigma(ggF+VBF)xB(H --> W W^*) = 12.3+-1.3 pb. The results are   given for mass(H) = 125.09 GeV. Measured cross sections and ratios to the SM predictions in the   reduced stage-1.2 (see their Fig. 5) simplified template cross section framework are shown in their   Table VII and Fig. 15.


pdgid: S126SWW
text:
AAD 2023BV measure fiducial total and differential cross sections of VBF process at Ecm  = 13 TeV with 139 fb**-1 using H --> W W^* --> e nu mu nu. The measured total fiducial  cross section is 1.68+-0.33(stat)+-0.23(syst) fb in their fiducial region (Table II and  Section V). See their Fig. 9 for the comparison with theory predictions. The fiducial differential  cross sections are shown in their Figs. 11, 12, and 13. Wilson coefficients in the Warsaw basis at  95% confidence interval are measured; see their Table V and Fig. 16.


pdgid: S126SWW
text:
TUMASYAN 2023W measure Higgs production rates with H --> W W^* at Ecm = 13 TeV    with 138  fb**-1 data. The quoted results are given for mass(H) = 125.38 GeV.


pdgid: S126SWW
text:
The quoted global signal strength is obtained assuming the relative ratios of different Higgs  production modes fixed to the SM values.


pdgid: S126SWW
text:
The 4 signal strengths for gluon-fusion (ggF), VBF, W H and Z H modes are fit assuming t tbar H  and  b bbar H fixed to the SM values.


pdgid: S126SWW
text:
Measured cross sections and ratios to the SM predictions in the reduced stage-1.2 (see their Fig.  17) simplified template cross section framework (6 ggF, 4 VBF, and 4 V H) are shown in their  Table 18 and Fig. 26.


pdgid: S126SWW
text:
AAD 2022V probe the Higgs couplings to longitudinally and transversely polarized W and   Z using VBF (H --> W W^* --> e nu mu nu plus two jets) with 36.1 fb**-1 of data at    Ecm = 13 TeV. The ratios of the polarization-dependent couplings g(H V_L V_L) and   g(H V_T V_T) to the Higgs-V coupling predicted by the SM, a_{{L}} =   g(H V_L V_L)/g( HVV)**SM and a_{{T}} = g(H V_T V_T)/g( HVV)**SM are    measured to be 0.91+0.10-0.18+0.09-0.17 and 1.2+-0.4+0.2-0.3, respectively, assuming  the standard H g g coupling. These   measurements are translated into pseudo-observables of  kappa_{{VV}} and epsilon_{{VV}}:   kappa_{{VV}} = 0.91+0.10-0.18+0.09-0.17 and epsilon_{{VV}}  = 0.13+0.28-0.20+0.08-0.10,   where kappa_{{VV}} = 1 and epsilon_{{VV}} = 0 for the SM. See  their Tables 9 and 10.


pdgid: S126SWW
text:
AABOUD 2019F measure cross-sections times the H --> W W^* branching fraction in the  H --> W W^* --> e nu mu nu channel using 36.1 fb**-1 of p p collisions at Ecm =  13 TeV: sigma(ggF)xB(H --> W W^*) = 11.4+1.2-1.1+1.8-1.7 pb and  sigma(VBF)xB(H --> W W^*) = 0.50+0.24-0.22+-0.17 pb.


pdgid: S126SWW
text:
AAD 2019A use 36.1 fb**-1 data at 13 TeV. The cross section times branching fraction  values are measured to be 0.67+0.31-0.27+0.18-0.14 pb for W H, H --> W W^* and  0.54+0.31-0.24+0.15-0.07 pb for Z H, H --> W W^*.


pdgid: S126SWW
text:
SIRUNYAN 2019AX measure the signal strengths, cross sections and so on using gluon fusion,  VBF and V H production processes with 35.9 fb**-1 of data. The quoted signal strength is  given for mass(H) = 125.09 GeV. Signal strengths for each production process is found in their  Fig. 9. Measured cross sections and ratios to the SM predictions in the stage-0 simplified template  cross section framework are shown in their Fig. 10. kappa_{{F}} = 1.52+0.48-0.41 and  kappa_{{V}} = 1.10+-0.08 are obtained (see their Fig. 11 (right)).


pdgid: S126SWW
text:
AAD 2016AO measure fiducial total and differential cross sections of gluon fusion process at  Ecm = 8 TeV with 20.3 fb**-1 using H --> W W^* --> e nu mu nu. The measured fiducial  total cross section is 36.0+-9.7 fb in their fiducial region (Table 7). See their Fig. 6 for  fiducial differential cross sections. The results are given for mass(H) = 125 GeV.


pdgid: S126SWW
text:
AAD 2016K use up to 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and up to 20.3  fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.36 GeV.


pdgid: S126SWW
text:
AAD 2015AA use 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1  at Ecm = 8 TeV. The signal strength for the gluon fusion and vector boson fusion mode is   1.02+-0.19+0.22-0.18 and 1.27+0.44-0.40+0.30-0.21, respectively. The quoted signal  strengths are given for mass(H) = 125.36  GeV.


pdgid: S126SWW
text:
AAD 2015AQ use 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1  at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.36 GeV.


pdgid: S126SWW
text:
AAD 2015AQ combine their result on W / Z H production with the results of AAD 2015AA (gluon  fusion and vector boson fusion, slightly updated). The quoted signal strength is given for  mass(H) = 125.36 GeV.


pdgid: S126SWW
text:
CHATRCHYAN 2014G use 4.9 fb**-1 of p p collisions at Ecm = 7 TeV and 19.4 fb**-1 at Ecm = 8 TeV. The last uncertainty in the measurement is theory systematics. The quoted signal strength is given for mass(H) = 125.6 GeV.


pdgid: S126SWW
text:
AAD 2013AK use 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and 20.7 fb**-1 at Ecm = 8 TeV.  The quoted signal strength is given for mass(H) = 125.5 GeV. Superseded by AAD 2015AA.


pdgid: S126SWW
text:
AAD 2012AI obtain results based on 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and 5.8 fb**-1 at Ecm = 8 TeV. The quoted signal strengths are given for mass(H) = 126 GeV. See also AAD 2012DA.


pdgid: S126SWW
text:
CHATRCHYAN 2012N obtain results based on 4.9 fb**-1 of p p collisions at Ecm = 7 TeV and 5.1 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.5 GeV. See also CHATRCHYAN 2013Y.


pdgid: S126SZZ
text:
AAD 2020AQ perform analyses using H --> Z Z^* --> 4 lepton  (lepton = e , mu)   with data of 139 fb**-1 at Ecm = 13 TeV. Results are given for  mass(H) = 125 GeV.


pdgid: S126SZZ
text:
AAD 2020AQ measured the inclusive cross section  times branching ratio for H --> Z Z^*   decay (|y(H)| < 2.5) to be 1.34+-0.12 pb  (with 1.33+-0.08 pb expected in   the SM).


pdgid: S126SZZ
text:
AAD 2016AN: In the fit, relative production cross sections are fixed to those in the Standard  Model. The quoted signal strength is given for mass(H) = 125.09 GeV.


pdgid: S126SZZ
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The signal  strengths for individual production processes are 1.13+0.34-0.31 for gluon fusion and 0.1+1.1-0.6  for vector boson fusion.


pdgid: S126SZZ
text:
AAD 2024AQ measure fiducial and total cross sections at Ecm = 13.6 TeV with 29.0  fb**-1 data. The quoted results are given for mass(H) = 125.09 GeV. The inclusive fiducial  cross section is 2.80+-0.74 fb with their defined fiducial region (see their Table 5), where  3.67+-0.19 fb is expected in the SM. Assuming SM values for the acceptance and the branching  fraction, the total cross section is 46+-12 pb, where 59.9+-2.6 pb is expected in the SM.


pdgid: S126SZZ
text:
HAYRAPETYAN 2023 measure the cross sections for p p --> H --> Z Z^* --> 4 lepton    (lepton = e , mu) using 138 fb**-1 at Ecm = 13 TeV. They give sigma =   2.73+-0.22(stat) +-0.15(syst) fb  in their fiducial region (see their Section5 and Table   2), where 2.86+-0.15 fb is expected in  the Standard Model for mass(H) = 125.38 GeV. 26   differential and 6 double-differential cross  sections are given; see their Figs. 6-23 and 24-25.


pdgid: S126SZZ
text:
SIRUNYAN 2021AE obtains constraints on anomalous couplings to vector bosons (W, Z,  and gluon) and top quark using H --> Z Z^* --> 4 lepton (lepton = e , mu) with data of  137 fb**-1 at Ecm = 13 TeV. Their Table 5 and Figs 14 -- 17 show (effective)  couplings to gluon and top with combining gluon fusion, t tbar H and t H production  channels and the result of t tbar H, H --> gamma gamma (SIRUNYAN 2020AS). Their  Tables 6 -- 9 and Figs 18 -- 22 show couplings to W and Z for different  assumptions and bases (Higgs and Warsaw).


pdgid: S126SZZ
text:
SIRUNYAN 2021S measure cross sections with the H --> Z Z^* --> 4 lepton (lepton =  e , mu) channel using 137 fb**-1 data at Ecm = 13 TeV. Results are given for  mass(H) = 125.38 GeV. The signal strengths for individual production processes in their Table 4.  Cross sections are given in their Table 6 and Fig. 14, which are based on the simplified template  cross section framework (reduced stage-1.2).


pdgid: S126SZZ
text:
AAD 2020AQ present several results for the  channel H --> Z Z^* --> 4 lepton   (lepton = e , mu) with the  simplified template  cross section with   kappa-frameworks and the effective field theory  (EFT) approach; see  their Table 8 and  Fig.  10 for simplified template cross sections. kappa_{{V}}  = 1.02+-0.06  and kappa_{{F}} =  0.88+-0.16  are obtained, see their Fig. 12 for the   kappa-framework. See their  Tables 9 and 10 and  Figs. 16 -- 18 for the EFT-framework.


pdgid: S126SZZ
text:
AAD 2020BA measure the cross section for p p --> H --> Z Z^* --> 4 lepton (lepton =  e , mu) using 139 fb**-1 at Ecm = 13 TeV. They give sigma.B =  3.28+-0.30+-0.11 fb in their fiducial region, where 3.41+-0.18 fb is expected in the  Standard Model for mass(H) = 125 GeV. Various differential cross sections are also given; see  their Figs. 19-39. Constraints on Yukawa couplings for bottom and charm quarks are given in their  Table 9 and Fig. 41.


pdgid: S126SZZ
text:
AABOUD 2019N measure the spectrum  of the four-lepton invariant mass m(4 lepton)  (lepton = e or mu) using 36.1 fb**-1 of data at Ecm = 13 TeV. The quoted  signal strength upper limit is obtained from 180 GeV < m(4 lepton) < 1200 GeV.


pdgid: S126SZZ
text:
AABOUD 2018AJ perform analyses using H --> Z Z^* --> 4 lepton (lepton = e , mu)  with data of 36.1 fb**-1 at Ecm = 13 TeV. Results are given for mass(H) = 125.09 GeV.  The inclusive cross section times branching ratio for H --> Z Z^* decay  (|eta(H)| < 2.5) is measured to be 1.73+0.26-0.24 pb (with  1.34+0.09-0.09 pb expected in the SM).


pdgid: S126SZZ
text:
AABOUD 2018BP measure an off-shell Higgs boson production using Z Z --> 4 lepton and   Z Z --> 2 lepton 2 nu (lepton = e , mu) decay channels with 36.1 fb**-1 of data at  Ecm = 13 TeV. The quoted signal strength upper limit is obtained from a combination of these  two channels, where 220 GeV < m(4 lepton) < 2000 GeV for Z Z --> 4 lepton  and 250 GeV < m(T)**ZZ < 2000 GeV for Z Z --> 2 lepton 2 nu (m(T)**ZZ  is defined in their Section 5). See their Table 2 for each measurement.


pdgid: S126SZZ
text:
SIRUNYAN 2017AV use 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. The quoted  signal strength, obtained from the analysis of H --> Z Z^* --> 4 lepton (lepton = e , mu)  decays, is given for mass(H) = 125.09 GeV. The signal strengths for different production modes  are given in their Table 3. The fiducial and differential cross sections are shown in their Fig. 10.


pdgid: S126SZZ
text:
KHACHATRYAN 2016AR use data of 5.1 fb**-1 at Ecm = 7 TeV and 19.7 fb**-1 at 8  TeV. The fiducial cross sections for the production of 4 leptons via H --> 4 lepton decays are  measured to be 0.56+0.67-0.44+0.21-0.06 fb at 7 TeV and 1.11+0.41-0.35+0.14-0.10 fb at  8 TeV in their fiducial region (Table 2). The differential cross sections at Ecm = 8 TeV are  also shown in Figs. 4 and 5. The results are given for mass(H) = 125 GeV.


pdgid: S126SZZ
text:
AAD 2015F use 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.36 GeV. The signal strength for the gluon fusion production mode is 1.66+0.45-0.41+0.25-0.15, while the signal strength for the vector boson fusion production mode is 0.26+1.60-0.91+0.36-0.23.


pdgid: S126SZZ
text:
AAD 2014AR measure the cross section for p p --> H --> Z Z^* --> 4 lepton (lepton =  e , mu) using 20.3fb**-1 at Ecm = 8 TeV. They give sigma.B = 2.11+0.53-0.47+-0.08  fbin their fiducial region, where 1.30+-0.13 fb is expected in the Standard Model for  mass(H)= 125.4 GeV. Various differential cross sections are also given; see their Fig. 2.


pdgid: S126SZZ
text:
CHATRCHYAN 2014AA use 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.6 GeV. The signal strength for the gluon fusion and t tbar H production mode is 0.80+0.46-0.36, while the signal strength for the vector boson fusion and W H, Z H production mode is 1.7+2.2-2.1.


pdgid: S126SZZ
text:
AAD 2013AK use 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and 20.7 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.5 GeV.


pdgid: S126SZZ
text:
CHATRCHYAN 2013J obtain results based on Z Z --> 4 lepton final states in 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 12.2 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given  for mass(H) = 125.8 GeV. Superseded by CHATRCHYAN 2014AA.


pdgid: S126SZZ
text:
AAD 2012AI obtain results based on 4.7 -- 4.8 fb**-1 of p p collisions at Ecm = 7 TeV and 5.8 fb**-1 at Ecm = 8 TeV. The quoted signal strengths are given for mass(H) = 126 GeV. See also AAD 2012DA.


pdgid: S126SZZ
text:
CHATRCHYAN 2012N obtain results based on 4.9 -- 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 5.1 -- 5.3 fb**-1 at Ecm = 8 TeV. An excess of events over background with a local significance of 5.0 sigma is observed at about mass(H) = 125 GeV. The quoted signal strengths are given for mass(H) = 125.5 GeV. See also CHATRCHYAN 2012BY and CHATRCHYAN 2013Y.


pdgid: S126SGG
text:
AAD 2023Y use 139 fb**-1 of p p collisions at Ecm = 13 TeV. The quoted results     are given for mass(H) = 125.09 GeV and width(H) = 4.07 MeV. Measured  and ratios to   the  SM predictions for the different production modes are shown in their Table 9 and Fig. 9.   Measured  cross sections and ratios to the SM predictions in the reduced stage-1.2 (see their Fig.   11)  simplified template cross section framework are shown in their Table 10 and Fig. 12. Wilson   coefficients in the Warsaw basis (see their Table 11) at 95% CL are measured; see their Table   16 and Fig. 17.


pdgid: S126SGG
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The signal  strengths for individual production processes are 1.10+0.23-0.22 for gluon fusion, 1.3+-0.5 for  vector boson fusion, 0.5+1.3-1.2 for W H production, 0.5+3.0-2.5 for Z H  production, and 2.2+1.6-1.3 for t tbar H production.


pdgid: S126SGG
text:
AAD 2024AQ measure fiducial and total cross sections at Ecm = 13.6 TeV with 31.4  fb**-1 data. The quoted results are given for mass(H) = 125.09 GeV. The inclusive fiducial  cross section is 76+14-13 fb with their defined fiducial region (see their Table 2), where  67.6+-3.7 fb is expected in the SM. Assuming SM values for the acceptance and the branching  fraction, the total cross section is 67+12-11 pb, where 59.9+-2.6 pb is expected in the  SM.


pdgid: S126SGG
text:
TUMASYAN 2023Q measure fiducial and differential cross sections at Ecm = 13 TeV with     137 fb**-1 data. The quoted results are given for mass(H) = 125.38 GeV. The inclusive    fiducial  is 73.4+5.4-5.3(stat)+2.4(syst) fb with their defined fiducial   region (see  their  Section 7 and Table 2), where 75.4+-4.1 fb is expected in the Standard   Model. See their  Fig.  8 including other fiducial  defined in their Table 3. Differential    are  shown in  their Figs. 10 -- 15. Double-differential  are in their   Figs. 16 and 17.


pdgid: S126SGG
text:
AAD 2022N measure fiducial and differential cross sections of p p --> H --> gamma gamma  at Ecm = 13 TeV with 139 fb**-1 data. The quoted results are given for mass(H) = 125.09  GeV. The inclusive fiducial sigma.B is 67+-5+-4 fb with their defined  fiducial region. Other fiducial  are in their Table 3. Differential  are shown in  their Figs. 8 -- 13, 15, 25 -- 32, 35, 36. Double-differential  are in their  Figs. 14, 33, 34. Modifications of the b- and c-quark Yukawa couplings to H,  kappa_{{b}} and kappa_{{c}} at 95% CL are in their Table 6 and Fig. 18. Wilson coefficients  at 95% CL are in their Table 7 and Fig. 21.


pdgid: S126SGG
text:
SIRUNYAN 2021O measures cross sections and couplings with the H --> gamma gamma channel   using 137 fb**-1 data at Ecm = 13 TeV. Results are given for mass(H) = 125.38 GeV. The   signal strengths for individual production processes are given in their Fig. 16. Cross sections  are given in  their Tables 12 and 13 and Figs. 18 and 20, which are based on the simplified  template cross  section framework (reduced stage-1.2). Results in the kappa-framework are  given in their Fig. 22.


pdgid: S126SGG
text:
SIRUNYAN 2019L measure fiducial and differential cross sections of the process p p --> H --> gamma gamma at  Ecm = 13 TeV with 35.9 fb**-1. See their Figs. 4 -- 11.


pdgid: S126SGG
text:
AABOUD 2018BO use 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. The signal  strengths for the individual production modes are: 0.81+0.19-0.18 for gluon fusion, 2.0+0.6-0.5 for  vector boson fusion, 0.7+0.9-0.8 for V H production (V = W, Z), and 0.5+-0.6 for  t tbar H and t H production. Other measurements of cross sections and couplings are  summarized in their Section 10. The quoted values are given for mass(H) = 125.09 GeV.


pdgid: S126SGG
text:
SIRUNYAN 2018DS use 35.9 fb**-1 of p p --> H collisions with H --> gamma gamma  at Ecm = 13 TeV. The Higgs mass is floated in the measurement of a signal strength. The  result is 1.18+0.12-0.11(stat.)+0.09(syst.)+0.07(theory), which is largely  insensitive to the Higgs mass around 125 GeV.


pdgid: S126SGG
text:
KHACHATRYAN 2016G measure fiducial and differential cross sections of the process p p --> H X,  H --> gamma gamma at Ecm = 8 TeV with 19.7 fb**-1.  See their Figs. 4 -- 6  and  Table 1 for data.


pdgid: S126SGG
text:
AAD 2014BC use 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The last uncertainty in the measurement is theory systematics. The quoted  signal strength is given for mass(H) = 125.4 GeV. The signal strengths for the individual  production modes are: 1.32+-0.38 for gluon fusion, 0.8+-0.7 for vector boson fusion,  1.0+-1.6 for W H production, 0.1+3.7-0.1 for Z H production, and 1.6+2.7-1.8 for  t tbar H production.


pdgid: S126SGG
text:
AAD 2014BJ measure fiducial and differential cross sections of the process p p --> H X,  H --> gamma gamma at Ecm = 8 TeV with 20.3 fb**-1.  See their Table 3 and Figs.  3 -- 12   for data.


pdgid: S126SGG
text:
KHACHATRYAN 2014P use 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7  fb**-1 at Ecm = 8 TeV. The last uncertainty in the measurement is theory systematics. The quoted signal strength is given  for mass(H) = 124.7 GeV. The signal strength for the gluon fusion and t tbar H production  mode is 1.13+0.37-0.31, while the signal strength for the vector boson fusion and W H, Z H production mode is 1.16+0.63-0.58.


pdgid: S126SGG
text:
AAD 2012AI obtain results based on 4.8 fb**-1 of p p collisions at Ecm = 7 TeV and 5.9 fb**-1 at Ecm = 8 TeV. The quoted signal strengths are given for mass(H) = 126 GeV. See also AAD 2012DA.


pdgid: S126SGG
text:
CHATRCHYAN 2012N obtain results based on 5.1 fb**-1 of p p collisions at Ecm=7 TeV and 5.3 fb**-1 at Ecm=8 TeV. The quoted signal strength is given for mass(H)=125.5 GeV. See also CHATRCHYAN 2013Y.


pdgid: S126SCC
text:
TUMASYAN 2023AH search for V H, H --> c cbar (V = W , Z) using 138 fb**-1   of p p collision data at Ecm = 13 TeV. The upper limit on CS(p p --> V H).B(H --> c cbar)  is 0.94  pb at 95% CL. See their Fig. 4. The quoted values are given for mass(H) = 125.38 GeV.


pdgid: S126SCC
text:
TUMASYAN 2023AD search for Higgs produced with transverse momenta greater than 450 GeV and    decaying to c cbar using 138 fb**-1 of p p collision data at Ecm = 13 TeV.


pdgid: S126SCC
text:
The analysis of V H, H --> c cbar is combined with V H, H --> b bbar (AAD 2021AB).  The ratio |kappa_{{c}}/kappa_{{b}}| is constrained to be less than 4.5 at 95% CL. See  their Fig. 7.


pdgid: S126SCC
text:
AAD 2022W search for V H, H --> c cbar (V = W , Z) using 139 fb**-1 of    p p collision data at Ecm = 13 TeV. The results are given for mass(H) = 125 GeV.


pdgid: S126SCC
text:
The constraint on the charm Yukawa coupling modifier kappa_{{c}} is measured to be  |kappa_{{c}}| <8.5 at 95% CL. See their Fig. 4.


pdgid: S126SCC
text:
SIRUNYAN 2020AE use 35.9 fb**-1 at of p p collisions at Ecm = 13 TeV. The  measured best fit value of CS(p p --> V H).B(H --> c cbar) is 2.40+1.12-1.11+0.65-0.61 pb  (equivalent to < 4.5 pb at 95% CL upper limit, i.e. 70 times the standard model), where  V is W --> lepton nu, Z --> lepton lepton, or Z --> nu nu (lepton = e , mu). The  quoted values are given for mass(H) = 125 GeV.


pdgid: S126SCC
text:
AABOUD 2018M use 36.1 fb**-1 at of p p collisions at Ecm = 13 TeV. The upper  limit on CS(p p --> Z H).B(H --> c cbar) is 2.7 pb at 95% CL. This  corresponds to 110 times the standard model. The quoted values are given for mass(H) = 125 GeV.


pdgid: S126SBB
text:
AAD 2021AB search for V H, H --> b bbar (V = W , Z) using 139 fb**-1 of   p p collision data at Ecm = 13 TeV. The results are given for mass(H) = 125 GeV. Cross   sections are given in their Table 13 and Fig. 7, which are based on the simplified template cross   section framework (reduced stage-1.2). Wilson coefficients of the Warsaw-basis operators are given   in their Fig. 9.


pdgid: S126SBB
text:
AAD 2021AJ present measurements of H --> b bbar in the VBF production mode. The  inclusive VBF cross sections with and without the branching ratio of H --> b bbar are 2.07+-0.70+0.46-0.37  fb and 3.56+-1.21+0.80-0.64 fb, respectively. The latter is obtained assuming the SM value of  B(H --> b bbar) = 0.5809 and mass(H) = 125 GeV.


pdgid: S126SBB
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The signal  strengths for individual production processes are 1.0+-0.5 for W H production, 0.4+-0.4 for  Z H production, and 1.1+-1.0 for t tbar H production.


pdgid: S126SBB
text:
AAD 2024F present studies of the V H production mode in the boosted V --> q qbar and  H --> b bbar (pT(H) > 250 GeV) using 137 fb**-1 of p p collision data  at Ecm = 13 TeV. The quoted signal strength is given for mass(H) = 125.09 GeV and  corresponds to a significance of 1.7 standard deviations. The corresponding inclusive cross section  is 3.1+-1.3+1.8-1.4 pb. The signal strengths and cross sections are given in their Table I  for three pT(H) regions: 250 < pT(H) < 450 GeV, 450 <  pT(H) < 650 GeV, 650 GeV < pT(H) with |y(H)| < 2.


pdgid: S126SBB
text:
HAYRAPETYAN 2024AM search for Z H, H --> b bbar, Z --> b bbar using 133  fb**-1 of p p collision data at Ecm = 13 TeV. The upper limit at 95% CL on the  Z H production is 5.0 times the SM prediction.


pdgid: S126SBB
text:
HAYRAPETYAN 2024AY present measurements of boosted H --> b bbar (pT > 450  GeV) via VBF or gluon fusion productions using 138 fb**-1 of p p collision data at  Ecm = 13 TeV. The result is given for the VBF production. See their Table 3. The V H and  t tbar H production rates are fixed to the SM values. The VBF signal strengths and the fiducial  cross sections for two different m(j j) regions and STXS stage 1.2 bins are shown in their  Figs. 9 and 10, respectively.


pdgid: S126SBB
text:
HAYRAPETYAN 2024AY present measurements of boosted H --> b bbar (pT > 450  GeV) via VBF or gluon fusion productions using 138 fb**-1 of p p collision data at  Ecm = 13 TeV. The result is given for the gluon fusion production. See their Table 3. The  V H and t tbar H production rates are fixed to the SM values. The gluon fusion signal  strengths and the fiducial cross sections for 6 different pT regions and STXS stage 1.2 bins  are shown in their Figs. 9 and 10, respectively.


pdgid: S126SBB
text:
HAYRAPETYAN 2024U present measurements of H --> b bbar in the VBF production mode using  90.8 fb**-1 of data at Ecm = 13 TeV constraining the ggF production to be the SM  expectation. The quoted signal strength corresponds to a significance of 2.4 standard deviations.


pdgid: S126SBB
text:
HAYRAPETYAN 2024U present measurements of H --> b bbar in the inclusive (ggF+VBF)  production mode using 90.8 fb**-1 of data at Ecm = 13 TeV. The quoted signal strength  corresponds to a significance of 2.6 standard deviations.


pdgid: S126SBB
text:
HAYRAPETYAN 2024U present measurements of H --> b bbar in the ggF and VBF production  modes using 90.8 fb**-1 of data at Ecm = 13 TeV. The signal strengths for the ggF and VBF  production modes are independently obtained. See their Fig. 11.


pdgid: S126SBB
text:
TUMASYAN 2024 report the measurement of V H, H --> b bbar (V = W , Z) using  138 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted signal strength  corresponds to a significance of 6.3 standard deviations. Signal strengths for W H and Z H  are given in their Fig. 7. Signal strengths and  for 8 different bins defined based on the  the simplified template cross section framework are given in their Figs. 8 and 9 and Table VII.


pdgid: S126SBB
text:
AAD 2022X measure cross sections using a boosted H --> b bbar with large-radius jets.  The data is 136 fb**-1 of p p collisions at Ecm = 13 TeV. All the results are given  for mass(H) = 125 GeV. The inclusive signal strength is given using data with a H candidate  jet pT>250 GeV. The fiducial H production cross section  (pT(H)>450 GeV and |y(H)|<2) is <115 fb (95% CL) and  the upper limits for other four different pT regions are shown in their Fig 12. The measured  fiducial H production cross section (pT(H)>1 TeV) is 2.3+-3.9(stat)+-1.3(syst)+-0.5(theory) fb.


pdgid: S126SBB
text:
AAD 2021H present measurements of H --> b bbar with a boosted vector boson (pT   > 250 GeV) using 139 fb**-1 of p p collision data at Ecm = 13 TeV. Cross   sections are given in their Table 6 and Fig. 4, which are based on the simplified template cross   section framework (reduced stage-1.2). Wilson coefficients of the Warsaw-basis operators are given   in their Fig. 5.


pdgid: S126SBB
text:
AAD 2021M search for VBF+gamma, H --> b bbar using 132 fb**-1 of p p   collision data at Ecm = 13 TeV.


pdgid: S126SBB
text:
SIRUNYAN 2020BL search for boosted H --> b bbar (a H candidate jet  pT>450 GeV) using 137 fb**-1 of p p collision data at Ecm = 13 TeV. The  quoted signal strength corresponds to a significance of 2.5 standard deviations and is given for  mass(H) = 125 GeV. A differential fiducial cross section as a function of Higgs boson pT  for ggF is shown in their Fig. 7, assuming the other production modes occur at the expected SM  rates. The reported value is 3.7+-1.2+0.8-0.7+0.8-0.5 where the last uncertainty comes from  theoretical modeling. We have combined the systematic uncertainties in quadrature.


pdgid: S126SBB
text:
AABOUD 2019U measure cross sections of p p --> V H, H --> b bbar production as a  function of the gauge boson transverse momentum using data of 79.8 fb**-1. The kinematic  fiducial volumes used is based on the simplified template cross section framework (reduced  stage-1). See their Table 3 and Fig. 3.


pdgid: S126SBB
text:
AABOUD 2018BN search for V H, H --> b bbar (V = W , Z) using 79.8   fb**-1 of p p collision data at Ecm = 13 TeV. The quoted signal strength corresponds   to a significance of 4.9 standard deviations and is given for mass(H) = 125 GeV.


pdgid: S126SBB
text:
AABOUD 2018BN combine results of 79.8 fb**-1 at Ecm = 13 TeV with results of V H at  Ecm = 7 and 8 TeV.


pdgid: S126SBB
text:
AABOUD 2018BN combine results of V H at Ecm = 7, 8 and 13 TeV with results of  VBF (+gluon fusion) and t tbar H at Ecm = 7, 8, and 13 TeV to perform a search for the  H --> b bbar decay. The quoted signal strength assumes a SM production strength and  corresponds to a significance of 5.4 standard deviations.


pdgid: S126SBB
text:
AABOUD 2018BQ search for H --> b bbar produced through vector-boson fusion (VBF) and  VBF+gamma with 30.6 fb**-1 p p collision data at Ecm = 13 TeV. The quoted signal  strength is given for mass(H) = 125 GeV.


pdgid: S126SBB
text:
The signal strength is measured for VBF-only and others (ggF, V H, t tbar H) are  constrained to Standard Model expectations with uncertainties described in their Section VIII B.


pdgid: S126SBB
text:
AALTONEN 2018C use 5.4 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. The upper  limit at 95% CL on p pbar --> H --> b bbar is 33 times the SM prediction, which  corresponds to a cross section of 40.6 pb.


pdgid: S126SBB
text:
SIRUNYAN 2018AE use 35.9 fb**-1 of p p collision data at Ecm = 13 TeV. The  quoted signal strength corresponds to 3.3 standard deviations and is given for mass(H) = 125.09  GeV.


pdgid: S126SBB
text:
SIRUNYAN 2018AE combine the result of 35.9 fb**-1 at Ecm = 13 TeV with the results  obtained from data of up to 5.1 fb**-1 at Ecm = 7 TeV and up to 18.9 fb**-1 at  Ecm = 8 TeV (CHATRCHYAN 2014AI and KHACHATRYAN 2015Z). The quoted signal strength  corresponds to 3.8 standard deviations and is given for mass(H) = 125.09 GeV.


pdgid: S126SBB
text:
SIRUNYAN 2018DB search for V H, H --> b bbar (V = W , Z) using 77.2  fb**-1 of p p collision data at Ecm = 13 TeV. The quoted signal strength corresponds  to a significance of 4.4 standard deviations and is given for mass(H) = 125.09 GeV.


pdgid: S126SBB
text:
SIRUNYAN 2018DB combine the result of 77.2 fb**-1 at Ecm = 13 TeV with the results  obtained from data of up to 5.1 fb**-1 at Ecm = 7 TeV and up to 18.9 fb**-1 at  Ecm = 8 TeV. The quoted signal strength corresponds to a significance of 4.8 standard  deviations and is given for mass(H) = 125.09 GeV.


pdgid: S126SBB
text:
SIRUNYAN 2018DB combine results of 77.2 fb**-1 at Ecm = 13 TeV with results of  gluon fusion (ggF), VBF and t tbar H at Ecm = 7 TeV, 8 TeV and 13 TeV to perform a  search for the H --> b bbar decay. The quoted signal strength assumes a SM production strength  and corresponds to a significance of 5.6 standard deviations and is given for mass(H) = 125.09  GeV.


pdgid: S126SBB
text:
SIRUNYAN 2018E use 35.9 fb**-1 at Ecm = 13 TeV. The quoted signal strength is given  for mass(H) = 125 GeV. They measure sigma.B for gluon fusion production of H --> b bbar with  pT>450 GeV, |eta|<2.5 to be 74+-48+17-10 fb.


pdgid: S126SBB
text:
AABOUD 2017BA use 36.1 fb**-1 at Ecm = 13 TeV. The quoted signal strength is given  for mass(H) = 125 GeV. They give CS(W H).B(H --> b bbar) = 1.08+0.54-0.47  pb and CS(Z H).B(H --> b bbar) = 0.57+0.26-0.23 pb.


pdgid: S126SBB
text:
AABOUD 2017BA combine 7, 8 and 13 TeV analyses. The quoted signal strength is given for  mass(H) = 125 GeV.


pdgid: S126SBB
text:
AABOUD 2016X search for vector-boson fusion production of H decaying to b bbar in  20.2 fb**-1 of p p collisions at Ecm = 8 TeV. The quoted signal strength is given for  mass(H) = 125 GeV.


pdgid: S126SBB
text:
AAD 2015G use 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.36 GeV.


pdgid: S126SBB
text:
KHACHATRYAN 2015Z search for vector-boson fusion production of H decaying to b bbar  in   up to 19.8 fb**-1 of p p collisions at Ecm = 8 TeV. The quoted signal strength  is  given for mass(H) = 125 GeV.


pdgid: S126SBB
text:
KHACHATRYAN 2015Z combined vector boson fusion, W H, Z H production, and t tbar H  production results. The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126SBB
text:
CHATRCHYAN 2014AI use up to 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and up  to 18.9 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125  GeV. See also CHATRCHYAN 2014AJ.


pdgid: S126SBB
text:
AAD 2012AI obtain results based on 4.6 -- 4.8 fb**-1 of p p collisions at Ecm = 7 TeV. The quoted signal strengths are given in their Fig. 10 for mass(H) = 126 GeV. See also Fig. 13 of AAD 2012DA.


pdgid: S126SBB
text:
AALTONEN 2012T combine AALTONEN 2012Q, AALTONEN 2012R, AALTONEN 2012S, ABAZOV 2012O, ABAZOV 2012P, and ABAZOV 2012K. An excess of events over background is observed which is most significant in the region mass(H) = 120 -- 135 GeV, with a local significance of up to 3.3 sigma. The local  significance at mass(H) = 125 GeV is 2.8 sigma, which corresponds to  (CS(H W) + CS(H Z)) . B(H --> b bbar) = (0.23+0.09-0.08) pb, compared to the Standard Model expectation at mass(H) = 125 GeV of 0.12+-0.01 pb. Superseded by AALTONEN 2013M.


pdgid: S126SBB
text:
CHATRCHYAN 2012N obtain results based on 5.0 fb**-1 of p p collisions at Ecm=7 TeV and 5.1 fb**-1 at Ecm=8 TeV. The quoted signal strength is given for mass(H)=125.5 GeV. See also CHATRCHYAN 2013Y.


pdgid: S126SMU
text:
AAD 2021 search for H --> mu+ mu- using 139 fb**-1 of p p collision data at  Ecm = 13 TeV. The quoted signal strength corresponds to a significance of 2.0 standard  deviations and is given for mass(H) = 125.09 GeV. The upper limit on the cross section times  branching fraction is 2.2 times the SM prediction at 95% CL, which corresponds to the  branching fraction upper limit of 4.7E-4 (assuming SM production cross sections).


pdgid: S126SMU
text:
SIRUNYAN 2021 search for H --> mu+ mu- using 137 fb**-1 of p p collision data at  Ecm = 13 TeV. The quoted signal strength corresponds to a significance of 3.0 standard  deviations and is given for mass(H) = 125.38 GeV.


pdgid: S126SMU
text:
SIRUNYAN 2019E search for H --> mu+ mu- using 35.9 fb**-1 of p p collisions at  Ecm = 13 TeV and combine with results of 7 TeV (5.0 fb**-1) and 8 TeV (19.7 fb**-1).  The upper limit at 95% CL on the signal strength is 2.9, which corresponds to the SM Higgs  boson branching fraction to a muon pair of 6.4E-4.


pdgid: S126SMU
text:
AABOUD 2017Y use 36.1 fb**-1 of p p collisions at Ecm = 13 TeV, 20.3 fb**-1  at 8 TeV and 4.5 fb**-1 at 7 TeV. The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126SMU
text:
KHACHATRYAN 2015H use 5.0 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at 8 TeV. The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126SMU
text:
AAD 2014AS search for H --> mu+ mu- in 4.5 fb**-1 of p p collisions at Ecm  = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H)  = 125.5 GeV.


pdgid: S126STT
text:
AABOUD 2019AQ use 36.1 fb**-1 of data. The first, second and third quoted errors are  statistical, experimental systematic and theory systematic uncertainties, respectively. The quoted  signal strength is given for mass(H) = 125 GeV and corresponds to 4.4 standard deviations.  Combining with 7 TeV and 8 TeV results (AAD 2015AH), the observed significance is 6.4  standard deviations. The cross sections in the H --> tau tau decay channel (mass(H) = 125  GeV) are measured to 3.77+0.60-0.59 (stat) +0.87 (syst) pb for the inclusive, 0.28+-0.09+0.11-0.09  pb for VBF, and 3.1+-1.0+1.6-1.3 pb for gluon-fusion production. See their Table XI for the  cross sections in the framework of simplified template cross sections.


pdgid: S126STT
text:
AAD 2016AN perform fits to the ATLAS and CMS data at Ecm = 7 and 8 TeV. The signal  strengths for individual production processes are 1.0+-0.6 for gluon fusion, 1.3+-0.4 for  vector boson fusion, -1.4+-1.4 for W H production, 2.2+2.2-1.8 for Z H  production, and -1.9+3.7-3.3 for t tbar H production.


pdgid: S126STT
text:
AAD 2024BE measure the V H Higgs production (V = W , Z) with H --> tau tau at  Ecm = 13 TeV with 140 fb**-1 data. The quoted signal strength corresponds to 4.2 standard  deviations. The signal strengths for individual W H and Z H productions are 1.48+0.56-0.50 and  1.09+0.51-0.44, respectively. The results are given for mass(H) = 125 GeV. See their Fig. 4.


pdgid: S126STT
text:
HAYRAPETYAN 2024AT present measurements of the boosted H --> tau tau (pT >  250 GeV) using 138 fb**-1 of p p collision data at Ecm = 13 TeV. The quoted signal  strength corresponds to a significance of 3.5 standard deviations. The fiducial inclusive  production cross section is measured to be 3.88+1.69-1.35 fb. The differential fiducial cross  sections as a function of Higgs boson and leading jet pT are given in their Fig. 3.


pdgid: S126STT
text:
TUMASYAN 2023Y measure Higgs production with p p --> H --> tau tau at Ecm = 13 TeV  with 138 fb**-1 data. The quoted results are given for mass(H) = 125.38 GeV.


pdgid: S126STT
text:
The inclusive  is 2800+356-335 fb (see their Figs. 10 and 14). See their Fig. 15 for  the 68 % and 95 % CL contours in the kappa_{{V}}-kappa_{{F}}  plane.


pdgid: S126STT
text:
The quoted result is for the stage-0 simplified template cross section (STXS) and the    sigma_{{ggF}}.B is 2030+598-555 fb (see their Figs. 10 and 14). Measured    cross sections and ratios to the SM predictions in the reduced stage-1.2 STXS (see their Fig. 1)    are shown in their Table 9 and Figs. 12 and 14.


pdgid: S126STT
text:
The quoted result is for the stage-0 STXS and the sigma(VBF).B is 267+53.9-52.6 fb   (see their Figs. 10 and 14).  Measured cross sections and ratios to the SM predictions in the   reduced stage-1.2 STXS (see their Fig.  2) are shown in their Table 9 and Figs. 12, 14.


pdgid: S126STT
text:
The quoted result is for the stage-0 STXS and the sigma_{{VH}}.B is 79.0+20.5-18.6 fb  (see   their Figs. 10 and 14).  Measured cross sections and ratios to the SM predictions in the  reduced   stage-1.2 STXS (see their Fig.  3) are shown in their Table 9 and Figs. 12, 14.


pdgid: S126STT
text:
AAD 2022Q measure cross sections of p p --> H --> tau tau at Ecm = 13 TeV with 139   fb**-1 data. The quoted results are given for mass(H) = 125.09 GeV and   |y(H)|<2.5 is required. The inclusive fiducial sigma.B is 2.94+-0.21+0.37-0.32   pb. The fiducial sigma.B for the four dominant production modes are 2.65+-0.41+0.91-0.67 pb for   ggF, 0.197+-0.028+0.032-0.026 pb for VBF, 0.115+-0.058+0.042-0.040 pb for V H,   0.033+-0.031+0.022-0.017 pb for t tbar H. The cross sections using simplified template   cross section framework (STXS) are given in their Fig. 14(a) and Table 15. The STXS bins (a reduced   stage 1.2) are defined in their Fig. 1.


pdgid: S126STT
text:
TUMASYAN 2022AJ measure cross sections with p p --> H --> tau tau at Ecm = 13 TeV   with 138 fb**-1 data. The fiducial inclusive  is 426+-102 fb while  408+-27  fb is expected in the Standard Mode for mass(H) = 125.38 GeV. Three differential cross  sections  are given; see their Fig. 1.


pdgid: S126STT
text:
SIRUNYAN 2019AF use 35.9 fb**-1 of data. The quoted signal strength is given for  mass(H) = 125 GeV and corresponds to 2.3 standard deviations.


pdgid: S126STT
text:
SIRUNYAN 2019AF use 35.9 fb**-1 of data. H W/Z channels are added with a few  updates on gluon fusion and vector boson fusion with respect to SIRUNYAN 2018Y. The quoted  signal strength is given for mass(H) = 125 GeV and corresponds to 5.5 standard deviations. The  signal strengths for the individual production modes are: 1.12+0.53-0.50 for gluon fusion,  1.13+0.45-0.42 for vector boson fusion, 3.39+1.68-1.54 for W H and 1.23+1.62-1.35 for  Z H. See their Fig. 7 for other couplings (kappa_V, kappa_f).


pdgid: S126STT
text:
SIRUNYAN 2019AT perform a combine fit to 35.9 fb**-1 of data at Ecm = 13 TeV. This  combination is based on SIRUNYAN 2018Y.


pdgid: S126STT
text:
SIRUNYAN 2018Y use 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. The quoted  signal strength is given for mass(H) = 125.09 GeV and corresponds to 4.9 standard deviations.


pdgid: S126STT
text:
SIRUNYAN 2018Y combine the result of 35.9 fb**-1 at Ecm = 13 TeV with the results  obtained from data of 4.9 fb**-1 at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV  (KHACHATRYAN 2015AM). The quoted signal strength is given for mass(H) = 125.09 GeV and corresponds to 5.9 standard deviations.


pdgid: S126STT
text:
AAD 2016AC measure the signal strength with p p --> H W/Z X processes using 20.3  fb**-1 of Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126STT
text:
AAD 2015AH use 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1   at Ecm = 8 TeV.  The third uncertainty in the measurement is theory systematics. The signal   strength for the gluon  fusion mode is 2.0+-0.8+1.2-0.8+-0.3 and that for vector boson   fusion and W / Z H  production modes is 1.24+0.49-0.45+0.31-0.29+-0.08. The quoted   signal strength is given for mass(H) = 125.36 GeV.


pdgid: S126STT
text:
CHATRCHYAN 2014K use 4.9 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125 GeV. See also CHATRCHYAN 2014AJ.


pdgid: S126STT
text:
AAD 2012AI obtain results based on 4.7 fb**-1 of p p collisions at Ecm = 7 TeV. The quoted signal strengths are given in their Fig. 10 for mass(H) = 126 GeV. See also Fig. 13 of AAD 2012DA.


pdgid: S126STT
text:
CHATRCHYAN 2012N obtain results based on 4.9 fb**-1 of p p collisions at Ecm=7 TeV and 5.1 fb**-1 at Ecm=8 TeV. The quoted signal strength is given for mass(H)=125.5 GeV. See also CHATRCHYAN 2013Y .


pdgid: S126SZG
text:
AAD 2024D report combined results of ATLAS (AAD 2020AG) and CMS (TUMASYAN 2023F).  The reported signal strength corresponds to a significance of 3.4 sigma.


pdgid: S126SZG
text:
TUMASYAN 2023F search for H --> Z gamma, Z --> e e , mu mu in 138 fb**-1 of p p  collisions at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV. CS(p p --> H).B(H --> Z gamma) is  measured to be 0.21+-0.08 pb. The ratio of branching fractions B(H --> Z gamma)/B(H --> gamma gamma)  is measured to be 1.5+0.7-0.6.


pdgid: S126SZG
text:
AAD 2020AG search for H --> Z gamma, Z --> e e , mu mu in 139 fb**-1 of p p  collisions at Ecm = 13 TeV. The signal strength is 2.0+-0.9+0.4-0.3 at mass(H) =  125.09 GeV, which corresponds to a significance of 2.2 sigma. The upper limit of CS(p p --> H).B(H --> Z gamma) is 305  fb at 95% CL.


pdgid: S126SZG
text:
SIRUNYAN 2018DQ search for H --> Z gamma, Z --> e e , mu mu in 35.9 fb**-1 of  p p collisions at Ecm = 13 TeV. The quoted signal strength (see their Figs. 6 and 7) is  given for mass(H) = 125 GeV.


pdgid: S126SZG
text:
AABOUD 2017AW search for H --> Z gamma, Z --> e e , mu mu in 36.1 fb**-1 of p p  collisions at Ecm = 13 TeV. The quoted signal strength is given for mass(H) = 125.09 GeV.  The upper limit on the branching ratio of H --> Z gamma is 1.0% at 95% CL assuming  the SM Higgs boson production.


pdgid: S126SZG
text:
AAD 2014J search for H --> Z gamma --> lepton lepton gamma in 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.5 GeV.


pdgid: S126SZG
text:
CHATRCHYAN 2013BK search for H -->  Z gamma --> lepton  lepton gamma in 5.0 fb**-1 of p p collisions at Ecm = 7 TeV and 19.6 fb**-1 at Ecm = 8 TeV. A limit on cross section times branching ratio which corresponds to (4 -- 25) times the expected Standard Model cross section is given in the range mass(H) = 120 -- 160 GeV at 95% CL. The quoted limit is given for mass(H) = 125 GeV, where 10 is expected for no signal.


pdgid: S126A01
text:
AAD 2021I search for H -->  lepton lepton gamma (lepton = e , mu) in 139   fb**-1 of p p collisions at Ecm = 13 TeV. The mass of dilepton m(lepton lepton) is   smaller than 30 GeV. This region is dominated by the decay through gamma^*. The quoted signal   strength corresponds to a significance of 3.2 standard deviations and is given for mass(H) =   125.09 GeV. The cross section times the branching ratio of H -->  lepton lepton gamma for   m(lepton lepton)< 30 GeV is measured to be 8.7+-2.7+0.7-0.6 fb.


pdgid: S126A01
text:
SIRUNYAN 2018DQ search for H --> gamma^* gamma, gamma^* --> mu mu in 35.9 fb**-1  of p p collisions at Ecm = 13 TeV. The mass of gamma^* is smaller than 50 GeV except  in J/psi and Upsilon mass regions. The quoted signal strength (see their Figs. 6 and 7) is  given for mass(H) = 125 GeV.


pdgid: S126A01
text:
KHACHATRYAN 2016B search for H --> gamma^* gamma --> e+ e- gamma and mu+ mu- gamma  (with m(e+ e-) < 3.5 GeV and m(mu+ mu-) < 20 GeV) in 19.7 fb**-1 of p p  collisions at Ecm = 8 TeV. See their Fig. 6 for limits on individual channels.


pdgid: S126KFC
text:
TUMASYAN 2023W measure Higgs production rates with H --> W W^* at Ecm = 13 TeV    with 138  fb**-1 data, assuming mass(H) = 125.38 GeV. See their Fig. 25 for the 68% and    95%  CL contours in the kappa_{{V}}-kappa_{{f}} plane.


pdgid: S126KFC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139  fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV, kappa(V)     >= 0, and kappa(F) >= 0 (B(inv) = B(undetected) = 0). See   their Fig. 4.


pdgid: S126KFC
text:
AAD 2023Y measure Higgs production rates with H --> gamma gamma at Ecm = 13 TeV   with 139 fb**-1 data, assuming mass(H) = 125.09 GeV. See their Fig. 23 for the 68% and   95% CL contours in the kappa_{{V}}-kappa_{{F}} plane, where kappa_{{F}} > 0 is  assumed.


pdgid: S126KFC
text:
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb**-1  of data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV. No uncertainty is given while  their    Fig. 3 left shows 68% and 95% CL contours.


pdgid: S126KVC
text:
TUMASYAN 2023W measure Higgs production rates with H --> W W^* at Ecm = 13 TeV     with 138  fb**-1 data, assuming mass(H) = 125.38 GeV. See their Fig. 25 for the 68% and    95%  CL contours in the  kappa_{{V}}-kappa_{{f}} plane.


pdgid: S126KVC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139   fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV, kappa(V)   >= 0, and kappa(F) >= 0 (B(inv) = B(undetected) = 0). See  their Fig. 4.


pdgid: S126KVC
text:
HAYRAPETYAN 2024AW search for non-resonant H H production in association with a vector  boson using H H --> b bbar b bbar with data of 138 fb**-1 at Ecm = 13 TeV. The vector  boson decays both leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton  = e , mu) and hadronically. See their Fig. 19. All other Higgs couplings are fixed to the SM  values.


pdgid: S126KVC
text:
AAD 2023Y measure Higgs production rates with H --> gamma gamma at Ecm = 13 TeV   with 139 fb**-1 data, assuming mass(H) = 125.09 GeV. See their Fig. 23 for the 68% and   95% CL contours in the kappa_{{V}}-kappa_F plane, where kappa_{{F}} > 0 is  assumed.


pdgid: S126KVC
text:
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb**-1  of  data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV. See their Fig. 3 left.


pdgid: S126KWC
text:
HAYRAPETYAN 2025B present the determination of the relative sign of kappa(W) and  kappa(Z) with VBF W H, H --> b bbar using 138 fb**-1 of data at Ecm =  13 TeV. The opposite-sign coupling hypothesis is excluded with a significance beyond 5sigma.


pdgid: S126KWC
text:
AAD 2024BM present the determination of the relative sign of kappa(W) and  kappa(Z) with VBF W H, H --> b bbar using 140 fb**-1 of data at Ecm =  13 TeV. The opposite-sign coupling hypothesis is excluded with a significance beyond 5sigma.


pdgid: S126KWC
text:
All  modifiers(kappa) > 0, and kappa(c) = kappa(t)  (B(inv)  = B(undetected) = 0) are assumed. Only SM particles assume to contribute  to the loop-induced  processes.See their Fig. 5, which shows both kappa(c) =  kappa(t)  andkappa(c) floating.


pdgid: S126KWC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139   fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV.


pdgid: S126KWC
text:
B(inv) =   B(undetected) = 0 is assumed. Coupling strength modifiers including  effective photon, Z gamma and   gluon are measured. See their Fig. 6.


pdgid: S126KWC
text:
B(inv) floating,  B(undetected) >= 0, and kappa(V) <= 1 are  assumed. Coupling strength modifiers  including effective photon, Z gamma and gluon are  measured. See their Fig. 6.


pdgid: S126KWC
text:
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb**-1  of   data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV.


pdgid: S126KWC
text:
Coupling strength modifiers including  effective photon, Z gamma and gluon are measured. See  their Fig. 4 left.


pdgid: S126KZC
text:
All  modifiers(kappa) > 0, and kappa(c) = kappa(t)  (B(inv)  =B(undetected) = 0) are assumed. Only SM particles assume to contribute to  the loop-induced  processes.See their Fig. 5, which shows both kappa(c) =  kappa(t)  andkappa(c) floating.


pdgid: S126YTC
text:
AAD 2024J measure the CP structure of the top Yukawa coupling using 139 fb**-1 of  data at Ecm = 13 TeV. The top Yukawa coupling strength modifier kappa(t) is  measured with the CP-mixing angle alpha. See their Fig. 3.


pdgid: S126YTC
text:
AAD 2023BC measure the production of four top quarks with same-sign and multilepton final  states with 140 fb**-1 p p collision data at Ecm = 13 TeV. The results constraint the  ratio of the top quark Yukawa coupling y_{{t}} to its Standard Model value, yielding  |y_{{t}}/y_{{t}}^SM()| < 1.9 (see their erratum) at 95% CL. See their Fig. 8 as a  function of kappa(t) and CP-mixing angle.


pdgid: S126YTC
text:
AAD 2023Y constrain kappa_{{t}} from Higgs production rates with H --> gamma gamma with   139 fb**-1 p p collision data at Ecm = 13 TeV. The quoted result is obtained  assuming  the SM loop structure in g g --> H and H --> gamma gamma. See their Fig. 14.


pdgid: S126YTC
text:
AAD 2023Y constrain kappa_{{t}} from Higgs production rates with H --> gamma gamma with    139 fb**-1 p p collision data at Ecm = 13 TeV. The quoted result is obtained   assuming  effective couplings kappa_{{gluon}} and kappa_{{gamma}} for g g --> H and H --> gamma gamma,    respectively. See their Fig. 14.


pdgid: S126YTC
text:
TUMASYAN 2023P constrain kappa_{{t}} from t tbar H and t H decaying H --> W W^*     and H --> tau tau (multilepton decay mode) with 138 fb**-1 p p collision data at     Ecm = 13 TeV. The kappa_{{t}} is obtained by fixing kappatilde_{{t}} = 0 and other     couplings (kappa_{{V}} etc.) to the SM values. See their Fig. 9 for 2-dim contours and Table 6.


pdgid: S126YTC
text:
The quoted result is obtained by combining with other t tbar H decaying H --> gamma gamma  (SIRUNYAN 2020AS)  and  (SIRUNYAN 2021AE) and     kappatilde_{{t}}  = 0. See their Fig. 12 for 2-dim contours and Table7.


pdgid: S126YTC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139  fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV.


pdgid: S126YTC
text:
SIRUNYAN 2021R constrain the ratio of the top quark Yukawa coupling y_{{t}} to its Standard   Model value from t tbar H and t H production rates using 137 fb**-1 p p     collision data at Ecm = 13 TeV. Assuming a SM Higgs couplings to tau's, the joint   interval   -0.9 < kappa_{{t}}(=y_{{t}}/y_{{t}}^SM) < -0.7 and 0.7 <   kappa_{{t}}  <  1.1 is obtained at 95% CL (see their Fig. 17).


pdgid: S126YTC
text:
SIRUNYAN 2020C search for the production of four top quarks with same-sign and multilepton   final states with 137 fb**-1 p p collision data at Ecm = 13 TeV. The results   constraint the ratio of the top quark Yukawa coupling y_{{t}} to its Standard Model value by   comparing to the central value of a theoretical prediction (see their Refs. [1-2]), yielding   |y_{{t}}/y_{{t}}^SM()| < 1.7 at 95% CL. See their Fig. 5.


pdgid: S126YTC
text:
SIRUNYAN 2019BY measure the top quark Yukawa coupling from t tbar kinematic  distributions, the invariant mass of the top quark pair and the rapidity difference between t  and tbar, in the lepton+jets final state with 35.8 fb**-1 p p collision data at  Ecm = 13 TeV. The results constraint the ratio of the top quark Yukawa coupling to its the  Standard Model to be 1.07+0.34-0.43 with an upper limit of 1.67 at 95% CL (see their  Table III).


pdgid: S126YTC
text:
SIRUNYAN 2018BU search for the production of four top quarks with same-sign and multilepton  final states with 35.9 fb**-1 p p collision data at Ecm = 13 TeV. The results  constraint the ratio of the top quark Yukawa coupling y_{{t}} to its the Standard Model by  comparing to the central value of a theoretical prediction (see their Ref. [16]), yielding  |y_{{t}}/y_{{t}}^SM()| < 2.1 at 95% CL.


pdgid: S126KBC
text:
AAD 2023C combine results of H --> gamma gamma and H --> Z Z^* --> 4 lepton   (lepton = e , mu) using 139 fb**-1 at Ecm = 13 TeV. The Higgs boson transverse   momentum (p**H(T)) distribution constrains kappa(b) and   kappa(c), assuming other couplings fixed to the SM values. The kappa(b) is   obtained using the p**H(T) shape and  normalisation. Other cases are given in their  Tables 6 and 7.


pdgid: S126KBC
text:
AAD 2023CD search for H --> Upsilon(nS) gamma, Upsilon(nS) --> mu+ mu- (n=1,2,3) with  138 fb**-1 of p p collision data at Ecm = 13 TeV. They interpret the H --> Upsilon(nS) gamma search  to constraint the bottom Yukawa coupling by comparing to H --> gamma gamma. An observed  95% CL interval of (-37, 40) is obtained for kappa_{{b}}/kappa_{{gamma}}.


pdgid: S126KBC
text:
HAYRAPETYAN 2023 measure the cross sections for p p --> H --> Z Z^* --> 4 lepton  (lepton = e , mu) using 138 fb**-1 at Ecm = 13 TeV. The kappa(b)     is   obtained from the pT differential cross section of the ggF production employing the  dependence  of  the branching fraction on kappa(b) and kappa(c).


pdgid: S126KBC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to  139fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV.


pdgid: S126KBC
text:
All modifiers  (kappa) > 0, and kappa(c) = kappa(t)  (B(inv) =  B(undetected) = 0) are assumed. Only SM particles assume to contribute  to the loop-induced processes.  See their Fig. 5, which shows both kappa(c) =  kappa(t) and  kappa(c) floating.


pdgid: S126KBC
text:
B(inv) = B(undetected) = 0 is assumed. Coupling strength modifiers including  effective photon, Z gamma and gluon are measured. See their Fig. 6.


pdgid: S126KBC
text:
B(inv) floating, B(undetected) >= 0, and kappa(V) <= 1 are  assumed. Coupling strength modifiers including effective photon, Z gamma and gluon are  measured. See their Fig. 6.


pdgid: S126KCC
text:
HAYRAPETYAN 2024D search for the H gamma production using H --> W W^* --> e nu mu nu  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. They interpret the H gamma  search to constraint the charm Yukawa coupling assuming that the charm quark and the Higgs  interaction vertex shown in their Fig. 1 is the only parameter. See their Table II.


pdgid: S126KCC
text:
AAD 2023C combine results of H --> gamma gamma and H --> Z Z^* --> 4 lepton    (lepton = e , mu) using 139 fb**-1 at Ecm = 13 TeV. The Higgs boson transverse    momentum (p^H_T) distribution constrains kappa(b) and  kappa(c),   assuming other couplings fixed to the SM values. The kappa(c) is  obtained using the   p^H_T shape and  normalisation. Other cases are given in their Tables 6 and 7. See  their Table  8 for results  combined with V H, H --> b bbar and c cbar.


pdgid: S126KCC
text:
AAD 2023CD search for H --> J/psi gamma, J/psi --> mu+ mu- with 138 fb**-1 of  p p collision data at Ecm = 13 TeV. They interpret the H --> J/psi gamma search to  constraint the charm Yukawa coupling by comparing to H --> gamma gamma. An observed 95%  CL interval of (-133, 175) is obtained for kappa_{{c}}/kappa_{{gamma}}.


pdgid: S126KCC
text:
HAYRAPETYAN 2023 measure the cross sections for p p --> H --> Z Z^* --> 4 lepton  (lepton = e , mu) using 138 fb**-1 at Ecm = 13 TeV. The kappa(c)   is  obtained from the pT differential cross section of the ggF production employing the  dependence of    the branching fraction of kappa(b) and kappa(c).


pdgid: S126KCC
text:
TUMASYAN 2023AH search for V H, H --> c cbar (V = W , Z) using 138 fb**-1  of p p collision data at Ecm = 13 TeV. The quoted values are obtained from the   measured signal strength in the kappa-framework, where only the Higgs decay width for H --> c cbar is   changed while assuming all the other decay widths and the production cross section to be SM ones.  The quoted values are given for  mass(H) = 125.38 GeV.


pdgid: S126KCC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139  fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV, and all modifiers  (kappa) > 0 (B(inv) = B(undetected) = 0). Only SM particles assume to  contribute to the loop-induced processes. See their Fig. 5, which shows both kappa(c) =  kappa(t) and kappa(c) floating.


pdgid: S126KSC
text:
HAYRAPETYAN 2024D search for the H gamma production using H --> W W^* --> e nu mu nu  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. They interpret the H gamma  search to constraint the strange quark Yukawa coupling assuming that the strange quark and the  Higgs interaction vertex shown in their Fig. 1 is the only parameter. See their Table II.


pdgid: S126KDC
text:
HAYRAPETYAN 2024D search for the H gamma production using H --> W W^* --> e nu mu nu  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. They interpret the H gamma  search to constraint the down quark Yukawa coupling assuming that the down quark and the Higgs  interaction vertex shown in their Fig. 1 is the only parameter. See their Table II.


pdgid: S126KUC
text:
HAYRAPETYAN 2024D search for the H gamma production using H --> W W^* --> e nu mu nu  with 138 fb**-1 of p p collision data at Ecm = 13 TeV. They interpret the H gamma  search to constraint the up quark Yukawa coupling assuming that the up quark and the Higgs  interaction vertex shown in their Fig. 1 is the only parameter. See their Table II.


pdgid: S126KMU
text:
All modifiers(kappa) > 0, and kappa(c) = kappa(t)  (B(inv) =B(undetected) = 0) are assumed. Only SM particles assume to contribute to  the loop-induced processes.See their Fig. 5, which shows both kappa(c) =  kappa(t) andkappa(c) floating.


pdgid: S126KMU
text:
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb**-1  of data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV.


pdgid: S126KGC
text:
AAD 2023Y constrain kappa_{{gamma}} from Higgs production rates with H --> gamma gamma   with 139 fb**-1 p p collision data at Ecm = 13 TeV. The quoted result is obtained   assuming effective couplings kappa_{{gluon}} and kappa_{{gamma}} for g g --> H and H --> gamma gamma,   respectively and other couplings fixed to the SM values. See their Fig. 15.


pdgid: S126KGC
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139    fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV. Coupling strength  modifiers including effective photon, Z gamma and   gluon are measured. See their Fig. 6.


pdgid: S126KGC
text:
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb**-1  of  data at Ecm = 13 TeV, assuming mass(H) = 125.38 GeV. Coupling strength modifiers  including  effective photon, Z gamma and gluon are measured. See their Fig. 4 left.


pdgid: S126KGL
text:
AAD 2023Y constrain kappa_{{gluon}} from Higgs production rates with H --> gamma gamma   with 139 fb**-1 p p collision data at Ecm = 13 TeV. The quoted result is obtained   assuming effective couplings kappa_{{gluon}} and kappa_{{gamma}} for g g --> H and H --> gamma gamma,   respectively and other couplings fixed to the SM values. See their Fig. 15.


pdgid: S126KGL
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to  139fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV. Coupling strength  modifiers including effective photon, Z gamma andgluon are measured. See their Fig. 6.


pdgid: S126KZG
text:
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139    fb**-1 of data at Ecm = 13 TeV, assuming mass(H) = 125.09 GeV. Coupling strength  modifiers including effective photon, Z gamma and gluon are measured. See their Fig. 6.


pdgid: S126STH
text:
SIRUNYAN 2021R search for t tbar H in final states with electrons, muons and   hadronically decaying tau leptons (H --> W W^* , Z Z^* , tau tau) with 137 fb**-1 of   p p collision data at Ecm = 13 TeV. The quoted signal strength corresponds to a   significance of 4.7 standard deviations and is given for mass(H) = 125 GeV.


pdgid: S126STH
text:
AABOUD 2018AC combine results of t tbar H, H --> tau tau, W W^*(lepton nu lepton nu,  lepton nu q qbar), Z Z^*(lepton lepton nu nu, lepton lepton q qbar) with  results of t tbar H, H --> b bbar (AABOUD 2018T), gamma gamma (AABOUD 2018BO), Z Z^*(4 lepton)  (AABOUD 2018AJ) in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. The quoted  signal strength is given for mass(H) = 125 GeV. See their Table 14.


pdgid: S126STH
text:
AAD 2016AN: In the fit, relative branching ratios are fixed to those in the Standard Model.  The quoted signal strength is given for mass(H) = 125.09 GeV.


pdgid: S126STH
text:
TUMASYAN 2023AI measure boosted H --> b bbar (pT > 200 GeV) in t tbar H   production using 138 fb**-1 of data at Ecm = 13 TeV. The differential cross section for   the Higgs pT is shown in their Fig. 8 and Table V. Limits on eight Wilson coefficients at  68% and  95% CL are shown in their Fig. 10 and Table VI.


pdgid: S126STH
text:
AAD 2022M measure H --> b bbar in t tbar H production using 139 fb**-1 of data   at Ecm = 13 TeV. See their Fig. 14. The signal strengths and 95% CL cross section  upper  limits with simplified template cross section bins are given in their Figs. 18 and 19,  respectively.


pdgid: S126STH
text:
AAD 2020Z measure sigma(t tbar H) .B(H --> gamma gamma) to  be 1.64+0.38-0.36+0.17-0.14 fb in 139 fb**-1 of data at Ecm = 13 TeV.


pdgid: S126STH
text:
SIRUNYAN 2020AS measure sigma(t tbar H).B(H --> gamma gamma)  to be 1.56+0.34-0.32 fb in 137 fb**-1 of data at Ecm = 13 TeV.


pdgid: S126STH
text:
SIRUNYAN 2019R search for t tbar H production with H decaying to b bbar in 35.9  fb**-1 of data at Ecm = 13 TeV. The quoted signal strength is given for mass(H) = 125  GeV.


pdgid: S126STH
text:
AABOUD 2018AC search for t tbar H production with H decaying to tau tau, W W^*(lepton nu lepton nu,  lepton nu q qbar), Z Z^*(lepton lepton nu nu, lepton lepton q qbar) in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. The quoted signal strength is given for  mass(H) = 125 GeV. See their Table 13 and Fig. 13.


pdgid: S126STH
text:
AABOUD 2018BK use 79.8 fb**-1 data for t tbar H production with H --> gamma gamma and  Z Z^* --> 4 lepton (lepton = e, mu) and 36.1 fb**-1 for other decay channels at  Ecm = 13 TeV. A significance of 5.8 standard deviations is observed for mass(H) = 125.09  GeV and its signal strength without the uncertainty of the t tbar H cross section is 1.32+0.28-0.26.  Combining with results of 7 and 8 TeV (AAD 2016K), the significance is 6.3 standard  deviations. Assuming Standard Model branching fractions, the total t tbar H production cross  section at 13 TeV is measured to be 670+-90+110-100 fb.


pdgid: S126STH
text:
AABOUD 2018T search for t tbar H production with H decaying to b bbar in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. The quoted signal strength is given for  mass(H) = 125 GeV.


pdgid: S126STH
text:
SIRUNYAN 2018BD search for t tbar H, H --> b bbar in the all-jet final state with  35.9 fb**-1 p p collision data at Ecm = 13 TeV. The quoted signal strength is given  for mass(H) = 125 GeV.


pdgid: S126STH
text:
SIRUNYAN 2018BQ search for t tbar H in final states with electrons, muons and  hadronically decaying tau leptons (H --> W W^* , Z Z^* , tau tau) with 35.9 fb**-1 of  p p collision data at Ecm = 13 TeV. The quoted signal strength corresponds to a  significance of 3.2 standard deviations and is given for mass(H) = 125 GeV.


pdgid: S126STH
text:
SIRUNYAN 2018L use up to 5.1, 19.7 and 35.9 fb**-1  of p p collisions at Ecm =  7, 8, and 13 TeV, respectively. The quoted signal strength corresponds to a significance of 5.2  standard deviations and is given for mass(H) = 125.09 GeV. H decay channels of W W^*,  Z Z^*, gamma gamma, tau tau, and b bbar are used. See their Table 1 and Fig. 2 for  results on individual channels.


pdgid: S126STH
text:
AAD 2016AL search for t tbar H production with H decaying to gamma gamma in 4.5  fb**-1 of p p collisions at Ecm = 7 TeV and b bbar, tau tau, gamma gamma,  W W^*, and Z Z^* in 20.3 fb**-1 at Ecm = 8 TeV. The quoted signal strength is  given for mass(H) = 125 GeV. This paper combines the results of previous papers, and the new  result of this paper only is: mu = 1.6+-2.6.


pdgid: S126STH
text:
AAD 2016K use up to 4.7 fb**-1 of p p collisions at Ecm = 7 TeV and up to 20.3  fb**-1 at Ecm = 8 TeV.  The third uncertainty in the measurement is theory systematics.   The quoted signal strength is given for mass(H) = 125.36 GeV.


pdgid: S126STH
text:
AAD 2015 search for t tbar H production with H decaying to gamma gamma in 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. The quoted result on the signal strength is equivalent to an upper limit of 6.7 at 95% CL and is given for mass(H) = 125.4 GeV.


pdgid: S126STH
text:
AAD 2015BC search for t tbar H production with H decaying to b bbar in 20.3  fb**-1 of p p collisions at Ecm = 8 TeV. The corresponding upper limit is 3.4 at   95% CL.  The quoted signal strength is given for mass(H) = 125 GeV.


pdgid: S126STH
text:
AAD 2015T search for t tbar H production with H resulting in multilepton final  states (mainly from W W^*, tau tau, Z Z^*) in 20.3 fb**-1 of p p collisions  at   Ecm = 8 TeV. The quoted result on the signal strength is given for mass(H) = 125 GeV  and corresponds to an upper limit of 4.7 at 95% CL.   The data sample is independent from  AAD 2015 and  AAD 2015BC.


pdgid: S126STH
text:
KHACHATRYAN 2015AN search for t tbar H production with H decaying to b bbar in  19.5 fb**-1 of p p collisions at Ecm = 8 TeV. The quoted result on the signal   strength is equivalent to an upper limit of 4.2 at  95% CL and is given for mass(H) = 125  GeV.


pdgid: S126STH
text:
KHACHATRYAN 2014H search for t tbar H production with H decaying to b bbar, tau tau, gamma gamma, W W^*, and Z Z^*, in 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. The quoted signal strength is given for mass(H) = 125.6 GeV.


pdgid: S126STH
text:
CHATRCHYAN 2013X search for t tbar H production followed by H -->  b bbar, one top  decaying to lepton nu and the other to either lepton nu or q qbar in 5.0 fb**-1 and  5.1 fb**-1 of p p collisions at Ecm = 7 and 8 TeV. A limit on cross section times  branching ratio which corresponds to (4.0 -- 8.6) times the expected Standard Model cross  section is given for mass(H) = 110 -- 140 GeV at 95% CL. The quoted limit is given  for mass(H) = 125 GeV, where 5.2 is expected for no signal.


pdgid: S126SBH
text:
HAYRAPETYAN 2025 search for b bbar H and b H in final states with leptons using 138  fb**-1 of data at Ecm = 13 TeV. H --> tau tau or H --> W W^* --> lepton nu lepton nu are  considered. Upper limits at 95% CL on the signal strength for each final state are found in  their Fig. 3. Combing with TUMASYAN 2023Y, two-dimensional exclusion regions as a function of  the kappa(b) and kappa(t) parameters are shown in their Fig. 4. The best  fit value is (kappa(t), kappa(b)) = (-0.73, 1.58). All other Higgs  couplings are fixed to the SM values.


pdgid: S126SVB
text:
HAYRAPETYAN 2025B present the determination of the relative sign of kappa(W) and  kappa(Z) with VBF W H, H --> b bbar using 148 fb**-1 of data at Ecm =  13 TeV. The upper limit at 95% CL on the cross section for VBF W H production is  obtained. The signal strength is measured to be 2.2+6.1-5.8.


pdgid: S126SVB
text:
AAD 2024BM present the determination of the relative sign of kappa(W) and  kappa(Z) with VBF W H, H --> b bbar using 140 fb**-1 of data at Ecm =  13 TeV. The upper limit at 95% CL on the cross section for VBF W H production is obtained.  The signal strength is measured to be 0.9+4.0-4.3.


pdgid: S126SHH
text:
AAD 2023AT combine results from 126 -- 139 fb**-1 of data at Ecm = 13 TeV  for p p --> H H --> b bbar b bbar  (AAD 2023BK), b bbar tau tau (AAD 2023Z),  and b bbar gamma gamma (AAD 2022Y).


pdgid: S126SHH
text:
AAD 2024AZ search for non-resonant H H production using H H --> b bbar tau tau with  data of 140 fb**-1 at Ecm = 13 TeV. The result is interpreted: limits on Wilson  coefficients of the Higgs effective field theory (HEFT) and the SM effective field theory (SMEFT)  are shown in their Table IV and Figs. 11 and 12; the ggF H H production cross sections (7  benchmark points) of HEFT are shown in their Fig. 10. In those interpretations the VBF H H  production is neglected.


pdgid: S126SHH
text:
AAD 2024BG search for non-resonant H H production targeting the b bbar Z Z^*, V V V V, V V tau tau,  tau tau tau tau,  gamma gamma V V, gamma gamma tau tau decay channels with data of 140 fb**-1 at  Ecm = 13 TeV. Signal strengths for the 11 different signal regions are given in their Fig. 8.


pdgid: S126SHH
text:
AAD 2024BL combine results from 126 -- 140 fb**-1 of data at Ecm = 13 TeV  for p p --> H H --> b bbar b bbar (AAD 2023BK, AAD 2024BV), b bbar tau tau  (AAD 2024AZ), b bbar gamma gamma (AAD 2024X), multilepton (AAD 2024BG), and  b bbar lepton lepton (AAD 2024Y). See their Fig. 2. The signal strength is measured to be  0.5+1.2-1.0. Constraints for three interaction parameters (c(tthh), c(gghh),  c(hhh)) in the Higgs effective field theory are set. See their Fig. 4.


pdgid: S126SHH
text:
AAD 2024X search for non-resonant H H production using H H --> b bbar gamma gamma  with data of 140 fb**-1 at Ecm = 13 TeV. The result is interpreted: limits on three  Wilson coefficients and the ggF H H production cross sections (7 benchmark points shown in  their Table 5) of the Higgs effective field theory are shown in their Table 4 and Fig. 8,  respectively; limits on two Wilson coefficients of the SM effective field theory are shown in their  Table 6 and Fig. 9. In those interpretations only the ggF H H production is considered instead  of both ggF and VBF.


pdgid: S126SHH
text:
AAD 2024Y search for non-resonant H H production in 2 b + 2 lepton + nus final state  (lepton = e , mu) targeting b bbar W W^*, b bbar Z Z^*, and b bbar tau tau  decay channels with data of 140 fb**-1 at Ecm = 13 TeV. The signal strength is measured  to be -8.5+7.7-8.4. See their Fig. 6.


pdgid: S126SHH
text:
HAYRAPETYAN 2024AE search for non-resonant H H production using H H --> b bbar W W^*  with data of 138 fb**-1 at Ecm = 13 TeV. The result is interpreted: the ggF H H  production cross sections (20 benchmark points) of the Higgs effective field theory are shown in  their Fig. 16; the coupling between two top quarks and two Higgs bosons is constrained between  [-0.8, 1.3] at 95%CL (see their Fig. 17) with all other Higgs couplings fixed to the SM  values.


pdgid: S126SHH
text:
HAYRAPETYAN 2024AW search for non-resonant H H production in association with a vector  boson using H H --> b bbar b bbar with data of 138 fb**-1 at Ecm = 13 TeV. The vector  boson decays both leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton  = e , mu) and hadronically. The quoted value is the upper limit of the V H H cross section.  See their Figs. 13 and 16 (left) for the best fit and the upper limit of the V H H cross  section, respectively. In addition, upper limits at 95% CL on V H H and H H cross  sections are shown as a function of kappa(lambda), kappa(2V), and  kappa(V) in their Figs. 17, 18, and 19.


pdgid: S126SHH
text:
AAD 2023AD search for non-resonant H H production in association with a vector boson   using H H --> b bbar b bbar with data of 139 fb**-1 at Ecm = 13 TeV. The vector  boson  decays leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton =  e , mu).


pdgid: S126SHH
text:
AAD 2023BK search for non-resonant H H production using H H --> b bbar b bbar with  data of 126 fb**-1 at Ecm = 13 TeV.


pdgid: S126SHH
text:
AAD 2023Z search for non-resonant H H production using H H --> b bbar tau tau with  data of 139 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H production  cross section at 95% CL is measured to be 140 fb, which corresponds to 4.7 times the SM  prediction (see their Table 6).


pdgid: S126SHH
text:
TUMASYAN 2023AE search for H H production using H H --> b bbar b bbar, where both  b bbar pairs are highly boosted, with data of 138 fb**-1 at Ecm = 13 TeV.


pdgid: S126SHH
text:
TUMASYAN 2023D search for non-resonant H H production using H H --> b bbar tau tau   with data of 138 fb**-1 at Ecm = 13 TeV.


pdgid: S126SHH
text:
The upper limit on the p p --> H H  production cross section (gluon fusion and VBF) at   95% CL is  measured to be 102 fb, which corresponds to 3.3 times the SM prediction (see their   Table 2).


pdgid: S126SHH
text:
The upper limit on the VBF p p --> H H production cross section at 95% CL is measured to  be 212 fb, which corresponds to 124 times the SM prediction (see their Table 3).


pdgid: S126SHH
text:
TUMASYAN 2023I search for non-resonant H H production using H H --> b bbar Z Z^*  (Z Z^* --> 4 lepton, lepton = e , mu) with data of 138 fb**-1 at Ecm = 13 TeV.


pdgid: S126SHH
text:
TUMASYAN 2023O search for non-resonant H H production using H H --> W W^* W W^*, W W^* tau tau, and   tau tau tau tau (multilepton) with data of 138 fb**-1 at Ecm = 13 TeV. See their Fig.   9 for different final states and these combination.


pdgid: S126SHH
text:
AAD 2022Y search for non-resonant H H production using H H --> gamma gamma b bbar  with data of 139 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H  production cross section at 95% CL is measured to be 130 fb, which corresponds to 4.2 times  the SM prediction.


pdgid: S126SHH
text:
CMS 2022 report combined results (see their Extended Data Table 2) using 138 fb**-1 of    data at Ecm = 13 TeV. See their Fig. 5 (left) for different final states and these  combination.


pdgid: S126SHH
text:
TUMASYAN 2022AN search for non-resonant H H production using H H --> b bbar b bbar with    data of 138 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H production    cross section at 95% CL is measured to be 120 fb, which corresponds to 3.9 times the SM    prediction.


pdgid: S126SHH
text:
SIRUNYAN 2021K search for non-resonant H H production using H H --> gamma gamma b bbar with   data of 137 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H --> gamma gamma b bbar   production cross section at 95% CL is measured to be 0.67 fb, which corresponds to about 7.7   times the SM prediction.


pdgid: S126SHH
text:
AAD 2020C combine results of up to 36.1 fb**-1 data at Ecm = 13 TeV for p p --> H H --> b bbar gamma gamma,  b bbar tau tau, b bbar b bbar, b bbar W W^*, W W^* gamma gamma, W W^* W W^*  (AABOUD 2018CW, AABOUD 2018CQ, AABOUD 2019A, AABOUD 2019O, AABOUD 2018BU, and  AABOUD 2019T).


pdgid: S126SHH
text:
AAD 2020E search non-resonant for H H production using H H --> b bbar lepton nu lepton nu,  where one of the Higgs bosons decays to b bbar and the other decays to either W W^*, Z Z^*, or  tau tau, with data of 139 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H  production cross section at 95% CL is measured to be 1.2 pb, which corresponds to about 40  times the SM prediction.


pdgid: S126SHH
text:
AAD 2020X search for H H --> b bbar b bbar  process via VBF with data of 126 fb**-1    at Ecm = 13 TeV. The upper limit on the SM  non-resonant H H production cross section  is   1460 fb at 95% CL, which corresponds to 840  times the SM prediction.


pdgid: S126SHH
text:
AABOUD 2019A search for H H production using H H --> b bbar b bbar with data of  36.1 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H --> b bbar b bbar  production cross section at 95% is measured to be 147 fb, which corresponds to about 12.9  times the SM prediction.


pdgid: S126SHH
text:
AABOUD 2019O search for H H production using H H --> b bbar W W^* with data of  36.1 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H production cross  section at 95% CL is calculated to be 10 pb from the observed upper limit on the p p --> H H --> b bbar W W^*  production cross section of 2.5 pb assuming the SM branching fractions. The former corresponds to  about 300 times the SM prediction.


pdgid: S126SHH
text:
AABOUD 2019T search for H H production using H H --> W W^* W W^* with data of  36.1 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H production cross  section at 95% is measured to be 5.3 pb, which corresponds to about 160 times the SM  prediction.


pdgid: S126SHH
text:
SIRUNYAN 2019 search for H H production using H H --> gamma gamma b bbar with   data of 35.9 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H --> gamma gamma b bbar   production cross section at 95% CL is measured to be 2.0 fb, which corresponds to about 24   times the SM prediction.


pdgid: S126SHH
text:
SIRUNYAN 2019AB search for H H production using H H --> b bbar b bbar, where 4  heavy flavor jets from two Higgs bosons are resolved, with data of 35.9 fb**-1 at Ecm =  13 TeV. The upper limit on the p p --> H H --> b bbar b bbar production cross section at  95% is measured to be 847 fb, which corresponds to about 75 times the SM prediction.


pdgid: S126SHH
text:
SIRUNYAN 2019BE combine results of 13 TeV 35.9 fb**-1 data: SIRUNYAN 2019,  SIRUNYAN 2018A, SIRUNYAN 2019AB, SIRUNYAN 2019H, and SIRUNYAN 2018F.


pdgid: S126SHH
text:
SIRUNYAN 2019H search for H H production using H H --> b bbar b bbar, where one  of b bbar pairs is highly boosted and the other one is resolved, with data of 35.9 fb**-1  at Ecm = 13 TeV. The upper limit on the p p --> H H --> b bbar b bbar production cross  section at 95% is measured to be 1980 fb, which corresponds to about 179 times the SM  prediction.


pdgid: S126SHH
text:
AABOUD 2018BU search for H H production using gamma gamma W W^* with the final  state of gamma gamma lepton nu j j using data of 36.1 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H production cross section at 95% CL is measured to  be 7.7 pb, which corresponds to about 230 times the SM prediction. The upper limit on the p p --> H H --> gamma gamma W W^*  at 95% CL is measured to be 7.5 fb (see thier Table 6).


pdgid: S126SHH
text:
AABOUD 2018CQ search for H H production using H H --> b bbar tau tau with data of  36.1 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H --> b bbar tau tau  production cross section at 95% is measured to be 30.9 fb, which corresponds to about 12.7  times the SM prediction.


pdgid: S126SHH
text:
AABOUD 2018CW search for H H production using H H --> gamma gamma b bbar with   data of 36.1 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H production   cross section at 95% is measured to be 0.73 pb, which corresponds to about 22 times the SM   prediction.


pdgid: S126SHH
text:
SIRUNYAN 2018A search for H H production using H H --> b bbar tau tau with data   of 35.9 fb**-1 at Ecm = 13 TeV. The upper limit on the g g --> H H --> b bbar tau tau   production cross section is measured to be 75.4 fb, which corresponds to about 30 times the SM   prediction.


pdgid: S126SHH
text:
SIRUNYAN 2018F search non-resonant for H H production using H H --> b bbar lepton nu lepton nu, where  lepton nu lepton nu is either W W --> lepton nu lepton nu or Z Z --> lepton lepton nu nu  (lepton is e , mu or a leptonically decaying tau), with data of 35.9 fb**-1 at  Ecm = 13 TeV. The upper limit on the H H --> b bbar lepton nu lepton nu production  cross section at 95% CL is measured to be 72 fb, which corresponds to about 79 times the SM  prediction.


pdgid: S126SHH
text:
SIRUNYAN 2017CN search for H H production using H H --> b bbar tau tau with data  of 18.3 fb**-1 at Ecm = 8 TeV. Results are then combined with the published results of  the H H --> gamma gamma b bbar and H H --> b bbar b bbar, which use data of up to 19.7  fb**-1 at Ecm = 8 TeV. The upper limit on the g g --> H H production cross section  is measured to be 0.59 pb from b bbar tau tau, which corresponds to about 59 times the SM  prediction (gluon fusion). The combined upper limit is 0.43 pb, which is about 43 times the SM  prediction. The quoted values are given for mass(H) = 125 GeV.


pdgid: S126SHH
text:
AABOUD 2016I search for H H production using H H --> b bbar b bbar with data of 3.2 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H --> b bbar b bbar production cross section is measured to be 1.22 pb. This result corresponds to about 108 times the SM prediction (gluon fusion), which is 11.3+0.9-1.0 fb (NNLO+NNLL) including top quark mass effects. The quoted values are given for mass(H) = 125 GeV.


pdgid: S126SHH
text:
KHACHATRYAN 2016BQ search for H H production using H H --> gamma gamma b bbar   with data of 19.7 fb**-1 at Ecm = 8 TeV. The upper limit on the g g --> H H --> gamma gamma b bbar   production is measured to be 1.85 fb, which corresponds to about 74 times the SM prediction and is   translated into 0.71 pb for g g --> H H production cross section.


pdgid: S126SHH
text:
AAD 2015CE search for H H production using H H --> b bbar tau tau and H H --> gamma gamma W W with  data of 20.3 fb**-1 at Ecm = 8 TeV. These results are then combined with the published  results of the H H --> gamma gamma b bbar and H H --> b bbar b bbar, which use data of  up to 20.3 fb**-1 at Ecm = 8 TeV. The upper limits on the g g --> H H production  cross section are measured to be 1.6 pb, 11.4 pb, 2.2 pb and 0.62 pb from b bbar tau tau,  gamma gamma W W, gamma gamma b bbar and b bbar b bbar, respectively. The combined upper  limit is 0.69 pb, which corresponds to about 70 times the SM prediction. The quoted results are  given for mass(H) = 125.4 GeV. See their Table 4.


pdgid: S126KLA
text:
AAD 2024BL combine results from 126 -- 140 fb**-1 of data at Ecm = 13 TeV  for p p --> H H --> b bbar b bbar (AAD 2023BK, AAD 2024BV), b bbar tau tau  (AAD 2024AZ), b bbar gamma gamma (AAD 2024X), multilepton (AAD 2024BG), and  b bbar lepton lepton (AAD 2024Y). See their Fig. 3.  All other Higgs couplings are fixed to the SM values.


pdgid: S126KLA
text:
AAD 2024AZ search for non-resonant H H production using H H --> b bbar tau tau with  data of 140 fb**-1 at Ecm = 13 TeV. Two-dimensional exclusion regions as a function of  the kappa_{{lambda}} and kappa_{{2V}} couplings are shown in their Fig. 9. All other Higgs  couplings are fixed to the SM values.


pdgid: S126KLA
text:
AAD 2024BG search for non-resonant H H production targeting the b bbar Z Z^*, V V V V, V V tau tau, tau tau tau tau,  gamma gamma V V, gamma gamma tau tau decay channels with data of 140 fb**-1 at  Ecm = 13 TeV. The limits are obtained with the values of all other couplings fixed to their  SM value.


pdgid: S126KLA
text:
AAD 2024X search for non-resonant H H production using H H --> b bbar gamma gamma  with data of 140 fb**-1 at Ecm = 13 TeV. Two-dimensional exclusion regions as a function  of the kappa(lambda) and kappa(2V) couplings are shown in their  Fig. 6. All other Higgs couplings are fixed to the SM values.


pdgid: S126KLA
text:
AAD 2024Y search for non-resonant H H production in 2 b + 2 lepton + nus final state  (lepton = e , mu) targeting b bbar W W^*, b bbar Z Z^*, and b bbar tau tau  decay channels with data of 140 fb**-1 at Ecm = 13 TeV.  All other coupling modifiers are set to their SM values.


pdgid: S126KLA
text:
HAYRAPETYAN 2024AE search for non-resonant H H production using H H --> b bbar W W^*  with data of 138 fb**-1 at Ecm = 13 TeV. Two-dimensional exclusion regions as a function  of the (kappa(lambda), kappa(2V)) and  (kappa(lambda), kappa(t)) are shown in their Figs. 13 and 15. All  other Higgs couplings are fixed to the SM values.


pdgid: S126KLA
text:
HAYRAPETYAN 2024AW search for non-resonant H H production in association with a vector  boson using H H --> b bbar b bbar with data of 138 fb**-1 at Ecm = 13 TeV. The vector  boson decays both leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton  = e , mu) and hadronically. All other Higgs couplings are fixed to the SM values.  Two-dimensional exclusion regions as a function of the kappa(2V) and  kappa(lambda) parameters are shown in their Fig. 14, with other couplings fixed  to the SM values. The best fit value is (kappa(lambda), kappa(2V))  = (-2.6, 10.1).


pdgid: S126KLA
text:
AAD 2023AD search for non-resonant H H production in association with a vector boson   using H H --> b bbar b bbar with data of 139 fb**-1 at Ecm = 13 TeV. The vector  boson  decays leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton =  e , mu). The  quoted kappa(lambda) is measured assuming all other Higgs  boson couplings are  at their SM value.


pdgid: S126KLA
text:
AAD 2023AT combine results from 126 -- 139 fb**-1 of data at Ecm = 13 TeV  for  p p --> H H --> b bbar b bbar   (AAD 2023BK), b bbar tau tau (AAD 2023Z),  and  b bbar gamma gamma (AAD 2022Y). The quoted values are obtained from the profile  likelihood scan as a function of kappa(lambda) as shown in their Fig. 5(a). All  other coupling modifiers are assumed to have their  SM values.


pdgid: S126KLA
text:
AAD 2023AT combine results from 126 -- 139 fb**-1 of data at Ecm = 13 TeV  for p p --> H H --> b bbar b bbar  (AAD 2023BK), b bbar tau tau (AAD 2023Z),  and b bbar gamma gamma (AAD 2022Y) with  single-Higgs boson analyses (gamma gamma,  Z Z^*, W W^*, tau tau, b bbar, see  their Table 1). The quoted values are obtained  from the profile likelihood scan as a function of kappa(lambda) as shown in  their Fig. 5(a), assuming that all other Higgs boson couplings are at their SM values. Results with  other assumptions are shown in  their Table 2.


pdgid: S126KLA
text:
AAD 2023BK search for non-resonant H H production using H H --> b bbar b bbar with  data of 126 fb**-1 at Ecm = 13 TeV. The quoted values are obtained from the  one-dimensional profile likelihood scan as a function of kappa(lambda). See  their Fig. 12 (a). The mu(ggF+VBF) measurement for different values of  kappa(lambda) constrains -3.9 < kappa(lambda) <  11.1 at 95% CL as shown in their Fig. 10 (a). kappa(2V)= kappa(V)=1  is assumed in both cases.


pdgid: S126KLA
text:
HAYRAPETYAN 2023 measure the cross sections for p p --> H --> Z Z^* --> 4 lepton   (lepton = e , mu) using 138 fb**-1 at Ecm = 13 TeV.


pdgid: S126KLA
text:
TUMASYAN 2023AE search for H H production using H H --> b bbar b bbar, where both   b bbar pairs are highly boosted, with data of 138 fb**-1 at Ecm = 13 TeV. The quoted   kappa(lambda) is measured assuming all other Higgs boson couplings are at  their  SM values.


pdgid: S126KLA
text:
TUMASYAN 2023D search for non-resonant H H production using H H --> b bbar tau tau  with data of 138 fb**-1 at Ecm = 13 TeV. The quoted values are obtained from the   upper limit on the H H production cross section times the b bbar tau tau branching fraction   for different values of kappa(lambda). See their Fig. 8 (left). All other   coupling modifiers are assumed to be 1. In addition, two-dimensional exclusion regions as a   function of the kappa(lambda) and kappa(t) couplings, with   kappa(2V)  = kappa(V) = 1, are shown in their Fig. 9 (left). The   one-dimensional likelihood scan as a function of kappa(lambda) is given in   their Fig 10 (left), from which a 95% confidence interval of -1.77 <    kappa(lambda) < 8.73 is extracted.


pdgid: S126KLA
text:
TUMASYAN 2023AI search for non-resonant H H production using H H --> b bbar Z Z^*    (Z Z^* --> 4 lepton, lepton=e,mu) with data of 138 fb**-1 at Ecm = 13    TeV. See their Fig. 4.


pdgid: S126KLA
text:
TUMASYAN 2023O search for non-resonant H H production using H H --> W W^* W W^*, W W^* tau tau, and    tau tau tau tau (multilepton) with data of 138 fb**-1 at Ecm = 13 TeV. See their   Fig. 10 for different final states and these combination. Limits are set on a variety of   new-physics models using an effective field theory approach. See their Figs. 11, 12, and 13.


pdgid: S126KLA
text:
AAD 2022Y search for non-resonant H H production using H H --> gamma gamma b bbar  with data of 139 fb**-1 at Ecm = 13 TeV. The quoted kappa_{{lambda}} is obtained from  their Fig. 12 where the theory uncertainties are not included while a negative log-likelihood scan  vs. kappa_{{lambda}}is shown in their Fig. 13 with the theory uncertainties, which provides  kappa_{{lambda}} = 2.8+2.0-2.2 for the 1sigma confidence interval.


pdgid: S126KLA
text:
CMS 2022 report combined results (see their Extended Data Table 2) using 138 fb**-1 of   data at Ecm = 13 TeV. See their Fig. 6 (left).


pdgid: S126KLA
text:
TUMASYAN 2022AN search for non-resonant H H production using H H --> b bbar b bbar with  data of 138 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H      production     cross section at 95% CL is shown as a function of   kappa(lambda) in    their Fig. 2  (top).


pdgid: S126KLA
text:
SIRUNYAN 2021K search for non-resonant H H production using H H --> gamma gamma b bbar with   data of 137 fb**-1 at Ecm = 13 TeV.


pdgid: S126KLA
text:
SIRUNYAN 2019 search for H H production using H H --> gamma gamma b bbar with   data of 35.9 fb**-1 at Ecm = 13 TeV. The quoted kappa(lambda) is  measured assuming all other Higgs boson couplings are at their SM value.


pdgid: S126KLA
text:
AABOUD 2018CW search for H H production using H H --> gamma gamma b bbar with   data of 36.1 fb**-1 at Ecm = 13 TeV. The quoted kappa(lambda) is  measured assuming all other Higgs boson couplings are at their SM value.


pdgid: S126KLA
text:
SIRUNYAN 2018A search for H H production using H H --> b bbar tau tau with data  of 35.9 fb**-1 at Ecm = 13 TeV. The upper limit on production cross section times  branching fraction at 95% CL is shown as a function of  kappa(lambda)/kappa(t) in their Fig. 6 (top) where  kappa(t) = y_t / y_t**SM (top Yukawa coupling y_t).


pdgid: S126KLA
text:
KHACHATRYAN 2016BQ search for H H production using H H --> gamma gamma b bbar  with data of 19.7 fb**-1 at Ecm = 8 TeV.


pdgid: S126K2V
text:
AAD 2024BL combine results from 126 -- 140 fb**-1 of data at Ecm = 13 TeV  for p p --> H H --> b bbar b bbar (AAD 2023BK, AAD 2024BV), b bbar tau tau  (AAD 2024AZ), b bbar gamma gamma (AAD 2024X), multilepton (AAD 2024BG), and  b bbar lepton lepton (AAD 2024Y). See their Fig. 3. All other Higgs couplings are fixed  to the SM values.


pdgid: S126K2V
text:
AAD 2024BV search for non-resonant H H production via vector boson fusion in the b bbar b bbar  final state using two boosted Higgs (pT > 250 GeV) with data of 140 fb**-1 at  Ecm = 13 TeV. The result is obtained by combining with the resolved result (AAD 2023BK). The  value kappa(2V) = 0 is excluded with a significance of 3.8 sigma with other  Higgs couplings fixed to their SM values. Two-dimensional exclusion regions as a function of the  kappa(lambda) and kappa(2V) parameters are shown in their Fig. 6.  All other Higgs couplings are fixed to the SM values.


pdgid: S126K2V
text:
AAD 2024BV search for non-resonant H H production via vector boson fusion in the b bbar b bbar  final state using two boosted Higgs (pT > 250 GeV) with data of 140 fb**-1 at  Ecm = 13 TeV. The value kappa(2V) = 0 is excluded with a significance of 3.4  sigma with other Higgs couplings fixed to their SM values.


pdgid: S126K2V
text:
HAYRAPETYAN 2024AE search for non-resonant H H production using H H --> b bbar W W^*  with data of 138 fb**-1 at Ecm = 13 TeV. Two-dimensional exclusion regions as a function  of the (kappa(lambda), kappa(2V)) and (kappa(V),  kappa(2V)) are shown in their Figs. 13 and 14. All other Higgs couplings are fixed to  the SM values.


pdgid: S126K2V
text:
HAYRAPETYAN 2024AW search for non-resonant H H production in association with a vector  boson using H H --> b bbar b bbar with data of 138 fb**-1 at Ecm = 13 TeV. The vector  boson decays both leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton  = e , mu) and hadronically. All other Higgs couplings are fixed to the SM values.  Two-dimensional exclusion regions as a function of the kappa(2V) and  kappa(lambda) parameters are shown in their Fig. 14, with other couplings fixed  to the SM values. The best fit value is (kappa(lambda), kappa(2V))  = (-2.6, 10.1). The constraints on kappa(2W) and kappa(2Z) are separately  measured to be -14.0 < kappa(2W) < 15.4 and -17.4 <  kappa(2Z) < 18.5 (95% CL). The quoted kappa(2V) (V = W , Z) is  measured assuming all other Higgs boson couplings are at their SM value. See their Table 7.


pdgid: S126K2V
text:
AAD 2023AD search for non-resonant H H production in association with a vector boson   using H H --> b bbar b bbar with data of 139 fb**-1 at Ecm = 13 TeV. The vector  boson  decays leptonically (W --> lepton nu, Z --> lepton lepton, nu nu, lepton =  e , mu). The  constraints on kappa(2W) and kappa(2Z) are separately  measured to be -12.3  < kappa(2W) < 13.5 and -9.9 <  kappa(2Z) < 11.3  (95% CL). The quoted kappa(2V) (V = W , Z) is  measured assuming all other  Higgs boson couplings are at their SM value.


pdgid: S126K2V
text:
AAD 2023AT combine results from 126 -- 139 fb**-1 of data at Ecm = 13 TeV  for  p p --> H H --> b bbar b bbar   (AAD 2023BK), b bbar tau tau (AAD 2023Z),  and  b bbar gamma gamma (AAD 2022Y). The quoted values are obtained from the 95% CL  VBF H H cross-section upper limit as a function of kappa(2V) as shown in their Fig.  4(b). All  other coupling modifiers are assumed to have their  SM values.


pdgid: S126K2V
text:
AAD 2023BK search for non-resonant H H production using H H --> b bbar b bbar with  data of 126 fb**-1 at Ecm = 13 TeV. The quoted values are obtained from the  one-dimensional profile likelihood scan as a function of kappa(2V). See their Fig. 12  (b). The mu(VBF) measurement for different values of kappa(2V) constrains  -0.03 < kappa(2V) < 2.11 at 95% CL as shown in their Fig. 10 (b).  kappa(lambda)= kappa(V) = 1 is assumed in both cases.


pdgid: S126K2V
text:
TUMASYAN 2023AE search for H H production using H H --> b bbar b bbar, where both    b bbar pairs are highly boosted, with data of 138 fb**-1 at Ecm = 13 TeV. The   kappa(2V) = 0 is excluded at 6.3 sigma assuming all other Higgs boson couplings    are at their SM values.


pdgid: S126K2V
text:
TUMASYAN 2023D search for non-resonant H H production using H H --> b bbar tau tau     with data of 138 fb**-1 at Ecm = 13 TeV. The quoted values are obtained from the upper  limits on the H H production cross section times the b bbar tau tau branching fraction for  different values of kappa(2V). See their Fig. 8 (right). All other coupling modifiers  are assumed to be 1. In addition, two-dimensional exclusion regions as a function of the  kappa(2V) and kappa(V) couplings, with kappa(lambda) =  kappa(t) = 1, are shown in their Fig. 9 (right). The one-dimensional likelihood scan as  a function of kappa(2V) is given in their Fig. 10 (right), from which a 95%  confidence interval of -0.34 < kappa(2V) < 2.49 is extracted.


pdgid: S126K2V
text:
CMS 2022 report combined results (see their Extended Data Table 2) using 138 fb**-1 of  data at Ecm = 13 TeV. See their Fig. 6 (right).


pdgid: S126K2V
text:
TUMASYAN 2022AN search for non-resonant H H production using H H --> b bbar b bbar with  data of 138 fb**-1 at Ecm = 13 TeV. The upper limit on the p p --> H H    production     cross section at 95% CL is shown as a function of kappa(2V) in    their Fig. 2  (bottom).


pdgid: S126K2V
text:
SIRUNYAN 2021K search for non-resonant H H production using H H --> gamma gamma b bbar with  data of 137 fb**-1 at Ecm = 13 TeV.


pdgid: S126K2V
text:
AAD 2020X search for H H --> b bbar b bbar process via VBF with data of 126 fb**-1   at Ecm = 13 TeV.


pdgid: S126PTH
text:
SIRUNYAN 2021R search for t H in final states with electrons, muons and hadronically   decaying tau leptons (H --> W W^* , Z Z^* , tau tau) with 137 fb**-1 of p p   collision data at Ecm = 13 TeV. The quoted signal strength corresponds to a significance of   1.4 standard deviations and is given for mass(H) = 125 GeV.


pdgid: S126PTH
text:
AAD 2020Z search for the t H associated production using H --> gamma gamma in 139  fb**-1 of data at Ecm = 13 TeV. An upper limit on its rate is set to be 12 times the  Standard Model at 95% CL (mass(H) = 125.09 GeV).


pdgid: S126PTH
text:
SIRUNYAN 2019BK search for the t H associated production using multilepton signatures  (H --> W W^*, H --> tau tau, H --> Z Z^*) and signatures with a single lepton and a  b bbar pair (H --> b bbar) using 35.9 fb**-1 at Ecm = 13 TeV. Results are  combined with H --> gamma gamma (SIRUNYAN 2018DS). The observed 95% CL upper limit  on the t H production cross section times H --> W W^* + tau tau + Z Z^* + b bbar + gamma gamma  branching fraction is 1.94 pb (assuming SM t tbar H production cross section). See their Table  X and Fig. 14. The values outside the ranges of [-0.9, -0.5] and [1.0, 2.1] times the  standard model top quark Yukawa coupling are excluded at 95% CL.


pdgid: S126PTH
text:
KHACHATRYAN 2016AU search for the t H associated production in 19.7 fb**-1 at  Ecm = 8 TeV. The 95% CL upper limits on the t H associated production cross  section is measured to be 600 -- 1000 fb depending on the assumed gamma gamma branching  ratios of the Higgs boson. The gamma gamma branching ratio is varied to be by a factor of  0.5 -- 3.0 of the Standard Model Higgs boson (mass(H) = 125 GeV). The results of the  signal strengths for a negative Higgs-boson trilinear coupling are given. The results are given for mass(H) = 125 GeV.


pdgid: S126A02
text:
AAD 2023C combine AAD 2022N and AAD 2020BA, where both use 139 fb**-1 of p p  collisions at Ecm = 13 TeV. The Higgs production cross sections at Ecm = 7 and 8 TeV  are obtained to be 34+11-10 pb and 33.3+5.8-5.4 pb, respectively. The quoted value is  given for mass(H) = 125.09 GeV. The  differential cross sections are given in their Figs. 3 and 4.


pdgid: S126A02
text:
AAD 2022N use 139 fb**-1 of p p collisions at Ecm = 13 TeV. The quoted value is  given for mass(H) = 125.09 GeV.


pdgid: S126A02
text:
AAD 2020BA use 139 fb**-1 of p p collisions at Ecm = 13 TeV with H --> Z Z^* --> 4 lepton  where lepton = e , mu. The quoted value is given for mass(H) = 125 GeV and assumes the  Standard Model branching ratio.


pdgid: S126A02
text:
AABOUD 2017CO use 36.1 fb**-1 of p p collisions at Ecm = 13 TeV with H --> Z Z^* --> 4 lepton  where lepton = e , mu for mass(H) = 125 GeV. Differential cross sections for the Higgs  boson transverse momentum, Higgs boson rapidity, and other related quantities are measured as shown  in their Figs. 8 and 9.


pdgid: S126A03
text:
AAD 2024AQ measure the total cross section to be 67+12-11 pb and 46+-12 pb using  H --> gamma gamma and H --> Z Z^* --> 4 lepton, respectively, with data of 31.4 fb**-1  and 29.0 fb**-1 of p p collisions at Ecm = 13.6 TeV. The SM expected value is 59.9+-2.6  pb. All the values are given for mass(H) = 125.09 GeV.


pdgid: S055HAD
text:
TUMASYAN 2023S search for production of H_2()0 / A0 --> tau+ tau- by gluon fusion and  b-associated prodution using 138 fb**-1 of p p collisions at Ecm = 13 TeV. See  their Fig. 13 for excluded regions in the mass(A0)-tan(beta) plane in  M(h)**125 and M(h EFT)**125 MSSM scenarios. In both scenarios mass(A0)  < 350 GeV is excluded at 95% CL.


pdgid: S055HAD
text:
AAD 2020AA search for H_{{2}}()0/A0 --> tau+ tau- produced by gluon fusion or  b-associated production using 139 fb**-1 of p p collisions at Ecm = 13 TeV.  See  their Fig. 2(c) for excluded region in the M(h)**125  scenario of MSSM.  Values of  tan(beta) > 8 (21) are excluded for mass(A0) = 1.0 (1.5) TeV at 95%CL.


pdgid: S055HAD
text:
AAD 2024AP search for production of a heavy H_{{2}}()0 and A0 decaying to t tbar in  140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 13(b) for excluded  parameter regions in hMSSM.


pdgid: S055HAD
text:
AAD 2024CB use ATLAS measurements from up to 139 fb**-1 of H production cross  sections and decays to constrain the MSSM Higgs sector. See their Figs. 22 and 23 for excluded  regions in various MSSM scenarios.


pdgid: S055HAD
text:
AAD 2024H combine searches for a scalar resonance decaying to H H using up to 139  fb**-1 of p p collisions at Ecm = 13 TeV from AAD 2022F, AAD 2023Z, and  AAD 2022Y. See their Fig. 3 for the excluded region in the MSSM M(h,EFT)**125 and  M(h,EFT)**125(chitilde) benchmark scenarios (where only the resonant H-exchange  contribution has been taken into account in the signal modelling).


pdgid: S055HAD
text:
AAD 2020 combine measurements on H production and decay using data taken in years  2015 -- 2017 (up to 79.8 fb**-1) of p p collisions at Ecm = 13 TeV.  See their  Fig. 19 for excluded region in the hMSSM parameter space.


pdgid: S055HAD
text:
AAD 2020C combine searches for a scalar resonance decaying to H H in 36.1 fb**-1 of  p p collisions at Ecm = 13 TeV from AABOUD 2019A, AABOUD 2019O, AABOUD 2018CQ,  AABOUD 2019T, AABOUD 2018CW, and AABOUD 2018BU. See their Fig. 7(b) for the  excluded region in the hMSSM parameter space.


pdgid: S055HAD
text:
AAD 2020L search for b-associated production of H_{{2}}()0 decaying to b bbar in 27.8  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 9 for excluded regions in  hMSSM, m(h)**mod+ and m(h)**mod- scenarios of MSSM.


pdgid: S055HAD
text:
SIRUNYAN 2020AC search for gluon-fusion and b-associated production of A0 decaying to  Z H in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 6 for  excluded regions in the M(h EFT)**125 and hMSSM scenarios of the MSSM.


pdgid: S055HAD
text:
SIRUNYAN 2020AF search for H_{{2}}()0/A0 --> t tbar with one or two charged leptons in  the final state using kinematic variables in 35.9 fb**-1 of p p collisions at Ecm =  13 TeV.  See their Fig. 8 for excluded region in the hMSSM scenario of MSSM.  Values of  tan(beta) below 1.0 -- 1.5 are excluded for mass(A0) = 0.4 -- 0.75 TeV at  95%CL.


pdgid: S055HAD
text:
SIRUNYAN 2020Y search for gluon-fusion and vector-boson-fusion production of H_{{2}}()0  decaying to W+ W- in the final states lepton nu lepton nu and lepton nu q q in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Figs. 8 and 9 for excluded  regions in various MSSM scenarios.


pdgid: S055HAD
text:
SIRUNYAN 2019CR search for production of H_2()0 / A0 in gluon fusion and in association  with a b bbar pair, decaying to mu+ mu- in 35.9 fb**-1 of p p collisions at  Ecm = 13 TeV.  See their Fig. 5 for the excluded region in the MSSM parameter space in the  m(h)**mod+ and hMSSM scenarios.


pdgid: S055HAD
text:
AABOUD 2018G search for production of H_2()0 / A0 --> tau+ tau- by gluon fusion and  b-associated prodution in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See  their Fig. 10 for excluded regions in the mass(A0)- tan(beta) plane in several  MSSM scenarios.


pdgid: S055HAD
text:
SIRUNYAN 2018A search for production of a scalar resonance decaying to H0 H0 --> b bbar tau+ tau-  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 5 (lower) for  excluded regions in the mass(A0) - tan(beta) plane in the hMSSM scenario.


pdgid: S055HAD
text:
SIRUNYAN 2018BP search for production of H_2()0 / A0 --> b bbar by b-associated  prodution in 35.7 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 6 for the  limits on cross section times branching ratio for mass(H_{{2}}()0), mass(A0) = 0.3 -- 1.3 TeV,  and Fig. 7 for excluded regions in the mass(A0)- tan(beta) plane in several  MSSM scenarios.


pdgid: S055HAD
text:
SIRUNYAN 2018CX search for production of H_1,2()0 / A0 --> tau+ tau- by gluon fusion and b-associated prodution in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 9 for excluded regions in the mass(A0)- tan(beta) plane in several MSSM scenarios.


pdgid: S055HAD
text:
AABOUD 2016AA search for production of a Higgs boson in gluon fusion and in association with  a b bbar pair followed by the decay A0 --> tau+ tau- in 3.2 fb**-1 of p p  collisions at Ecm = 13 TeV. See their Fig. 5(a, b) for limits on cross section times  branching ratio for mass(A0) = 200 -- 1200 GeV, and Fig. 5(c, d) for the excluded region in  the MSSM parameter space in the m(h)**mod+ and hMSSM scenarios.


pdgid: S055HAD
text:
KHACHATRYAN 2016A search for production of a Higgs boson in gluon fusion and in association  with a b bbar pair followed by the decay H_1,2()0 / A0 --> mu+ mu- in 5.1 fb**-1 of   p p  collisions at Ecm = 7 TeV and 19.3 fb**-1 at Ecm = 8 TeV. See their Fig. 7   for the  excluded region in the MSSM parameter space in the m(h)**mod+  benchmark  scenario and Fig. 9  for limits on cross section times branching ratio.


pdgid: S055HAD
text:
KHACHATRYAN 2016P search for gluon fusion production of an H_{{2}}()0 decaying to H0 H0 --> b bbar tau+ tau-  and an A0 decaying to Z H0 --> lepton+ lepton- tau+ tau- in 19.7 fb**-1 of p p  collisions at Ecm = 8 TeV. See their Fig. 12 for excluded region in the tan(beta)  - cos(beta-alpha) plane for mass(H_{{2}}()0) = mass(A0) = 300 GeV.


pdgid: S055HAD
text:
KHACHATRYAN 2015AY search for production of a Higgs boson in association with a b quark  in the decay H_1,2()0 / A0 --> b bbar in 19.7 fb**-1 of p p collisions at Ecm  =  8 TeV and combine with CHATRCHYAN  2013AG 7 TeV data.  See their Fig. 6 for the limits on   cross section times branching ratio for mass(A0) = 100 -- 900 GeV and Figs. 7 -- 9  for the excluded region in the MSSM parameter space in various benchmark scenarios.


pdgid: S055HAD
text:
AAD 2014AW search for production of a Higgs boson followed by the decay H_1,2()0 / A0 --> tau+ tau- in 19.5--20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 11 for the limits on cross section times branching ratio and their Figs. 9 and 10 for the excluded region in the MSSM parameter space. For mass(A0) = 140 GeV, the region tan(beta)> 5.4 is excluded at 95% CL in the m(h)**max scenario.


pdgid: S055HAD
text:
KHACHATRYAN 2014M search for production of a Higgs boson in gluon fusion and in association with a b quark followed by the decay H_1,2()0 / A0 --> tau+ tau- in 4.9 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. See their Figs. 7 and 8 for one- and two-dimensional limits on cross section times branching ratio and their Figs. 5 and 6 for the excluded region in the MSSM parameter space. For mass(A0) = 140 GeV, the region tan(beta)> 3.8 is excluded at 95% CL in the m(h)**max scenario.


pdgid: S055HAD
text:
AAD 2013O search for production of a Higgs boson in the decay H_1,2()0 / A0 --> tau+ tau- and mu+ mu- with 4.7 -- 4.8 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 6 for the excluded region in  the MSSM parameter space and their Fig. 7 for the limits on cross section times branching ratio.  For mass(A0) = 110 -- 170 GeV, tan(beta) ~> 10 is excluded, and for tan(beta) = 50,  mass(A0) below 470 GeV is excluded at 95% CL in the m(h)**max scenario.


pdgid: S055HAD
text:
AAIJ 2013T search for production of a Higgs boson in the forward region in the decay H_{{1,2}}()0/A0 --> tau+ tau- in 1.0 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 2 for the limits on cross section times branching ratio and the excluded region in the MSSM parameter space.


pdgid: S055HAD
text:
CHATRCHYAN 2013AG search for production of a Higgs boson in association with a b quark in the decay H_{{1,2}}()0/A0 --> b bbar in 2.7 -- 4.8 fb**-1 of p p collisions at Ecm = 7 TeV.  See their Fig. 6 for the excluded region in the MSSM parameter space and Fig. 5 for the limits on cross section times branching ratio. For mass(A0) = 90 -- 350 GeV, upper bounds on tan(beta) of 18 -- 42 at 95% CL are obtained in the m(h)**max  scenario with mu = +200 GeV.


pdgid: S055HAD
text:
AALTONEN 2012AQ combine AALTONEN 2012X and ABAZOV 2011K. See their Table I and Fig. 1 for the limit on cross section times branching ratio and Fig. 2 for the excluded region in the MSSM parameter space.


pdgid: S055HAD
text:
AALTONEN 2012X search for associated production of a Higgs boson and a b quark in the decay H_1,2()0 / A0 --> b bbar, with 2.6 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. See their Table III and Fig. 15 for the limit on cross section times branching ratio and Figs. 17, 18 for the excluded region in the MSSM parameter space.


pdgid: S055HAD
text:
ABAZOV 2012G search for production of a Higgs boson in the decay H_1,2()0 / A0 --> tau+ tau- with 7.3 fb**-1 of p pbar collisions at Ecm = 1.96 TeV and combine with ABAZOV 2011W and ABAZOV 2011K. See their Figs. 4, 5, and 6 for the excluded region in the MSSM parameter space.  For mass(A0) = 90 -- 180 GeV, tan(beta) ~> 30 is excluded at  95% CL. in the m(h)**max scenario.


pdgid: S055HAD
text:
CHATRCHYAN 2012K search for production of a Higgs boson in the decay H_1,2()0 / A0 --> tau+ tau- with 4.6 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 3 and Table 4 for the excluded region in the MSSM parameter space. For mass(A0) = 160 GeV, the region tan(beta) > 7.1 is excluded at 95% CL in the m(h)**max scenario. Superseded by KHACHATRYAN 2014M.


pdgid: S055HAD
text:
ABAZOV 2011K search for associated production of a Higgs boson and a b quark, followed by the decay  H_{{1,2}}()0/A0 --> b bbar, in 5.2 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. See their Fig.5/Table2 for the limit on cross section times branching ratio and Fig.6  for the excluded region in the MSSM parameter space for mu =  -200 GeV.


pdgid: S055HAD
text:
ABAZOV 2011W search for associated production of a Higgs boson and a b quark, followed by the decay  H_{{1,2}}()0/A0 --> tau tau, in 7.3 fb**-1 of p pbar collisions at Ecm = 1.96 TeV.  See their Fig.2 for the limit on cross section times branching ratio and for the excluded region in the MSSM parameter space.


pdgid: S055HAD
text:
AALTONEN 2009AR search for Higgs bosons decaying to tau+ tau- in two doublet models in 1.8 fb**-1 of  p pbar collisions at Ecm = 1.96 TeV. See their Fig. 2 for the limit on sigma.B(H^0_1,2()/A0 --> tau+ tau-) for different Higgs masses, and see their Fig. 3 for the excluded region in the MSSM parameter space.


pdgid: S055HAD
text:
ABDALLAH 2008B give limits in eight CP-conserving benchmark scenarios and some CP-violating scenarios. See paper for excluded regions for each scenario. Supersedes ABDALLAH 2004.


pdgid: S055HAD
text:
SCHAEL 2006B make a combined analysis of the LEP data.  The quoted limit is for the m(h)**max scenario with mass(t) = 174.3 GeV. In the CP-violating CPX scenario no lower bound  on mass(H_{{1}}^0()) can be set at 95% CL. See paper for excluded regions in various scenarios. See Figs. 2 -- 6 and Tabs. 14 -- 21 for limits on CS(Z H0). B(H0 --> b bbar, tau+ tau-) and CS(H_1^0() H_2^0()). B(H_{{1}}^0,H_{{2}}^0()b bbar,tau+ tau-).


pdgid: S055HAD
text:
ACOSTA 2005Q search for H^0_{1,2}()/A0 production in p pbar collisions at Ecm = 1.8 TeV with H^0_{1,2}()/A0 --> tau+ tau-. At mass(A0) = 100 GeV, the obtained cross section upper limit is above theoretical expectation.


pdgid: S055HAD
text:
Search for e+ e- --> H_1()0 A0 in the final states b bbar b bbar and b bbar tau+ tau-, and e+ e- --> H_1()0 Z.  Universal scalar mass of 1TeV, SU(2) gaugino mass of 200 GeV, and mu= -200 GeV are assumed, and two-loop radiative corrections incorporated.  The limits hold for mass(t)=175 GeV, and for the m(h)**max scenario.


pdgid: S055HAD
text:
ABBIENDI 2004M exclude 0.7 < tan(beta) < 1.9, assuming mass(t) = 174.3 GeV. Limits for other MSSM benchmark scenarios, as well as for CP violating cases, are also given.


pdgid: S055HAD
text:
ABBIENDI 2003G search for e+ e- --> H_1()0 Z followed by H_1()0 --> A0 A0, A0 --> c cbar, g g, or tau+ tau-. In the no-mixing scenario, the region mass(H_{{1}}()0) = 45-85 GeV and mass(A0) = 2-9.5 GeV is excluded at 95% CL.


pdgid: S055HAD
text:
ACHARD 2002H also search for the final state H_1()0 Z --> 2A0 q qbar, A0 --> q qbar. In addition, the MSSM parameter set in the ``large-mu'' and ``no-mixing'' scenarios are examined.


pdgid: S055HAD
text:
AKEROYD 2002 examine the possibility of a light A0 with tan(beta)<1. Electroweak measurements are found to be inconsistent with such a scenario.


pdgid: S055HAD
text:
HEISTER 2002 excludes the range 0.7<tan(beta)<2.3. A wider range is excluded with different stop mixing assumptions. Updates BARATE 2001C.


pdgid: S055H2D
text:
AAD 2024AB search for gluon-fusion and b bbar associated production of A0 decaying to  A0 --> Z H_2()0, in the final states lepton+ lepton- t tbar and nu nubar b bbar using  140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 5 and 6 for limits on  cross section times branching ratios in terms of two-Higgs-doublet models, and Fig. 7 for excluded  model parameter space.


pdgid: S055H2D
text:
AAD 2024AP search for production of a heavy H_{{2}}()0 and A0 decaying to t tbar in  140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 13(a) for excluded  parameter regions in a Type II two-Higgs-doublet model.


pdgid: S055H2D
text:
AAD 2024CB use ATLAS measurements from up to 139 fb**-1 of H production cross  sections and decays to constrain two Higgs doublet models. See their Figs. 19 -- 21 for  excluded regions of 2HDM parameter space.


pdgid: S055H2D
text:
AAD 2024H combine searches for a scalar resonance decaying to H H using up to 139  fb**-1 of p p collisions at Ecm = 13 TeV from AAD 2022F, AAD 2023Z, and  AAD 2022Y. See their Fig. 2 for the excluded region in the Type-I two-Higgs-doublet model  parameter space (where only the resonant H-exchange contribution has been taken into account in the  signal modelling).


pdgid: S055H2D
text:
HAYRAPETYAN 2024H search for H_{{2}}()0 and A0 having flavor-violating couplings to t c or t u,  produced in association with top quark(s), using 138 fb**-1 of p p collisions at Ecm  = 13 TeV. For the interpretation of the data in terms of flavor-violating two-Higs-doublet models,  given in the range mass(A0) = 0.2 -- 1.0 TeV, see their Figs. 4, 5, and 6.


pdgid: S055H2D
text:
AAD 2023AD search for associated production of W/Z H_2()0 and gluon fusion production  of A0 decaying to Z H_2()0, with the decay chain H_2()0 --> H H --> b bbar b bbar,  using 139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 12 and 13 for  excluded regions in Type-I and lepton-specific 2HDMs.


pdgid: S055H2D
text:
AAD 2023BG search for production of H_{{2}}()0/A0 in association with a t tbar pair,   decaying to t tbar, using 139 fb**-1 of p p collisions at Ecm = 13 TeV.  See   their Fig. 8 for excluded regions in the parameter space of the type II 2HDM.


pdgid: S055H2D
text:
AAD 2023O search for production of an A0 in gluon-gluon fusion and in association with a  b bbar, decaying to Z H in the final states nu nubar b bbar and lepton+ lepton- b bbar using  139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 12 and 13 for excluded  regions in the parameter space in various 2HDMs.


pdgid: S055H2D
text:
AAD 2021AF search for production of a heavy H_{{2}}()0 state decaying to Z Z in the final     states lepton+ lepton- lepton^'()+ lepton^'()- and lepton+ lepton- nu nubar in 139   fb**-1 of   p p collisions at Ecm = 13 TeV. See their Figs. 6 and 7 for excluded   parameter regions of the 2HDM Type I and II.


pdgid: S055H2D
text:
AAD 2021AI search for production of an A0 in gluon-gluon fusion and in association with a  b bbar, decaying to Z H_2()0 --> lepton+ lepton- b bbar or lepton+ lepton- W+ W- in 139  fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 10 and 14 for excluded  regions in the parameter space of various 2HDMs.


pdgid: S055H2D
text:
AAD 2020 combine measurements on H0 production and decay using data taken in years  2015 -- 2017 (up to 79.8 fb**-1) of p p collisions at Ecm = 13 TeV.  See their  Fig. 18 for excluded regions in various 2HDMs.


pdgid: S055H2D
text:
AAD 2020L search for b-associated production of H_{{2}}()0 decaying to b bbar in 27.8  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Figs. 10 and 11 for excluded  regions in the flipped two Higgs doublet model.


pdgid: S055H2D
text:
SIRUNYAN 2020AA search for H_2()0 --> Z A0, A0 --> b bbar or  A0 --> Z H_2()0,  H_2()0 --> b bbar in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.  See their  Figs. 8 and 9 for excluded regions in the parameter space of Type-II two Higgs doublet model.


pdgid: S055H2D
text:
SIRUNYAN 2020Y search for gluon-fusion and vector-boson-fusion production of H_{{2}}()0  decaying to W+ W- in the final states lepton nu lepton nu and lepton nu q q in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 7 for excluded regions in  Type I and II two Higgs doublet models.


pdgid: S055H2D
text:
SIRUNYAN 2019AE search for a pseudoscalar resonance produced in association with a b bbar  pair, decaying to tau+ tau- in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.   See their Fig. 4 for cross section limits for mass(A0) = 25 -- 70 GeV and comparison with  some representative 2HDMs.


pdgid: S055H2D
text:
SIRUNYAN 2019AV search for a scalar resonance produced by gluon fusion or b associated  production, decaying to Z H0 --> lepton+ lepton- b bbar (lepton = e, mu) or nu nubar b bbar in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 6 and 7 for excluded  regions in the parameter space of various 2HDMs.


pdgid: S055H2D
text:
AABOUD 2018AH search for production of an A0 in gluon-gluon fusion and in association  with a b bbar, decaying to Z H_2()0 --> lepton+ lepton- b bbar in 36.1 fb**-1 of p p  collisions at Ecm = 13 TeV.  See their Fig. 6 for excluded regions in the parameter space of  various 2HDMs.


pdgid: S055H2D
text:
AABOUD 2018AI search for production of an A0 in gluon-gluon fusion and in association  with a b bbar, decaying to Z H0 in the final states nu nubar b bbar and lepton+ lepton- b bbar in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Figs. 7 and 8 for excluded  regions in the parameter space in various 2HDMs.


pdgid: S055H2D
text:
AABOUD 2018BF search for production of a heavy H_{{2}}()0 state decaying to Z Z in the  final states lepton+ lepton- lepton+ lepton- and lepton+ lepton- nu nubar in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 8 and 9 for excluded  parameter regions in 2HDM Type I and II.


pdgid: S055H2D
text:
AABOUD 2018CE search for the process p p --> H_2()0 / A0 t tbar followed by the decay  H_2()0 / A0 --> t tbar in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV.  See  their Fig. 12 for limits on cross section times branching ratio, and for lower limits on  tan(beta) for mass(H_{{2}}()0), mass(A0) = 0.4 -- 1.0 TeV in the 2HDM type II.


pdgid: S055H2D
text:
HALLER 2018 perform global fits in the framework of two-Higgs-doublet models (type I, II,  lepton specific, flipped).  See their Fig. 8 for allowed parameter regions from fits to LHC H0  measurements, Fig. 9 bottom and charm decays, Fig. 10 muon anomalous magnetic moment, Fig. 11  electroweak precision data, and Fig. 12 by combination of all data.


pdgid: S055H2D
text:
SIRUNYAN 2018BP search for production of H_2()0 / A0 --> b bbar by b-associated  prodution in 35.7 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 6 for the  limits on cross section times branching ratio for mass(H_{{2}}()0), mass(A0) = 0.3 -- 1.3 TeV,  and Figs. 8 and 9 for excluded regions in the parameter space of type-II and flipped 2HDMs.


pdgid: S055H2D
text:
SIRUNYAN 2018ED search for production of an A0 in gluon-gluon fusion and in association  with a b bbar, decaying to Z H0 in the final states nu nubar b bbar or lepton+ lepton- b bbar  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 9 for excluded  regions in the parameter space in Type I and II 2HDMs.


pdgid: S055H2D
text:
AABOUD 2017AN search for production of a heavy H_2()0 and/or A0 decaying to t tbar in 20.3  fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 3 and Table III for excluded  parameter regions in Type II Two-Higgs-Doublet-Models.


pdgid: S055H2D
text:
SIRUNYAN 2017AX search for A0 b bbar production followed by the decay A0 --> mu+ mu-  in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. Limits are set in the range  mass(A0) = 25 -- 60 GeV. See their Fig. 5 for upper limits on CS(A0 b bbar).B(A0 --> mu+ mu-).


pdgid: S055H2D
text:
AAD 2016AX search for production of a heavy H0 state decaying to Z Z in the final  states lepton+ lepton- lepton+ lepton-, lepton+ lepton- nu nubar, lepton+ lepton- q qbar, and  nu nubar q qbar in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Figs.  13 and 14 for excluded parameter regions in Type I and II models.


pdgid: S055H2D
text:
KHACHATRYAN 2016P search for gluon fusion production of an H_{{2}}()0 decaying to H0 H0 --> b bbar tau+ tau-  and an A0 decaying to Z H0 --> lepton+ lepton- tau+ tau- in 19.7 fb**-1 of p p  collisions at Ecm = 8 TeV. See their Fig. 11 for limits on tan(beta) for mass(A0) =  230 -- 350 GeV.


pdgid: S055H2D
text:
KHACHATRYAN 2016W search for A0 b bbar production followed by the decay A0 --> tau+ tau- in  19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 3 for upper limits on  sigma(A0 b bbar).B(A0 --> tau+ tau-).


pdgid: S055H2D
text:
KHACHATRYAN 2016Z search for H_2()0 --> Z A0 followed by A0 --> b bbar or tau+ tau-, and  A0 --> Z H_2()0 followed by H_2()0 --> b bbar or tau+ tau-, in 19.8 fb**-1 of p p  collisions at Ecm = 8 TeV. See their Fig. 4 for cross section limits and Fig. 5 for excluded  region in the parameter space.


pdgid: S055H2D
text:
AAD 2015BK search for production of a heavy H_{{2}}()0 decaying to H0 H0 in the final  state b bbar b bbar in 19.5 fb**-1 of p p collisions at Ecm = 8 TeV. See their  Figs. 15 -- 18 for excluded regions in the parameter space.


pdgid: S055H2D
text:
AAD 2015S search for production of A0 decaying to Z H0 --> lepton+ lepton- b bbar,   nu nubar b bbar and  lepton+ lepton- tau+ tau- in 20.3 fb**-1 of p p  collisions  at  Ecm = 8 TeV.  See  their Figs. 4 and 5 for excluded regions in the parameter  space.


pdgid: S055H2D
text:
KHACHATRYAN 2015BB search for H_2()0 , A0 --> gamma gamma in 19.7 fb**-1 of p p   collisions at Ecm = 8 TeV.  See their Fig. 10 for  excluded regions in the two-Higgs-doublet   model parameter space.


pdgid: S055H2D
text:
KHACHATRYAN 2015N search for production of A0 decaying to    Z H0 --> lepton+ lepton- b bbar in   19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 5 for excluded regions  in the tan(beta) -  cos(beta-alpha) plane for mass(A0) =  300  GeV.


pdgid: S055H2D
text:
AAD 2014M search for the decay cascade H_2()0 --> H+- W-+ --> H0 W+- W-+, H0 decaying to b bbar in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Table IV for limits in a two-Higgs-doublet model for mass(H_{{2}}()0)= 325 -- 1025 GeV and mass(H+)= 225 -- 825 GeV.


pdgid: S055H2D
text:
KHACHATRYAN 2014Q search for H_2()0 --> H0 H0 and A0 --> Z H0 in 19.5 fb**-1 of  p p collisions at Ecm = 8 TeV. See their Figs. 4 and 5 for limits on cross section times  branching ratio for m(H_{{2}}(),A0)= 260 -- 360 GeV and their Figs. 7 -- 9 for  limits in two-Higgs-doublet models.


pdgid: S055H2D
text:
ABBIENDI 2005A search for e+ e- --> H_1^0() A^0() in general Type-II two-doublet models, with decays H_{{1}}^0(), A^0() --> q qbar, g g, tau+ tau-, and H_1^0() --> A^0() A^0().


pdgid: S055H2D
text:
ABDALLAH 2005D search for e+ e- --> H^0() Z and H^0() A^0() with H^0(), A^0() decaying to two jets of any flavor including g g. The limit is for SM H^0() Z production cross section with B(H^0() --> j j) = 1.


pdgid: S055H2D
text:
ABDALLAH 2004O search for Z --> b bbar H0, b bbar A0, tau+ tau- H0 and tau+ tau- A0 in the final states 4 b, b bbar tau+ tau-, and 4 tau. See paper for limits on Yukawa couplings.


pdgid: S055H2D
text:
ABDALLAH 2004O search for e+ e- --> H0 Z and H0 A0, with H0, A0 decaying to b bbar, tau+ tau-, or H0 --> A0 A0 at Ecm = 189 -- 208 GeV. See paper for limits on couplings.


pdgid: S055H2D
text:
ABBIENDI 2002D search for Z --> b bbar H_1()0 and b bbar A0 with H_1()0/A0 --> tau+ tau-, in the range 4<mass(H)<12 GeV. See their Fig.8 for limits on the Yukawa coupling.


pdgid: S055H2D
text:
ABBIENDI 2001E search for neutral Higgs bosons in general Type-II two-doublet models, at Ecm<=189 GeV.  In addition to usual final states, the decays H_{{1}}()0, A0 --> q qbar, g g are searched for. See their Figs.15,16 for excluded regions.


pdgid: S055H2D
text:
ABBIENDI 1999E search for e+ e- --> H0 A0 and H0 Z at Ecm = 183 GeV.  The limit is with mass(H)=mass(A) in general two Higgs-doublet models. See their Fig.18 for the exclusion limit in the mass(H)-mass(A) plane. Updates the results of ACKERSTAFF 1998S.


pdgid: S055H2D
text:
See Fig.4 of ABREU 1995H for the excluded region in the mass(H0)-mass(A0) plane for general two-doublet models. For tan(beta)>1, the region mass(H0)+mass(A0)~<87 GeV, mass(H0)<47 GeV is excluded at 95% CL.


pdgid: S055H2D
text:
PICH 1992 analyse H0 with mass(H0)< 2mass(mu) in general two-doublet models. Excluded regions in the space of mass-mixing angles from LEP, beam dump, and pi+-, eta rare decays are shown in Figs.3,4.  The considered mass region is not totally excluded.


pdgid: S055H2F
text:
AALTONEN 2013K search for H0 --> W W^(*)() in 9.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. A limit on cross section times branching ratio which corresponds to (1.3 -- 6.6) times the expected cross section is given in the range mass(H0) = 110 -- 200 GeV at 95% CL.


pdgid: S055H2F
text:
AALTONEN 2013L combine all CDF searches with 9.45 -- 10.0 fb**-1 of p pbar collisions at Ecm = 1.96 TeV.


pdgid: S055H2F
text:
AALTONEN 2013M combine all Tevatron data from the CDF and D0 Collaborations of p pbar collisions at Ecm = 1.96 TeV.


pdgid: S055H2F
text:
ABAZOV 2013G search for H0 --> W W^(*)() in 9.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. A limit on cross section times branching ratio which corresponds to (2 -- 9) times the expected cross section is given for mass(H0) = 100 -- 200 GeV at 95% CL.


pdgid: S055H2F
text:
ABAZOV 2013I search for H0 production in the final state with one lepton and two or more jets plus missing E(T) in 9.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. The search is sensitive to W H0, Z H0 and vector-boson fusion Higgs production with H0 --> W W^(*)(). A limit on cross section times branching ratio which corresponds to (8 -- 30) times the expected cross section is given in the range mass(H0) = 100 -- 200 GeV at 95% CL.


pdgid: S055H2F
text:
ABAZOV 2013J search for H0 production in the final states e e mu, e mu mu, mu tau tau, and e+- mu+- in 8.6 -- 9.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. The search is sensitive to W H0, Z H0 production with H0 --> W W^(*)(), Z Z^(*)(), decaying to leptonic final states. A limit on cross section times branching ratio which corresponds to (2.4 -- 13.0) times the expected cross section is given in the range mass(H0) = 100 -- 200 GeV at 95% CL.


pdgid: S055H2F
text:
CHATRCHYAN 2013AL search for H0 --> gamma gamma in 5.1 fb**-1 and 5.3 fb**-1 of p p collisions at Ecm = 7 and 8 TeV.


pdgid: S055H2F
text:
AAD 2012N search for H0 --> gamma gamma with 4.9 fb**-1 of p p collisions at Ecm = 7 TeV in the mass range mass(H0) = 110 -- 150 GeV.


pdgid: S055H2F
text:
AALTONEN 2012AN search for H0 --> gamma gamma with 10 fb**-1 of p pbar collisions at Ecm = 1.96 TeV in the mass range mass(H0) = 100 -- 150 GeV.


pdgid: S055H2F
text:
CHATRCHYAN 2012AO use data from CHATRCHYAN 2012G, CHATRCHYAN 2012E, CHATRCHYAN 2012H,  CHATRCHYAN 2012I, CHATRCHYAN 2012D, and CHATRCHYAN 2012C.


pdgid: S055H2F
text:
AALTONEN 2009AB search for H0 --> gamma gamma in 3.0 fb**-1 of p pbar collisions at Ecm = 1.96 TeV in the mass range mass(H0) = 70 -- 150 GeV. Associated H0 W, H0 Z production and W W, Z Z fusion  are considered.


pdgid: S055H2F
text:
ABAZOV 2008U search for H0 --> gamma gamma in p pbar collisions at Ecm = 1.96 TeV in the mass range mass(H0) = 70 -- 150 GeV. Associated H0 W, H0 Z production and W W, Z Z fusion are considered. See their Tab. 1 for the limit on sigma.B(H0 --> gamma gamma), and see their Fig. 3 for the excluded region in the mass(H0) -- B(H0 --> gamma gamma) plane.


pdgid: S055H2F
text:
SCHAEL 2007 search for Higgs bosons in association with a fermion pair and decaying to W W^*.  The limit is from this search and HEISTER 2002L for a H0 with SM production cross section.


pdgid: S055H2F
text:
Search for associated production of a gamma gamma resonance with a Zboson, followed by Z --> q qbar,  lepton+ lepton-, or nu nubar, at Ecm<=209 GeV.  The limit is for a H0 with SM production cross section.


pdgid: S055H2F
text:
ACHARD 2003C search for e+ e- --> Z H0 followed by H0 --> W W^* or Z Z^* at Ecm= 200-209 GeV and combine with the ACHARD 2002C result. The limit is for a H0 with SM production cross section.  For B(H0 --> W W^*) + B(H0 --> Z Z^*) = 1, m(H0) > 108.1 GeV is obtained. See fig.6 for the limits under different BR assumptions.


pdgid: S055H2F
text:
ACHARD 2002C search for associated production  of a gamma gamma resonance with a Z boson, followed by Z --> q qbar, lepton+ lepton-, or nu nubar, at Ecm<=209 GeV. The limit is for a H()0 with SM production cross section. For B(H()0 --> gamma gamma)=1, mass(H()0)>114 GeV is obtained.


pdgid: S055H2F
text:
AFFOLDER 2001H search for associated production of a gamma gamma resonance and a W or Z (tagged by two jets, an isolated lepton, or missing E(T)). The limit assumes Standard Model values for the production cross section and for the couplings of the H0 to W and Z bosons.  See their Fig.11 for limits with B(H0 --> gamma gamma)<1.


pdgid: S055H2F
text:
ACCIARRI 2000S search for associated production of a gamma gamma resonance with a q qbar, nu nubar, or lepton+ lepton- pair in e+ e- collisions at Ecm= 189GeV.  The limit is for a H0 with SM production cross section. For B(H0 --> gamma gamma)=1, mass(H0)>98GeV is obtained.  See their Fig.5 for limits on B(H --> gamma gamma).sigma(e+ e- --> H f fbar)/sigma(e+ e- --> H f fbar) (SM).


pdgid: S055H2F
text:
BARATE 2000L search for associated production of a gamma gamma resonance with a q qbar, nu nubar, or lepton+ lepton- pair in e+ e- collisions at Ecm= 88 -- 202GeV.  The limit is for a H0 with SM production cross section. For B(H0 --> gamma gamma)=1, mass(H0)>109GeV is obtained.  See their Fig.3 for limits on B(H --> gamma gamma).sigma(e+ e- --> H f fbar)/sigma(e+ e- --> H f fbar) (SM).


pdgid: S055H2F
text:
ABBIENDI 1999o search for associated production of a gamma gamma resonance with a q qbar, nu nubar, or lepton+ lepton- pair in e+ e- collisions at 189 GeV.  The limit is for a H0 with SM production cross section. See their Fig.4 for limits on sigma(e+ e- --> H0 Z0)*B(H0 --> gamma gamma)*B(X0 --> f fbar) for various masses. Updates the results of ACKERSTAFF 1998Y.


pdgid: S055H2F
text:
ABBOTT 1999B search for associated production of a gamma gamma resonance and a dijet pair.  The limit assumes Standard Model values for the production cross section and for the couplings of the H0 to W and Z bosons.  Limits in the range of CS(H0+Z/W).B(H0 --> gamma gamma)= 0.80 -- 0.34pb are obtained in the mass range mass(H0)= 65 -- 150 GeV.


pdgid: S055H2F
text:
ABREU 1999P search for e+ e- --> H0 gamma with H0 --> b bbar or gamma gamma, and e+ e- --> H0 q qbar with H0 --> gamma gamma. See their Fig.4 for limits on sigma*B.  Explicit limits within an effective interaction framework are also given.


pdgid: S055H2I
text:
AABOUD 2019AI search for H_{{{1,2}}}()0 production by vector boson fusion and decay to  invisible final states in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV.  See their  Fig. 6(b) for limits on cross section times branching ratios for mass(H_{{{1,2}}}()0) = 0.1 -- 3 TeV.


pdgid: S055H2I
text:
AAD 2015BD search for p p --> H0 W X and p p --> H0 Z X with W or Z decaying  hadronically and H0 decaying to invisible final states in 20.3 fb**-1 at Ecm = 8TeV.  See their Fig. 6 for a limit on the cross section times branching ratio for mass(H0) = 115 -- 300 GeV.


pdgid: S055H2I
text:
AAD 2015BH search for events with a jet and missing E(T) in 20.3 fb**-1 of p p  collisions at Ecm = 8 TeV. Limits on CS(H^'()0) B(H^'()0 --> invisible)  < (44 -- 10) pb (95%CL) is given for mass(H^'()0) = 115 -- 300 GeV.


pdgid: S055H2I
text:
AAD 2014BA search for H0 production in the decay mode H0 --> X0 X0, where X0 is a long-lived particle which decays to collimated pairs of e+ e-, mu+ mu-, or pi+ pi- plus invisible particles, in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Figs. 15 and 16 for limits on cross section times branching ratio.


pdgid: S055H2I
text:
AAD 2014O search for p p --> H0 Z X, Z --> lepton lepton, with H0 decaying to invisible final states in 4.5 fb**-1 at Ecm = 7 TeV and 20.3 fb**-1 at Ecm = 8 TeV. See their Fig. 3 for a limit on the cross section times branching ratio for mass(H0) = 110 -- 400 GeV.


pdgid: S055H2I
text:
CHATRCHYAN 2014B search for p p --> H0 Z X, Z --> lepton lepton and Z --> b bbar, and also p p --> q q H0 X with H0 decaying to invisible final states using data at Ecm = 7 and 8 TeV. See their Figs. 10, 11 for limits on the cross section times branching ratio for mass(H0) = 100 -- 400 GeV.


pdgid: S055H2I
text:
AAD 2013AG search for H0 production in the decay mode H0 --> X0 X0, where X0 is a long-lived particle which decays to mu+ mu- X^'()0, in 1.9 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 7 for limits on cross section times branching ratio.


pdgid: S055H2I
text:
AAD 2013AT search for H0 production in the decay H0 --> X0 X0, where X0 eventually decays to clusters of collimated e+ e- pairs, in 2.04 fb**-1 of p p collisions at Ecm = 7 TeV.  See their Fig. 3 for limits on cross section times branching ratio.


pdgid: S055H2I
text:
CHATRCHYAN 2013BJ search for H0 production in the decay chain H0 --> X0 X0, X0 --> mu+ mu- X^'()0 in 5.3 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 2 for limits on cross section times branching ratio.


pdgid: S055H2I
text:
AAD 2012AQ search for H0 production in the decay mode H0 --> X0 X0, where X0 is a long-lived particle which decays  mainly to b bbar in the muon detector, in 1.94 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 3 for limits on cross section times branching ratio for mass(H0) = 120, 140 GeV, mass(X0) = 20, 40 GeV in the ctau range of 0.5 -- 35 m.


pdgid: S055H2I
text:
AALTONEN 2012AB search for H0 production in the decay H0 --> X0 X0, where X0 eventually decays to clusters of collimated lepton+ lepton- pairs, in 5.1 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. Cross section limits are provided for a benchmark MSSM model incorporating the parameters given in Table VI.


pdgid: S055H2I
text:
AALTONEN 2012U search for H0 production in the decay mode H0 --> X0 X0, where X0 is a long-lived particle with ctau ~~ 1 cm which decays mainly to b bbar, in 3.2 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. See their Figs. 9 and 10 for limits on cross section times branching ratio for mass(H0) = (130 -- 170) GeV, mass(X0) = 20, 40 GeV.


pdgid: S055H2I
text:
ABBIENDI 2010 search for e+ e- --> H0 Z with H0 decaying invisibly.  The limit assumes SM production cross section and B(H0 --> invisible) = 1.


pdgid: S055H2I
text:
ABBIENDI 2007 search for e+ e- --> H0 Z with Z --> q qbar and H0 decaying to invisible final states. The H0 width is varied between 1 GeV and 3 TeV.  A limit sigma.B(H0 --> invisible) < (0.07 -- 0.57) pb (95%CL)  is obtained at Ecm = 206 GeV for mass(H0) = 60 -- 114GeV.


pdgid: S055H2I
text:
Search for e+ e- --> H0 Z with H0 decaying invisibly.  The limit assumes SM production cross section and B(H0 --> invisible) = 1.


pdgid: S055H2I
text:
ACCIARRI 2000M search for e+ e- --> Z H0 with H0 decaying invisibly at Ecm=183 -- 189GeV. The limit assumes SM production cross section and B(H0 --> invisible)=1. See their Fig. 6 for limits for smaller branching ratios.


pdgid: S055H2A
text:
ADACHI 2023A search for flavor-changing tau decays tau --> e A0 and tau --> mu A0, with   A0 invisible, using 62.8 fb**-1 of e+ e- collisions at Ecm = 10.58 GeV.  Limits  on B(tau --> e A0)/B(tau --> e nu nu) in the range 1.1E-3 -- 9.7E-3 (95%  CL) and B(tau --> mu A0)/B(tau --> mu nu nu) in the range 0.7E-3 -- 12.2E-3  (95% CL) are given for mass(A0) = 0 -- 1.6 GeV. See their Fig. 2.


pdgid: S055H2A
text:
TUMASYAN 2023AR search for the decay H --> A0 A0 with A0 --> gamma gamma (detected as  a merged photonlike object) using 136 fb**-1 of p p collisions at Ecm = 13 TeV.  Limits on B(H --> A0 A0).B**2(A0 --> gamma gamma) in the range 0.9E-3 -- 3.3E-3  (95% CL) are given for mass(A0) = 0.1 -- 1.2 GeV. See their Fig. 2.


pdgid: S055H2A
text:
ABLIKIM 2022H search for the process J/psi --> A0 gamma with A0 decaying to mu+ mu- in 9E9  J/psi events and  give limits on B(J/psi --> A0 gamma).B(A0 --> mu+ mu-)  in the range  1.2E-9 -- 7.78E-7 (90% CL) for 0.212 GeV <= mass(A0)<= 3.0  GeV. See their  Fig. 4.


pdgid: S055H2A
text:
JIA 2022 search for the process Upsilon(2S) --> Upsilon(1S) pi+ pi- --> A0 gamma pi+ pi-    with A0 decaying to tau+ tau- or mu+ mu- in 158E6 Upsilon(2S) events and  give  limits on B(Upsilon(1S) --> A0 gamma).B(A0 --> tau+ tau-) in the  range   3.8E-6 -- 1.5E-4 (90% CL) for mass(A0) = 3.6 -- 9.2 GeV, and    B(Upsilon(1S) --> A0 gamma).B(A0 --> mu+ mu-) in the range 3.1E-7 -- 1.6E-5    (90% CL) for mass(A0) = 0.21 -- 9.2 GeV. See their Fig. 4.


pdgid: S055H2A
text:
AAD 2020AE search for the decay H0 --> Z A0, Z --> lepton+ lepton-, A0 decaying  hadronically (A0 --> g g or s sbar), in 139 fb**-1 of p p collisions at Ecm =  13 TeV. Limit on the product of production cross section and the H0 --> Z A0 branching ratio in  the range 17 -- 340 pb (95% CL) is given for mass(A0) = 0.5 -- 4.0 GeV, see  their Table I.


pdgid: S055H2A
text:
AABOUD 2018AP search for the decay H0 --> A0 A0 --> mu+ mu- mu+ mu- in 36.1 fb**-1 of  p p collisions at Ecm = 13 TeV. See their Fig. 10(b) for limits on B(H0 --> A0 A0)  in the range mass(A0) = 1 -- 2.5, 4.5 -- 8 GeV, assuming a type-II two-doublet plus  singlet model with tan(beta) = 5.


pdgid: S055H2A
text:
KHACHATRYAN 2017AZ search for the decay H0 --> A0 A0 --> tau+ tau- tau+ tau-, mu+ mu- b bbar,  and mu+ mu- tau+ tau- in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their  Figs. 4, 5, and 6 for cross section limits in the range mass(A0) = 5 -- 62.5 GeV. See also  their Figs. 7, 8, and 9 for interpretation of the data in terms of models with two Higgs doublets  and a singlet.


pdgid: S055H2A
text:
ABLIKIM 2016E search for the process J/psi --> A0 gamma with  A0 decaying to mu+ mu- and  give limits on B(J/psi --> A0 gamma).B(A0 --> mu+ mu-) in the  range  2.8E-8 -- 5.0E-6 (90% CL) for 0.212 <= mass(A0)<= 3.0 GeV. See their Fig.  5.


pdgid: S055H2A
text:
KHACHATRYAN 2016F search for the decay H0 --> A0 A0 --> tau+ tau- tau+ tau- in 19.7  fb**-1 of p  p collisions at Ecm = 8 TeV. See their Fig. 8 for cross section limits  for mass(A0) = 4 -- 8 GeV.


pdgid: S055H2A
text:
LEES 2015H search for the process Upsilon(2S) --> Upsilon(1S) pi+ pi- --> A0 gamma pi+ pi- with  A0 decaying to c cbar and give limits on B(Upsilon(1S) --> A0 gamma).B(A0 --> c cbar) in  the range 7.4E-5 -- 2.4E-3 (90% CL) for 4.00 <= mass(A0)<= 8.95 and  9.10 <= mass(A0)<= 9.25 GeV. See their Fig. 6.


pdgid: S055H2A
text:
LEES 2013C search for the process Upsilon(2S, 3S)Upsilon(1S) pi+ pi- --> A0 gamma pi+ pi- with A0 decaying to  mu+ mu- and give limits on B(Upsilon(1S) --> A0 gamma).B(A0 --> mu+ mu-) in the range (0.3 -- 9.7)xE-6  (90% CL) for 0.212 <= mass(A0) <= 9.20 GeV. See their Fig. 5(e) for limits on the b-A0 Yukawa coupling  derived by combining this result with AUBERT 2009Z.


pdgid: S055H2A
text:
LEES 2013L search for the process Upsilon(2S) --> Upsilon(1S) pi+ pi- --> A0 gamma pi+ pi- with A0 decaying to g g or s sbar and give limits on B(Upsilon(1S) --> A0 gamma).B(A0 --> g g) between 1E-6 and 2E-2 (90% CL) for 0.5 <= mass(A0) <= 9.0 GeV, and B(Upsilon(1S) --> A0 gamma).B(A0 --> s sbar) between 4E-6 and 1E-3 (90%CL) for 1.5 <= mass(A0) <= 9.0 GeV. See their Fig. 4.


pdgid: S055H2A
text:
LEES 2013R search for the process Upsilon(2S) --> Upsilon(1S) pi+ pi- --> A0 gamma pi+ pi- with A0 decaying to tau+ tau- and give limits on B(Upsilon(1S) --> A0 gamma).B(A0 --> tau+ tau-) in the range 0.9 -- 13E-5 (90% CL) for 3.6 <= mass(A0)<= 9.2 GeV. See their Fig. 4 for limits on the b-A0 Yukawa coupling derived by combining this result with AUBERT 2009P.


pdgid: S055H2A
text:
ABLIKIM 2012 searches for the process psi(3686) --> pi pi J/psi, J/psi --> A0 gamma  with A0 decaying to mu+ mu-. It gives mass dependent limits on B(J/psi --> A0 gamma).B(A0 --> mu+ mu-) in the  range 4E-7 -- 2.1E-5 (90% C.L.) for 0.212 <= mass(A0)<= 3.0 GeV. See  their Fig. 2.


pdgid: S055H2A
text:
CHATRCHYAN 2012V search for A0 production in the decay A0 --> mu+ mu- with 1.3 fb**-1 of p p collisions at  Ecm = 7 TeV. A limit on sigma(A0).B(A0 --> mu+ mu-) in the range (1.5 -- 7.5) pb is given  for mass(A0) = (5.5 -- 8.7) and (11.5 -- 14) GeV at 95% CL.


pdgid: S055H2A
text:
AALTONEN 2011P search in 2.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV for the decay chain t --> b H+,  H+ --> W+ A0, A0 --> tau+ tau- with mass(A0) between 4 and 9 GeV. See their Fig.4 for limits on  B(t --> b H+) for 90 < mass(H+)< 160 GeV.


pdgid: S055H2A
text:
ABOUZAID 2011A search for the decay chain K_L --> pi0 pi0 A0, A0 --> mu+ mu- and give a limit B(K_L --> pi0 pi0 A0) . B(A0 --> mu+ mu-) < 1.0E-10 at 90% CL for mass(A0) = 214.3 MeV.


pdgid: S055H2A
text:
DEL-AMO-SANCHEZ 2011J search for the process Upsilon(2S) --> Upsilon(1S) pi+ pi- --> A0 gamma pi+ pi- with A0  decaying to invisible final states. They give limits on B(Upsilon(1S) --> A0 gamma).B(A0 --> invisible)  in the range (1.9 -- 4.5)xE-6 (90% CL) for 0 <= mass(A0) <= 8.0 GeV, and  (2.7 -- 37)xE-6 for 8.0 <= mass(A0) <= 9.2 GeV.


pdgid: S055H2A
text:
LEES 2011H search for the process Upsilon(2S,3S) --> A0 gamma with A0 decaying hadronically and give limits on B(Upsilon(2S,3S) --> A0 gamma).B(A0 --> hadrons) in the range 1E-6 -- 8E-5 (90% CL) for  0.3 < mass(A0) < 7 GeV. The decay rates for Upsilon(2S) and Upsilon(3S) are assumed to be equal  up to the phase space factor. See their Fig. 5.


pdgid: S055H2A
text:
ANDREAS 2010 analyze constraints from rare decays and other processes on a light A0 with mass(A0) < 2mass(mu) and give limits on its coupling to fermions at the level of E-4 times the Standard Model value.


pdgid: S055H2A
text:
HYUN 2010 search for the decay chain B0 --> K^*()0 A0, A0 --> mu+ mu- and give a limit on B(B0 --> K^*()0 A0) . B(A0 --> mu+ mu-) in the range (2.26 -- 5.53)xE-8 at 90%CL for  mass(A0) = 212 -- 300 MeV. The limit for mass(A0) = 214.3 MeV is 2.26E-8.


pdgid: S055H2A
text:
HYUN 2010 search for the decay chain B0 --> rho0 A0, A0 --> mu+ mu- and give a limit on B(B0 --> rho0 A0) . B(A0 --> mu+ mu-) in the range (1.73 -- 4.51)xE-8 at 90%CL for  mass(A0) = 212 -- 300 MeV. The limit for mass(A0) = 214.3 MeV is 1.73E-8.


pdgid: S055H2A
text:
AUBERT 2009P search for the process Upsilon(3S) --> A0 gamma with A0 --> tau+ tau- for 4.03 < mass(A0)< 9.52 and 9.61 < mass(A0)< 10.10 GeV, and give limits on B(Upsilon(3S) --> A0 gamma).B(A0 --> tau+ tau-) in the range (1.5 -- 16)xE-5 (90% CL).


pdgid: S055H2A
text:
AUBERT 2009Z search for the process Upsilon(2S) --> A0 gamma with A0 --> mu+ mu- for 0.212 < mass(A0) < 9.3 GeV and give limits on B(Upsilon(2S) --> A0 gamma).B(A0 --> mu+ mu-) in the range (0.3 -- 8)xE-6 (90% CL).


pdgid: S055H2A
text:
AUBERT 2009Z search for the process Upsilon(3S) --> A0 gamma with A0 --> mu+ mu- for 0.212 < mass(A0) < 9.3 GeV and give limits on B(Upsilon(3S) --> A0 gamma).B(A0 --> mu+ mu-) in the range (0.3 -- 5)xE-6 (90% CL).


pdgid: S055H2A
text:
TUNG 2009 search for the decay chain K_L --> pi0 pi0 A0, A0 --> gamma gamma and give a limit on B(K_L --> pi0 pi0 A0) . B(A0 --> gamma gamma) in the range (2.4 -- 10.7)xE-7 at 90%CL for mass(A0) = 194.3 -- 219.3 MeV. The limit for mass(A0) = 214.3 MeV is 2.4E-7.


pdgid: S055H2A
text:
LOVE 2008 search for the process Upsilon(1S) --> A0 gamma with A0 --> mu+ mu- (for mass(A0) < 2mass(tau)) and A0 --> tau+ tau-. Limits on B(Upsilon(1S) --> A0 gamma) . B(A0 --> lepton+ lepton-) in the range E-6 -- E-4 (90% CL) are given.


pdgid: S055H2A
text:
BESSON 2007 give a limit B(Upsilon(1S) --> eta_b gamma) . B(eta_b --> tau+ tau-)  < 0.27% (95% CL), which constrains a possible A0 exchange contribution to the eta_{{b}} decay.


pdgid: S055H2A
text:
PARK 2005 found three candidate events for Sigma+ --> p mu+ mu- in the HyperCP experiment. Due to a narrow spread in dimuon mass, they hypothesize the events as a possible signal of a new boson. It can be interpreted as a neutral particle with mass(A0) = 214.3+-0.5MeV and the branching fraction B(Sigma+ --> p A0).B(A0 --> mu+ mu-) = (3.1+2.4-1.9+-1.5)x10**-8.


pdgid: S055H2A
text:
BALEST 1995 give limits B(Upsilon(1S) --> A0 gamma) < 1.5E-5 at 90% CL for   mass(A0)< 5 GeV.  The limit becomes <10**-4 for mass(A0) <7.7  GeV.


pdgid: S055H2A
text:
ANTREASYAN 1990C give limits B(Upsilon(1S) --> A0 gamma) < 5.6E-5 at 90% CL   for mass(A0)< 7.2 GeV.  A0 is assumed not to decay in the detector.


pdgid: S055H2O
text:
HAYRAPETYAN 2025A search for the decay H_1()0 --> gamma gamma in 132 fb**-1 of p p  collisions at Ecm = 13 TeV.  See their Fig. 5 for limits on cross section times branching  ratio for mass(H_{{1}}()0) = 70 -- 110 GeV.


pdgid: S055H2O
text:
AAD 2024A search for the decay H_2()0 --> Z gamma with Z decaying to e+ e- or  mu+ mu- using 140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 4 for  limits on production cross section times branching ratios for mass(H_{{2}}()0) = 0.22 -- 3.4  TeV.


pdgid: S055H2O
text:
AAD 2024AP search for production of a heavy H_{{2}}()0 or A0 decaying to t tbar in  140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 15 and 16 for limits on  the Yukawa coupling for mass(A0), mass(H_{{2}}()0) = 0.4 -- 1.4 TeV for different assumptions  on width over mass.


pdgid: S055H2O
text:
AAD 2024BQ search for the decay chain H --> A0 A0 --> b bbar tau+ tau-, produced by gluon  fusion, vector boson fusion, or in association with a weak vector boson, in 140 fb**-1 of p p  collisions at Ecm = 13 TeV. See their Fig. 10 for limits on the product of branching ratios  in the range mass(A0) = 12 -- 60 GeV.


pdgid: S055H2O
text:
AAD 2024BV search for H_{{2}}()0 produced by vector-boson fusion, decaying to H H --> b bbar b bbar, using  140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for limits on the  product of production cross section times branching ratios for mass(H_{{2}}()0) = 1 -- 5 TeV.


pdgid: S055H2O
text:
AAD 2024BW search for production of H_{{3}}()0 decaying to H_2()0 H, H_2()0 --> W+ W-  or Z Z, and H --> gamma gamma using 140 fb**-1 of p p collisions at Ecm = 13  TeV. See their Figs. 6 -- 8 for limits on production cross section times branching ratios in  the ranges mass(H_{{3}}()0) = 0.3 -- 1.0 TeV and mass(H_{{2}}()0) = 0.17 -- 0.5 TeV.


pdgid: S055H2O
text:
AAD 2024BX search for production of H_{{4}}()0 decaying to H_2()0 H_3()0, H_2()0 --> invisible,  and H_3()0 --> Z Z --> 4 lepton, using 139 fb**-1 of p p collisions at Ecm = 13  TeV. See their Fig. 8 (a), (b) for limits on production cross section times branching ratios in the  ranges mass(H_{{4}}()0) = 0.39 -- 1.3 TeV, mass(H_{{3}}()0) = 0.22 -- 1.0 TeV, and  mass(H_{{2}}()0) = 160 GeV.


pdgid: S055H2O
text:
AAD 2024BX search for production of A0 decaying to H_2()0 Z, H_2()0 --> Z Z,  resulting in 4 lepton final states, using 139 fb**-1 of p p collisions at Ecm =  13 TeV. See their Fig. 8 (c), (d) for limits on production cross section times branching ratios in  the ranges mass(A0) = 0.32 -- 1.3 TeV and mass(H_{{2}}()0) = 0.22 -- 1.0 TeV.


pdgid: S055H2O
text:
AAD 2024CA search for production of H_{{3}}()0 decaying to H_1,2()0 H, H_1,2()0 --> b bbar,  and H --> gamma gamma using 140 fb**-1 of p p collisions at Ecm = 13 TeV. See  their Fig. 4 for limits on production cross section times branching ratios in the ranges  mass(H_{{3}}()0) = 0.17 -- 1.0 TeV and mass(H_{{{1,2}}}()0) = 0.015 -- 0.5 TeV.


pdgid: S055H2O
text:
AAD 2024CD search for production of H_{{2}}()0 decaying to Z A, A --> invisible, using  140 fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 8 -- 12 for  excluded parameter regions in two-Higgs-doublet plus singlet pseudoscalar model.


pdgid: S055H2O
text:
AAD 2024CF search for gluon-fusion production of A0 decaying to tau+ tau- in 140  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 7 for limits on cross  section times branching ratio in the range mass(A0) = 20 -- 90 GeV, and Fig. 8 for A0  coupling with the top quark.


pdgid: S055H2O
text:
AAD 2024CI search for production of H_{{2}}()0, A0 decaying to invisible final states, in  various channels including t tbar + missing E(T) and t tbar t tbar, using up to 140  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 3 for cross section limits  in a simplified model with fixed Dark Matter mass and couplings to quarks and Dark Matter.


pdgid: S055H2O
text:
AAD 2024CK combines published ATLAS data up to 139 fb**-1 to constrain two-Higgs-doublet  plus singlet pseudoscalar model with A_{{1}}()0 decaying to invisibly into Dirac Dark Matter final  states. See their Figs. 4 -- 9 for excluded parameter regions.


pdgid: S055H2O
text:
AAD 2024H combine searches for a scalar resonance decaying to H H using up to 139  fb**-1 of p p collisions at Ecm = 13 TeV from AAD 2022F, AAD 2023Z, and  AAD 2022Y. See their Fig. 1 for limits on cross section times branching ratio for  mass(H_{{2}}()0) = 0.251 -- 5.0 TeV.


pdgid: S055H2O
text:
AAD 2024K search for the decay H --> Z A0 with A0 --> gamma gamma and Z --> lepton+ lepton-  in 139 fb**-1 of p p collisions at Ecm = 13 TeV. Merged gamma gamma events as  well as resolved ones are looked for. See their Fig. 3 for limits on the product of the branching  ratios for mass(A0) = 0.1 -- 33 GeV.


pdgid: S055H2O
text:
ADACHI 2024F search for H_{{1}}()0, which couples preferentially to muon pairs, in the  process e+ e- --> mu+ mu- H_1()0 --> mu+ mu- mu+ mu- using 178 fb**-1 of e+ e-  collisions at Ecm = 10.58 GeV. See their Fig. 13 (lower) for limits on cross section times  branching ratio for mass(H_{{1}}()0) = 0.212 -- 9.0 GeV. Limits on the model parameter are  given in Fig. 14 (lower).


pdgid: S055H2O
text:
HAYRAPETYAN 2024AA search for the decay chain H --> A0 A0 --> b bbar b bbar, produced in  association with W+- or Z, in 138 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 3 for limits on the product of branching ratios in the range mass(A0) = 15 -- 60 GeV.


pdgid: S055H2O
text:
HAYRAPETYAN 2024AE search for H_2()0 --> H H in the final state b bbar W+ W- using  138 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 19 (upper) for limit on  the product of production cross section times branching ratios for mass(H_{{2}}()0) = 0.25 -- 0.9 TeV.


pdgid: S055H2O
text:
HAYRAPETYAN 2024AF search for H --> A0 A0 in the final state b bbar mu+ mu- and b bbar tau+ tau- in  138 fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 10, 11, and 12 for  limits on the product of branching ratios in the range mass(A0) = 12 -- 60 GeV.  Interpretation of the limits in terms of two Higgs doublet plus singlet models is given in their  Figs. 13 and 14.


pdgid: S055H2O
text:
HAYRAPETYAN 2024AI search for H --> H_1()0 H_1()0, with long-lived H_{{1}}()0 decaying in  the muon detectors to gamma gamma, e+ e-, pi0 pi0, pi+ pi-, K+ K-, K0 K0,  d dbar, tau+ tau-, or b bbar, using 138 fb**-1 of p p collisions at Ecm =  13 TeV. See their Figs. 13 -- 17 for limits on B(H --> H_1()0 H_1()0) in the mass  range between 0.4 and 55 GeV for each of the decay modes.


pdgid: S055H2O
text:
HAYRAPETYAN 2024AJ search for production of a scalar resonance decaying to gamma gamma in  138 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 3 (right) for limits on  production cross section times branching ratio for mass(H_{{2}}()0) = 0.6 -- 5.0 TeV, and Fig.  4 (lower) for their dependence on the  width.


pdgid: S055H2O
text:
HAYRAPETYAN 2024AZ search for pair production of A0 decaying to mu+ mu- using  101 -- 137 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 5 for  limits on cross section times branching ratio for mass(A0) = 0.21 -- 60 GeV.


pdgid: S055H2O
text:
HAYRAPETYAN 2024AZ search for H or H_{{{1,2}}}()0 decaying to A0 A0 --> mu+ mu- mu+ mu- using  101 -- 137 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 8 for  limits on cross section times branching ratio for mass(A0) = 0.5 -- 2.7 GeV and several  choices of mass(H_{{{1,2}}}()0) in a NMSSM scenario.


pdgid: S055H2O
text:
HAYRAPETYAN 2024I search for the decay H --> Z A0 with A0 --> gamma gamma and Z --> lepton+ lepton-  in 138 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 7 for limits on the  product of cross section times the branching ratios for mass(A0) = 1 -- 30 GeV.


pdgid: S055H2O
text:
TUMASYAN 2024A search for production of H_{{{1,2}}}()0 in association with W, Z, or  t tbar, decaying to e+ e-, mu+ mu-, or tau+ tau-, using 138 fb**-1 of p p  collisions at Ecm = 13 TeV. See their Fig. 13 for limits on cross section times branching  ratio for mass(H_{{{1,2}}}()0) = 15 -- 350 GeV.  See also Figs. 16 and 17 for limits on the  mixing with the Standard Model Higgs boson.


pdgid: S055H2O
text:
TUMASYAN 2024B search for H_2()0 --> H H in the final state gamma gamma b bbar using  138 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 6 (upper) for limit on  the product of production cross section times branching ratios for mass(H_{{2}}()0) = 0.26 -- 1.0 TeV.


pdgid: S055H2O
text:
TUMASYAN 2024B search for production of H_{{3}}()0 decaying to H_1,2()0 H --> b bbar gamma gamma  using 138 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 7 for limits on  production cross section times branching ratios for mass(H_{{3}}()0) = 0.3 -- 1.0 TeV and  mass(H_{{{1,2}}}()0) = 0.09 -- 0.8 TeV.


pdgid: S055H2O
text:
AAD 2023AD search for associated production of W/Z H_2()0 with the decay chain  H_2()0 --> H H --> b bbar b bbar using 139 fb**-1 of p p collisions at Ecm = 13  TeV. See their Fig. 9 for limits on cross section times branching ratios for mass(H_{{2}}()0) =  260 -- 1000 GeV.


pdgid: S055H2O
text:
AAD 2023AD search for gluon fusion production of A0 with the decay chain A0 --> Z H_2()0,  H_2()0 --> H H --> b bbar b bbar using 139 fb**-1 of p p collisions at Ecm = 13  TeV. See their Fig. 10 for limits on cross section times branching ratios for mass(A0) =  350 -- 800 GeV and mass(H_{{2}}()0) = 260 -- 400 GeV.


pdgid: S055H2O
text:
AAD 2023AJ search for production of H+- in association with a top quark, followed by  H+- --> W+- A0, A0 --> invisible, using 139 fb**-1 of p p collisions at  Ecm = 13 TeV. See their Fig. 10 for excluded parameter regions of 2HDM + CP-odd singlet  model.


pdgid: S055H2O
text:
AAD 2023BD search for a top quark decaying to q H_1,2()0 (q = u, c),   H_1,2()0 --> b bbar, using 139 fb**-1 of p p collisions at Ecm = 13 TeV.  See   their Fig. 9 for limits on production cross section times branching ratios for  mass(H_{{{1,2}}}()0) =  20 -- 160 GeV.


pdgid: S055H2O
text:
AAD 2023BE search for associated production of H_2()0 W and decay H_2()0 --> W+ W-  assuming the presence of higher dimensional H_2()0 W+ W- interactions, using 139 fb**-1 of  p p collisions at Ecm = 13 TeV.  See their Fig. 6 for excluded parameter region of higher  dimensional operators, and Fig. 7 for limits on cross section times branching ratio for  mass(H_{{2}}()0) = 0.3 -- 1.5 TeV.


pdgid: S055H2O
text:
AAD 2023BG search for production of H_{{2}}()0/A0 in association with a t tbar pair,  decaying to t tbar, using 139 fb**-1 of p p collisions at Ecm = 13 TeV.  See  their Fig. 7 for limits on cross section times branching ratios for mass(H_{{2}}()0) = mass(A0) =  0.4 -- 1.0 TeV.


pdgid: S055H2O
text:
AAD 2023BW search for A0 production in association with a t tbar pair, decaying to  mu+ mu-, using 139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 5(a)  for limits on production cross section times branching ratio for mass(A0) = 15 -- 72 GeV.


pdgid: S055H2O
text:
AAD 2023BX search for production of H --> tau+ tau- with missing transverse momentum  using 139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for  interpretation of the data in terms of 2HDM + a model.


pdgid: S055H2O
text:
AAD 2023CA search for production of H_{{3}}()0 decaying to H_2()0 H, H_2()0 --> W+ W-  or Z Z, and H --> tau+ tau- using 140 fb**-1 of p p collisions at Ecm = 13  TeV. See their Figs. 4, 5 for limits on production cross section times branching ratios in the  ranges mass(H_{{3}}()0) = 0.5 -- 1.5 TeV and mass(H_{{2}}()0) = 0.2 -- 0.5 TeV.


pdgid: S055H2O
text:
AAD 2023CR search for H_{{2}}()0 having flavor-violating couplings to t c or t u,  produced in association with top quark(s), using 139 fb**-1 of p p collisions at Ecm  = 13 TeV. See their Fig. 14 for limits on production cross section times branching ratios for  mass(H_{{2}}()0) = 0.2 -- 1.5 TeV with various assumptions on the flavor-changing couplings.


pdgid: S055H2O
text:
AAD 2023O search for production of an A0 in gluon-gluon fusion and in association with a    b bbar, decaying to Z H in the final states nu nubar b bbar and lepton+ lepton- b bbar  using   139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 9 for limits on  cross   section times branching ratio for mass(A0) = 0.22 -- 2.0 TeV, and Fig. 11 for  limits with both production components.


pdgid: S055H2O
text:
AAD 2023R search for the decay A0 --> gamma gamma in 138 fb**-1 of p p collisions  at Ecm = 13 TeV.  See their Fig. 7 for limits on cross section times branching ratio for  mass(A0) = 10 -- 70 GeV.


pdgid: S055H2O
text:
AAD 2023U search for the decay H_2()0 --> Z gamma with Z decaying hadronically in 139   fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8(a) for limits on   production cross section times branching ratios for mass(H_{{2}}()0) = 1.0 -- 6.8 TeV.


pdgid: S055H2O
text:
AAD 2023Z search for the decay chain H_2()0 --> H H --> b bbar tau+ tau- using 139  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 10 for limits on the  product of production cross section times branching ratios for mass(H_{{2}}()0) = 0.251 -- 1.6  TeV.


pdgid: S055H2O
text:
HAYRAPETYAN 2023C search for H_1,2()0 --> e mu using 138 fb**-1 of p p  collisions at Ecm = 13 TeV. See their Fig. 7 for limits on production cross section times  branching ratio for mass(H_{{{1,2}}}()0) = 110 -- 160 GeV.


pdgid: S055H2O
text:
HAYRAPETYAN 2023G search for dimuon resonance in the mass range 1.1 -- 2.6 or  4.2 -- 7.9 GeV in 96.6 fb**-1 of p p collisions at Ecm = 13 TeV, in inclusive  and high p_{{T}} selections. See their Fig. 5 for cross section times branching ratio limits and  Fig. 7 for mixing angle limits in two Higgs doublet plus singlet model (at 90% CL).


pdgid: S055H2O
text:
TUMASYAN 2023 search for production of H_{{3}}()0 decaying to H_1,2()0 H --> b bbar b bbar using    138 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 4 for limits on    production cross section times branching ratios for mass(H_{{3}}()0) = 0.9 -- 4.0 TeV and    mass(H_{{{1,2}}}()0) = 60 -- 600 GeV, and their interpretation in the NMSSM and the Two Real  Singlet Model (TRSM).


pdgid: S055H2O
text:
TUMASYAN 2023M search for the decay chain H --> A0 A0 --> gamma gamma gamma gamma in 132  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 6 for limits on cross  section times branching ratio in the range mass(A0) = 15 -- 62 GeV.


pdgid: S055H2O
text:
TUMASYAN 2023O search for H_2()0 --> H H, each H decaying to either W W^* or  tau+ tau- using 138 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 14  (upper) for limit on the product of production cross section times branching ratios for  mass(H_{{2}}()0) = 0.25 -- 1.0 TeV.


pdgid: S055H2O
text:
TUMASYAN 2023S search for gluon fusion and b-associated production of H_{{{1,2}}}()0   decaying  to tau+ tau- using 138 fb**-1 of p p collisions at Ecm = 13 TeV.  See   their Fig.  10 for limits on production cross section times branching ratios for mass(H_{{{1,2}}}()0)   =  0.06 -- 3.5 TeV.


pdgid: S055H2O
text:
AAD 2022A search for the decay chain H --> A0 A0 --> mu+ mu- b bbar in 139 fb**-1 of  p p collisions at Ecm = 13 TeV. See their Fig. 9 for limits on the overall branching  fraction in the range mass(A0) = 16 -- 62 GeV. See also Fig. 11 for limits without assuming  A0 is pseudoscalar.


pdgid: S055H2O
text:
AAD 2022D search for Z A0 associate production with Z --> lepton+ lepton-,  A0   decaying invisibly, in 139 fb**-1 of p p collisions at Ecm = 13 TeV. See  their Fig.  5  for excluded regions in the mass parameter space of two Higgs doublet plus singlet (2HDM+A0)  model with a  certain choice of the model parameters.


pdgid: S055H2O
text:
AAD 2022F search for gluon fusion production of H_{{2}}()0 decaying to H H --> b bbar b bbar  using 126 -- 139 fb**-1 of p p collisions at Ecm = 13 TeV. B(H --> b bbar) =  0.582 is assumed. See their Fig. 14 for limit on the product of production cross section times  branching ratios for mass(H_{{2}}()0) = 0.251 -- 5.0 TeV.


pdgid: S055H2O
text:
AAD 2022I search for Z H associate production with the decay chain H --> chitilde_2()0 chitilde_1()0,  chitilde_2()0 --> A0 chitilde_1()0, A0 --> b bbar, and Z --> lepton+ lepton-, in 139  fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 3 and 4 for limits on the  product of cross section times the branching ratios for mass(A0) = 20 -- 65 GeV with  various choices of NMSSM model parameters.


pdgid: S055H2O
text:
AAD 2022J search for the decay H --> Z A0 with A0 --> mu+ mu- and Z --> e+ e-,  mu+ mu- in 139 fb**-1 of  p p collisions at Ecm = 13 TeV assuming SM gluon-gluon  fusion production of the H. See their Fig. 17(b) for limits on the   product of cross  section  times the branching ratios for mass(A0) = 15 -- 30 GeV.


pdgid: S055H2O
text:
AAD 2022J search for the decay H --> A0 A0 with A0 --> mu+ mu- in 139 fb**-1 of    p p collisions at Ecm = 13 TeV assuming SM gluon-gluon fusion production of the H  in the range of mass(A0) = 1 -- 60 GeV .  See their Fig. 14(b) for limits on the product of  cross  section times the branching ratios for  mass(A0) = 1.5 -- 60 GeV (excluding psi  and  Upsilon regions). The limit also  applies to the decay H --> H_1()0 H_1()0.


pdgid: S055H2O
text:
AAD 2022P search for invisibly decaying H_{{1}}()0, H_{{2}}()0 produced by vector boson  fusion in 139 fb**-1 of p p collisions at Ecm = 13 TeV. Limit on the product of cross  section times branching ratio in the range 0.1 -- 1 pb (95% CL) is given for the mass  range 0.05 -- 2 TeV. See their Fig. 14.


pdgid: S055H2O
text:
AAD 2022Y search for gluon fusion production of H_{{2}}()0 decaying to H H --> b bbar gamma gamma  in 139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 15 for limit on the  product of production cross section times branching ratios to H H for mass(H_{{2}}()0) =  0.251 -- 1.0 TeV.


pdgid: S055H2O
text:
ABRATENKO 2022A search for a singlet scalar boson H_{{1}}()0 having a small mixing with the   SM Higgs boson in the decay chain K+ --> H_1()0 pi+, H_1()0 --> mu+ mu- from data   corresponding to 7.01E20 protons on NuMI target. See their Fig. 13 (right) and Table V for  limits on  the SM Higgs component of H_{{1}}()0 for mass(H_{{1}}()0) = 212 -- 279 MeV.


pdgid: S055H2O
text:
TUMASYAN 2022AK search for gluon-fusion production of H_{{3}}()0 decaying to H_1()0 H_1()0 --> b bbar b bbar  in 138 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 5 for limits on  cross section times branching ratio for mass(H_{{3}}()0) = 1 -- 3 TeV, mass(H_{{1}}()0) =  25 -- 100 GeV.


pdgid: S055H2O
text:
TUMASYAN 2022D search for production of an H_{{2}}()0 (denoted radion in the paper) in gluon  fusion and vector boson fusion, decaying to W+ W- in the final states lepton nu + hadrons,  using 137 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 7 for limits on  cross section times branching ratio for mass(H_{{2}}()0) = 1.0 -- 4.5 TeV.


pdgid: S055H2O
text:
AAD 2021AF search for production of a heavy H_{{2}}()0 state decaying to Z Z in the final     states lepton+ lepton- lepton^'()+ lepton^'()- and lepton+ lepton- nu nubar in 139    fb**-1 of  p p collisions at Ecm = 13 TeV. See their Fig. 4 for upper limits on cross    section times  branching ratio for mass(H_{{2}}()0) = 0.2 -- 2.0 TeV assuming ggF or VBF with  narrow width approximation, and  Fig. 5 for upper limits on cross section times branching ratio for  mass(H_{{2}}()0) =   0.4 -- 2.0 TeV  assuming ggF, and with several assumptions on its width.


pdgid: S055H2O
text:
AAD 2021AI search for production of an A0 in gluon-gluon fusion and in association with a  b bbar, decaying to Z H_2()0 --> lepton+ lepton- b bbar or lepton+ lepton- W+ W- in 139  fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 9 and 13 for cross section  limits for mass(A0) = 230 -- 800 GeV and mass(H_{{2}}()0) = 130 -- 700 GeV.


pdgid: S055H2O
text:
AAD 2021AY search for production of a scalar resonance decaying to gamma gamma in 139  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 5(a) for limits on fiducial  cross section times branching ratio for mass(H_{{2}}()0) = 0.16 -- 3 TeV with narrow width  approximation, and Table 2 with several assumptions on the width.


pdgid: S055H2O
text:
AAD 2021AZ search for production of A_{{2}}()0 decaying to H A_1()0 followed by H --> gamma gamma,  A_1()0 --> invisible in 139 fb**-1 of p p collisions at Ecm = 13 TeV. See their  Figs. 10 -- 12 for limits in terms of two-Higgs-doublet model plus singlet pseudoscalar and  a fermionic Dark Matter particle.


pdgid: S055H2O
text:
AAD 2021BB search for production of A_{{2}}()0 by gluon fusion or associated A_2()0 b bbar  production, decaying to H A_1()0 followed by H --> b bbar, A_1()0 --> invisible in  139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for limits in terms of  two-Higgs-doublet plus singlet pseudoscalar model.


pdgid: S055H2O
text:
AAD 2021BE search for production of A_{{1}}()0 associated with a single top quark and either  a light quark or a W boson, decaying  to invisible final states, in 139 fb**-1 of p p  collisions at Ecm = 13 TeV. See their  Figs. 13 -- 15 for limits in terms of  two-Higgs-doublet model plus singlet pseudoscalar,  which is assumed to decay to a pair of Dark  Matter particles.


pdgid: S055H2O
text:
ABRATENKO 2021 search for a singlet scalar boson H_{{1}}()0 having a small mixing with the  SM Higgs boson in the decay chain K+ --> H_1()0 pi+, H_1()0 --> e+ e- from data  corresponding to 1.93E20 protons on NuMI target. See their Fig. 2 for limits on the SM Higgs  component of H_{{1}}()0 for mass(H_{{1}}()0) = 3 -- 210 MeV.


pdgid: S055H2O
text:
SIRUNYAN 2021A search for H_2()0 --> Z A0 with Z --> lepton+ lepton-, A0 decaying  invisibly, in 137 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 8 for  excluded regions in the mass parameter space of two Higgs doublet plus singlet model with a certain  choice of the model parameters.


pdgid: S055H2O
text:
TUMASYAN 2021F search for gluon fusion production of H_{{3}}()0 decaying to H H_1,2()0 --> tau+ tau- b bbar   in 137  fb**-1 of p p collisions at Ecm = 13 TeV. See their Figs. 5 and 6 for limits   on cross  section times branching ratios for mass(H_{{1,2}}()0) = 0.06 -- 2.8 TeV and   mass(H_{{3}}()0) =  0.24 -- 3.0 TeV.


pdgid: S055H2O
text:
AAD 2020AA search for H_{{2}}()0/A0 --> tau+ tau- produced by gluon fusion or  b-associated production using 139 fb**-1 of p p collisions at Ecm = 13 TeV.  See  their Fig. 2(a), 2(b) for limits on the product of cross section and branching ratio for  mass(H_{{2}}()0), mass(A0) = 0.2 -- 2.5 TeV.


pdgid: S055H2O
text:
AAD 2020AI search for Z H production followed by the decay H --> A0 A0 --> b bbar b bbar in  36 fb**-1 of p p collisions at Ecm = 13 TeV. The search looks for collimated A0 --> b bbar  decays and is complementary to AABOUD 2018BX.   See their Fig. 10 for limits on the product  of production cross section and branching ratios in the range mass(A0) = 15 -- 30 GeV.


pdgid: S055H2O
text:
AAD 2020AO search for gluon fusion production of H_{{2}}()0 decaying to H H --> tau+ tau- b bbar  (with hadronically decaying tau+ tau-) using 139 fb**-1 of p p collisions at Ecm  = 13 TeV.  Limit on the product of production cross section times branching ratios in the range  28 -- 817 fb (95% CL) is given for mass(A0) = 1.0 -- 3.0 TeV, see their Fig.  13.


pdgid: S055H2O
text:
AAD 2020C combine searches for a scalar resonance decaying to H H in 36.1 fb**-1 of  p p collisions at Ecm = 13 TeV from AABOUD 2019A, AABOUD 2019O, AABOUD 2018CQ,  AABOUD 2019T, AABOUD 2018CW, and AABOUD 2018BU. See their Fig. 5(a) for limits on  cross section times branching ratio for mass(H_{{2}}()0) = 0.26 -- 3 TeV.


pdgid: S055H2O
text:
AAD 2020L search for b-associated production of H_{{2}}()0 decaying to b bbar in 27.8  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 8 for limits on the product  of cross section and branching ratio for mass(H_{{2}}()0) = 0.45 -- 1.4 TeV.


pdgid: S055H2O
text:
AAD 2020X search for vector-boson-fusion production of H_{{2}}()0 decaying to H H using  126 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 5 for limits on the  product of cross section and branching ratio for the assumptions of a narrow- and broad-width  resonance.


pdgid: S055H2O
text:
AAIJ 2020AL search for dimuon resonance in the mass range 0.2 -- 60 GeV in 5.1  fb**-1 of p p collisions at Ecm = 13 TeV, in inclusive and b quark associated  production.  Displaced decays are searched for for masses below 3 GeV.  See their Figs. 7 -- 9 for  cross section limits and Fig. 10 for limits for mixing angle in two Higgs doublet plus singlet  model (at 90% CL).


pdgid: S055H2O
text:
SIRUNYAN 2020 search for the decay H --> A0 A0 --> tau+ tau- tau+ tau- or tau+ tau- mu+ mu- in  35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 10 for limits on the  product of production cross section (normalized to the SM) and branching ratios in the range  mass(A0) = 4 -- 15 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2020AA search for H_2()0 --> Z A0, A0 --> b bbar or  A0 --> Z H_2()0,  H_2()0 --> b bbar in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.  See their  Fig. 7 for limits on the product of cross section and branching ratio for mass(H_{{2}}()0) =  0.12 -- 1 TeV and mass(A0) = 0.03 -- 1 TeV.


pdgid: S055H2O
text:
SIRUNYAN 2020AC search for gluon-fusion production of A0 decaying to Z H in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 5 for limits on the product  of cross section and branching ratios for mass(A0) = 220 -- 400 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2020AD search for lepton-flavor violating decays H_2()0 --> mu tau , e tau of  gluon-fusion-produced H_{{2}}()0 in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.   See their Fig. 5 (9) and Table 5 (6) for limits on production cross section times branching ratio  for mass(H_{{2}}()0) = 0.2 -- 0.9 TeV for the mu tau (e tau) final state.


pdgid: S055H2O
text:
SIRUNYAN 2020AF search for H_{{2}}()0/A0 --> t tbar with one or two charged leptons in  the final state using kinematic variables in 35.9 fb**-1 of p p collisions at Ecm =  13 TeV. See their Figs. 5 and 6 for limits on top Yukawa coupling of H_{{2}}()0 and A0 for  mass(H_{{2}}()0), mass(A0) = 0.4 -- 0.75 TeV for various width assumptions.


pdgid: S055H2O
text:
SIRUNYAN 2020AP search for the decay H or H_2()0 --> A0 A0 --> mu+ mu- tau+ tau-  (for mass(H_{{2}}()0) = 300 GeV) with boosted final-state topology in 35.9 fb**-1 of p p  collisions at Ecm = 13 TeV. See their Fig. 7 for limits on the product of production cross  section (normalized to the SM) and branching ratios in the range mass(A0) = 3.6 -- 21 GeV,  and Figs. 8 and 9 for its interpretation in terms of models with two Higgs doublets plus a singlet.


pdgid: S055H2O
text:
SIRUNYAN 2020Y search for gluon-fusion and vector-boson-fusion production of H_{{2}}()0  decaying to W+ W- in the final states lepton nu lepton nu and lepton nu q q in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 6 for limits on the product  of cross section and branching ratio for mass(H_{{2}}()0) = 0.2 -- 3 TeV.


pdgid: S055H2O
text:
SIRUNYAN 2020Z search for H_{{{1,2}}}()0 or A0 production in association with a t tbar pair,  decaying to e+ e- or mu+ mu-,  in 137 fb**-1 of p p collisions at Ecm = 13  TeV.  See their Fig. 12 for limits on production cross section times branching ratio for  mass(H_{{{1,2}}}()0), mass(A0) = 15 -- 75 GeV and 108 -- 340 GeV.


pdgid: S055H2O
text:
AABOUD 2019A search for a narrow scalar resonance decaying to H H --> b bbar b bbar in  27.5 -- 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 9(a) for  limits on cross section times branching ratios for mass(H_{{2}}()0) = 0.26 -- 3 TeV.


pdgid: S055H2O
text:
AABOUD 2019AG search for the decay H --> A0 A0 --> mu+ mu- b bbar in 36.7 fb**-1 of  p p collisions at Ecm = 13 TeV. See their Fig. 6 (a) for limits on the product of  production cross section (normalized to the SM) and branching ratios in the range mass(A0) =  20 -- 60 GeV.


pdgid: S055H2O
text:
AABOUD 2019O search for a scalar resonance decaying to H H --> b bbar W W^* in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 12 (left) for limits on  cross section times branching ratio for mass(H_{{2}}()0) = 0.5 -- 3 TeV.


pdgid: S055H2O
text:
AABOUD 2019T search for a scalar resonance decaying to H H --> W W^* W W^* in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 3 for limits on cross  section times branching ratio for mass(H_{{2}}()0) = 260 -- 500 GeV, assuming SM decay rates  for the H.


pdgid: S055H2O
text:
AABOUD 2019V combine published ATLAS data to constrain two-Higgs-doublet plus singlet  pseudoscalar model with A_{{1}}()0 decaying to invisible final states. See their Fig. 19 for  excluded parameter regions.


pdgid: S055H2O
text:
AABOUD 2019Y search for a narrow scalar resonance produced by gluon fusion or b  associated production, decaying to mu+ mu- in 36.1 fb**-1 of p p collisions at  Ecm = 13 TeV.  See their Figs. 4 and 5(a) for cross section limits for mass(H_{{2}}()0) =  0.2 -- 1.0 TeV.


pdgid: S055H2O
text:
AALTONEN 2019 search for b associated production of a scalar particle decaying to b bbar in 5.4  fb**-1 of p pbar collisions at Ecm = 1.96 TeV.  See their Fig. 3 for limits on cross  section times branching ratio for mass(H_{{{1,2}}}()0) = 100 -- 300 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2019 search for a narrow scalar resonance decaying to H H --> gamma gamma b bbar in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 9 (left) for limits on cross  section times branching ratios for mass(H_{{2}}()0) = 260 -- 900 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2019AE search for a scalar resonance produced in association with a b bbar pair,  decaying to tau+ tau- in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.  See  their Fig. 4 for cross section limits for mass(A0) = 25 -- 70 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2019AN search for production of A_{{2}}()0 decaying to H A_1()0 followed by  H --> b bbar, A_1()0 --> invisible in 35.9 fb**-1 of p p collisions at Ecm =  13 TeV, in the mass range mass(A_{{2}}()0) = 0.2 -- 1.6 TeV, mass(A_{{1}}()0) = 0.15 -- 0.5  TeV.  See their Fig. 6 for limits in terms of two-Higgs-doublet plus singlet pseudoscalar model.


pdgid: S055H2O
text:
SIRUNYAN 2019AV search for a scalar resonance produced by gluon fusion or b-associated  production, decaying to Z H --> lepton+ lepton- b bbar (lepton = e, mu) or nu nubar b bbar in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 5 for cross section limits  for mass(A0) = 0.22 -- 1.0 TeV.


pdgid: S055H2O
text:
SIRUNYAN 2019B search for gluon fusion production of narrow scalar resonance with large  transverse momentum, decaying to b bbar, in 35.9 fb**-1 of p p collisions at Ecm  = 13 TeV.  See their Figs. 7 and 8 for limits on cross section times branching ratio for the  resonance mass of 50 -- 350 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2019BB search for the decay H_1()0 --> gamma gamma in 19.7 fb**-1 of p p  collisions at Ecm = 8 TeV and 35.9 fb**-1 at Ecm = 13 TeV.  See their Figs.  4 -- 6 for limits on cross section times branching ratio for mass(H_{{1}}()0) = 80 -- 110 GeV  (some results in Fig. 5 for mass(H_{{1}}()0) = 70 -- 110 GeV).


pdgid: S055H2O
text:
SIRUNYAN 2019BD search for the decay H --> A0 A0 --> mu+ mu- b bbar in 35.9 fb**-1  of p p collisions at Ecm = 13 TeV. See their Fig. 5 for limits on the product of  cross section times branching ratios in the range mass(A0) = 20 -- 62.5 GeV. See also their  Figs. 6 and 7 for interpretation of the data in terms of models with two Higgs doublets and a  singlet.


pdgid: S055H2O
text:
SIRUNYAN 2019BE combine searches for H_2()0 --> H H in 35.9 fb**-1 of p p  collisions at Ecm = 13 TeV in various H decay modes, from SIRUNYAN 2018A,  SIRUNYAN 2018AF, SIRUNYAN 2018CW, SIRUNYAN 2019, and SIRUNYAN 2019H.  See  their Fig. 3 for limits on cross section times branching ratios for mass(H_{{2}}()0) = 0.25 -- 3 TeV.


pdgid: S055H2O
text:
SIRUNYAN 2019BQ search for production of H_{{{1,2}}}()0 decaying to A0 A0 --> mu+ mu- mu+ mu- in  35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 2 for limits on cross  section times branching ratio for mass(H_{{{1,2}}}()0) = 90 -- 150 GeV, mass(A0) = 0.25 -- 3.55  GeV.


pdgid: S055H2O
text:
SIRUNYAN 2019CR search for production of H_2()0 / A0 in gluon fusion and in association  with a b bbar pair, decaying to mu+ mu- in 35.9 fb**-1 of p p collisions at  Ecm = 13 TeV.  See their Fig. 6 for limits on cross section times branching ratio.


pdgid: S055H2O
text:
SIRUNYAN 2019H search for a narrow scalar resonance decaying to H H --> b bbar b bbar  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV, where one b bbar pair is  resolved and the other not. Limits on cross section times branching ratios for mass(H_{{2}}()0) =  0.75 -- 1.6 TeV are obtained and combined with data from SIRUNYAN 2018AF.  See their  Fig. 5 (right).


pdgid: S055H2O
text:
AABOUD 2018AA search for production of a scalar resonance decaying to Z gamma, with Z  decaying hadronically, in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See their  Fig. 8(a) for limits on cross section times branching ratio for mass(H_{{2}}()0) = 1.0 -- 6.8  TeV.


pdgid: S055H2O
text:
AABOUD 2018AG search for the decay H --> A0 A0 --> gamma gamma g g in 36.7 fb**-1 of  p p collisions at Ecm = 13 TeV. See their Fig. 2 and Table 6 for cross section limits in  the range mass(A0) = 20 -- 60 GeV.


pdgid: S055H2O
text:
AABOUD 2018AH search for production of an A0 in gluon-gluon fusion and in association  with a b bbar, decaying to Z H_2()0 --> lepton+ lepton- b bbar in 36.1 fb**-1 of p p  collisions at Ecm = 13 TeV.  See their Fig. 5 for cross section limits for mass(A0) =  230 -- 800 GeV and mass(H_{{2}}()0) = 130 -- 700 GeV.


pdgid: S055H2O
text:
AABOUD 2018AI search for production of an A0 in gluon-gluon fusion and in association  with a b bbar, decaying to Z H in the final states nu nubar b bbar and lepton+ lepton- b bbar in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 6 for cross section limits  for mass(A0) = 0.2 -- 2 TeV. See also AABOUD 2018CC.


pdgid: S055H2O
text:
AABOUD 2018BF search for production of a heavy H_{{2}}()0 state decaying to Z Z in the  final states lepton+ lepton- lepton+ lepton- and lepton+ lepton- nu nubar in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 6 for upper limits on cross  section times branching ratio for mass(H_{{2}}()0) = 0.2 -- 1.2 TeV assuming ggF or VBF with  the NWA. See their Fig. 7 for upper limits  on cross section times branching ratio for  mass(H_{{2}}()0) = 0.4 -- 1.0 TeV assuming ggF, and with several assumptions on its width.


pdgid: S055H2O
text:
AABOUD 2018BU search for a narrow scalar resonance decaying to H H --> gamma gamma W W^* in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 4 for limits on cross  section times branching ratios for mass(H_{{2}}()0) = 260 -- 500 GeV.


pdgid: S055H2O
text:
AABOUD 2018BX search for associated production of W H or Z H followed by the decay  H --> A0 A0 --> b bbar b bbar in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 9 for limits on cross section times branching ratios for mass(A0) = 20 -- 60  GeV.  See also their Fig. 10 for the dependence of the limit on A0 lifetime.


pdgid: S055H2O
text:
AABOUD 2018CQ search for a narrow scalar resonance decaying to H H --> b bbar tau+ tau-  in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 2 (above) for limits  on cross section times branching ratios for mass(H_{{2}}()0) = 260 -- 1000 GeV.


pdgid: S055H2O
text:
AABOUD 2018F search for production of a narrow scalar resonance decaying to W+ W- and  Z Z, followed by hadronic decays of W and Z, in 36.7 fb**-1 of p p collisions  at Ecm = 13 TeV. See their Fig. 5(c) for limits on cross section times branching ratio for  mass(H_{{2}}()0) = 1.2 -- 3.0 TeV.


pdgid: S055H2O
text:
AAIJ 2018AM search for gluon-fusion production of H_{{{1,2}}}()0 decaying to mu tau in 2  fb**-1 of p p collisions at Ecm = 8 TeV.  See their Fig. 2 for limits on cross  section times branching ratio for mass(H_{{{1,2}}}()0) = 45 -- 195 GeV.


pdgid: S055H2O
text:
AAIJ 2018AQ search for gluon-fusion production of a scalar particle A0 decaying to mu+ mu- in 1.99 fb**-1 of p p collisions at Ecm = 8 TeV and 0.98 fb**-1 at Ecm = 7  TeV.  See their Fig. 4 for limits on cross section times branching ratio for  mass(A0) =  5.5 -- 15 GeV (using the Ecm = 8 TeV data set).


pdgid: S055H2O
text:
AAIJ 2018AQ search for the decay H --> A0 A0, with one of the A0  decaying to mu+ mu-, in 1.99 fb**-1 of p p collisions at Ecm = 8 TeV and 0.98 fb**-1 at Ecm = 7  TeV.  See their Fig. 5 (right) for limits on the product of branching ratios for  mass(A0) =  5.5 -- 15 GeV (using the Ecm = 8 TeV data set).


pdgid: S055H2O
text:
SIRUNYAN 2018AF search for a narrow scalar resonance decaying to H H --> b bbar b bbar  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV, where both b bbar pairs are not  resolved. See their Fig. 9 for limits on cross section times branching ratios for mass(H_{{2}}()0) =  0.75 -- 3 TeV.


pdgid: S055H2O
text:
SIRUNYAN 2018BA search for production of a heavy H_{{2}}()0 state decaying to Z Z in the  final states lepton+ lepton- lepton+ lepton-, lepton+ lepton- q qbar, and lepton+ lepton- nu nubar in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Figs. 10 and 11 for upper limits  on cross section times branching ratio for mass(H_{{2}}()0) = 0.13 -- 3 TeV with several  assumptions on its width and on the fraction of Vector-Boson-Fusion of the total production cross  section.


pdgid: S055H2O
text:
SIRUNYAN 2018CW search for a narrow scalar resonance decaying to H H --> b bbar b bbar  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV, where both b bbar pairs are  resolved. See their Fig. 9 for limits on cross section times branching ratios for mass(H_{{2}}()0) =  260 -- 1200 GeV.


pdgid: S055H2O
text:
SIRUNYAN 2018DK search for production of a scalar resonance decaying to Z gamma, with  Z decaying to lepton+ lepton- or hadronically, in 35.9 fb**-1 of p p collisions at  Ecm = 13 TeV. See their Fig. 7 for limits on cross section times branching ratio for  mass(H_{{2}}()0) = 0.35 -- 4 TeV for different assumptions on the width of the resonance.


pdgid: S055H2O
text:
SIRUNYAN 2018DT search for the decay H --> A0 A0 --> tau+ tau- b bbar in 35.9 fb**-1  of p p collisions at Ecm = 13 TeV. See their Fig. 7 for limits on the product of  branching ratios in the range mass(A0) = 15 -- 60 GeV. See also their Fig. 8 for  interpretation of the data in terms of models with two Higgs doublets and a singlet.


pdgid: S055H2O
text:
SIRUNYAN 2018DU search for production of a narrow scalar resonance decaying to gamma gamma in 35.9  fb**-1 (taken in 2016) of p p collisions at Ecm = 13 TeV. See their Fig. 3 (right)  for limits on cross section times branching ratio for mass(H_{{2}}()0) = 0.5 -- 5 TeV for  several values of its width-to-mass ratio.


pdgid: S055H2O
text:
SIRUNYAN 2018ED search for production of an A0 in gluon-gluon fusion and in association  with a b bbar, decaying to Z H in the final states nu nubar b bbar or lepton+ lepton- b bbar  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for cross section  limits for mass(A0) = 0.8 -- 2 TeV.


pdgid: S055H2O
text:
SIRUNYAN 2018EE search for the decay H --> A0 A0 --> mu+ mu- tau+ tau- in 35.9  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 4 for limits on the product  of branching ratios in the range mass(A0) = 15 -- 62.5 GeV, normalized to the SM production  cross section. See also their Fig. 5 for interpretation of the data in terms of models with two  Higgs doublets and a singlet.


pdgid: S055H2O
text:
SIRUNYAN 2018F search for a narrow scalar resonance decaying to H H --> W W  b bbar or  Z Z b bbar in the final state lepton lepton nu nu b bbar in 35.9 fb**-1 of p p  collisions at Ecm = 13 TeV. See their Fig. 7 for limits on cross section times branching  ratios for mass(H_{{2}}()0) = 250 -- 900 GeV.


pdgid: S055H2O
text:
AABOUD 2017 search for production of a scalar resonance decaying to Z gamma in 3.2  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 4 for the limits on cross  section times branching ratio for mass(H_{{2}}()0) = 0.25 -- 3.0 TeV.


pdgid: S055H2O
text:
AABOUD 2017AP search for production of a scalar resonance decaying to gamma gamma in 36.7  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 4(a) for limits on fiducial  cross section times branching ratio for mass(H_{{2}}()0) = 0.2 -- 2.7 TeV with narrow width  approximation.


pdgid: S055H2O
text:
AABOUD 2017AW search for production of a scalar resonance decaying to Z gamma in 36.1  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 7 for limits on cross  section times branching ratio for mass(H_{{2}}()0) = 0.25 -- 2.4 TeV.


pdgid: S055H2O
text:
KHACHATRYAN 2017AZ search for the decay H --> A0 A0 --> tau+ tau- tau+ tau-, mu+ mu- b bbar,  and mu+ mu- tau+ tau- in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their  Figs. 4, 5, and 6 for cross section limits in the range mass(A0) = 5 -- 62.5 GeV. See also  their Figs. 7, 8, and 9 for interpretation of the data in terms of models with two Higgs doublets  and a singlet.


pdgid: S055H2O
text:
KHACHATRYAN 2017D search for production of a scalar resonance decaying to Z gamma in 19.7  fb**-1 of p p collisions at Ecm = 8 TeV and 2.7 fb**-1 at Ecm = 13 TeV. See  their Figs. 3 and 4 for the limits on cross section times branching ratio for mass(H_{{2}}()0) =  0.2 -- 2.0 TeV.


pdgid: S055H2O
text:
KHACHATRYAN 2017R search for production of a narrow scalar resonance decaying to gamma gamma in  12.9 fb**-1 (taken in 2016) of p p collisions at Ecm = 13 TeV. See their Fig. 2 for  limits on cross section times branching ratio for mass(H_{{2}}()0) = 0.5 -- 4.5 TeV for several  values of its width-to-mass ratio. Limits from combination with KHACHATRYAN 2016M are shown  in their Figs. 4 and 6.


pdgid: S055H2O
text:
SIRUNYAN 2017CN search for a narrow scalar resonance decaying to H H --> b bbar tau+ tau- in 18.3  fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 5 (above) and Table II for  limits on the cross section times branching ratios for mass(H_{{2}}()0) = 0.3 -- 1 TeV, and  Fig. 6 (above) and Table III for the corresponding limits by combining with data from  KHACHATRYAN 2016BQ and KHACHATRYAN 2015R.


pdgid: S055H2O
text:
SIRUNYAN 2017Y search for production of a scalar resonance decaying to Z gamma in 19.7  fb**-1 of p p collisions at Ecm = 8 TeV and 2.7 fb**-1 at Ecm = 13 TeV. See their Figs. 3, 4 and Table 3 for limits on cross section times branching ratio for  mass(H_{{2}}()0) = 0.7 -- 3.0 TeV, and Fig. 5 for the corresponding limits for mass(H_{{2}}()0) =  0.2 -- 3.0 TeV from combination with KHACHATRYAN 2017D data.


pdgid: S055H2O
text:
AABOUD 2016AB search for associated production of W H with the decay H --> A0 A0 --> b bbar b bbar in  3.2 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for limits on cross  section times branching ratios for mass(A0) = 20 -- 60 GeV.


pdgid: S055H2O
text:
AABOUD 2016AE search for production of a narrow scalar resonance decaying to W+ W- and  Z Z in 3.2 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 4 for limits  on cross section times branching ratio for mass(H_{{2}}()0) = 0.5 -- 3 TeV.


pdgid: S055H2O
text:
AABOUD 2016H search for production of a scalar resonance decaying to gamma gamma in 3.2  fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 12 for limits on cross  section times branching ratio for mass(H_{{2}}()0) = 0.2 -- 2 TeV with different assumptions on  the width.


pdgid: S055H2O
text:
AABOUD 2016I search for a narrow scalar resonance decaying to H H --> b bbar b bbar in  3.2 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 10(c) for limits on  cross section times branching ratios for mass(H_{{2}}()0) = 0.5 -- 3 TeV.


pdgid: S055H2O
text:
AAD 2016AX search for production of a heavy H state decaying to Z Z in the final states lepton+ lepton- lepton+ lepton-, lepton+ lepton- nu nubar, lepton+ lepton- q qbar,  andnu nubar q qbar in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their  Fig.12 for upper limits on CS(H) B(H --> Z Z) for mass(H) ranging from 140 GeV to  1000 GeV.


pdgid: S055H2O
text:
AAD 2016C search for production of a heavy H state decaying to W+ W- in the final    states lepton nu lepton nu and lepton nu q q in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV.  See their Figs. 12, 13, and 16 for upper limits on CS(H) B(H --> W+ W-) for mass(H) ranging from 300 GeV to 1000 or 1500 GeV with various assumptions on the total width of H.


pdgid: S055H2O
text:
AAD 2016L search for the decay H --> A0 A0 --> gamma gamma gamma gamma in 20.3  fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 4 (upper right) for limits on  cross section times branching ratios (normalized to the SM H cross section) for mass(A0) =  10 -- 60 GeV.


pdgid: S055H2O
text:
AAD 2016L search for the decay H_2()0 --> A0 A0 --> gamma gamma gamma gamma in 20.3  fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 4 (lower right) for limits on  cross section times branching ratios for mass(H_{{2}}()0) = 600 GeV and mass(A0) = 10 -- 245  GeV, and Table 5 for limits for mass(H_{{2}}()0)= 300 and 900 GeV.


pdgid: S055H2O
text:
AALTONEN 2016C search for electroweak associated production of H_1()0 H+- followed by the  decays H+- --> H_1()0 W^*, H_1()0 --> gamma gamma for mass(H_{{1}}()0) = 10 -- 105 GeV  and mass(H+-) = 30 -- 300 GeV.  See their Fig. 3 for excluded parameter region in a  two-doublet model in which H_{{1}}()0 has no direct decay to fermions.


pdgid: S055H2O
text:
KHACHATRYAN 2016BG search for a narrow scalar resonance decaying to H H --> b bbar b bbar in 19.7  fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 6 for limits on the cross  section times branching ratios for mass(H_{{2}}()0) = 1.15 -- 3 TeV.


pdgid: S055H2O
text:
KHACHATRYAN 2016BQ search for a resonance decaying to H H --> gamma gamma b bbar in  19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 9 for limits on the  cross section times branching ratios for mass(H_{{2}}()0) = 0.26 -- 1.1 TeV.


pdgid: S055H2O
text:
KHACHATRYAN 2016F search for the decay H --> H_1()0 H_1()0 --> tau+ tau- tau+ tau- in  19.7 fb**-1 of p  p collisions at Ecm = 8 TeV. See their Fig. 8 for cross section  limits for mass(H_{{1}}()0) = 4 -- 8 GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2016M search for production of a narrow resonance decaying to gamma gamma in  19.7 fb**-1 of p p collisions at Ecm = 8 TeV and 3.3 fb**-1 at Ecm = 13  TeV.  See their Fig. 3 (top) for limits on cross section times branching ratio for mass(H_{{2}}()0) =  0.5 -- 4 TeV.


pdgid: S055H2O
text:
KHACHATRYAN 2016P search for gluon fusion production of an H_{{2}}()0 decaying to H H --> b bbar tau+ tau-  in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 8 (lower right) for  cross section limits for mass(H_{{2}}()0) = 260 -- 350 GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2016P search for gluon fusion production of an A0 decaying to Z H --> lepton+ lepton- tau+ tau- in  19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 10 for cross section  limits for mass(H_{{2}}()0) = 220 -- 350 GeV.


pdgid: S055H2O
text:
AAD 2015BK search for production of a heavy H_{{2}}()0 decaying to H H in the final  state b bbar b bbar in 19.5 fb**-1 of p p collisions at Ecm = 8 TeV. See their  Fig. 14(c) for CS(H_{{2}}()0) B(H_2()0 --> H H) for mass(H_{{2}}()0) = 500 -- 1500 GeV  with width(H_{{2}}()0) = 1 GeV.


pdgid: S055H2O
text:
AAD 2015BZ search for the decay H --> A0 A0 --> mu+ mu- tau+ tau- (mass(H) = 125 GeV)   in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 6 for limits on cross  section times branching ratio for mass(A0) = 3.7 -- 50 GeV.


pdgid: S055H2O
text:
AAD 2015BZ search for a state H_{{2}}()0 via the decay H_2()0 --> A0 A0 --> mu+ mu- tau+ tau- in   20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 6 for limits on cross  section times branching ratio for mass(H_{{2}}()0) = 100 -- 500 GeV and mass(A0) = 5 GeV.


pdgid: S055H2O
text:
AAD 2015CE search for production of a heavy H_{{2}}()0 decaying to H H in the  final states b bbar tau+ tau- and gamma gamma W W^* in 20.3 fb**-1 of p p  collisions at Ecm = 8 TeV and combine with data from AAD 2015H and AAD 2015BK. A  limit CS(H_{{2}}()0) B(H_2()0 --> H H) < 2.1 -- 0.011 pb (95% CL) is  given for mass(H_{{2}}()0) = 260 -- 1000 GeV. See their Fig. 6.


pdgid: S055H2O
text:
AAD 2015H search for production of a heavy H_{{2}}()0 decaying to H H in the finalstate  gamma gamma b bbar in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV.A limit of  CS(H_{{2}}()0) B(H_2()0 --> H H) < 3.5 -- 0.7 pb is given for mass(H_{{2}}()0) =  260 -- 500 GeV at 95% CL. See their Fig. 3.


pdgid: S055H2O
text:
AAD 2015S search for production of A0 decaying to Z H --> lepton+ lepton- b bbar, nu nubar b bbar and   lepton+ lepton- tau+ tau- in 20.3 fb**-1 of p p collisions at  Ecm = 8 TeV.  See   their Fig. 3 for cross section limits for mass(A0) = 200 -- 1000  GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2015AW search for production of a heavy state H_2^0 of an electroweak singlet  extension of the Standard Model via the decays of H_2^0 to W+ W- and Z Z  in up to 5.1  fb**-1 of p p collisions at Ecm = 7 TeV and up to 19.7 fb**-1 at Ecm = 8  TeV in the range mass(H_{{2}}()0) = 145 -- 1000 GeV. See their Figs. 8 and 9 for limits in the  parameter space of the model.


pdgid: S055H2O
text:
KHACHATRYAN 2015BB search for production of a resonance H decaying to   gamma gamma  in    19.7 fb**-1 of p p collisions at Ecm = 8 TeV.  See their Fig. 7 for limits on  cross section times branching ratio for mass(H) = 150 -- 850 GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2015N search for production of A0 decaying to  Z H --> lepton+ lepton- b bbar in  19.7 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 3 for limits on cross  section times branching ratios for mass(A0) = 225 -- 600 GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2015O search for production of a high-mass narrow resonance A0 decaying to Z H --> q qbar tau+ tau- in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV.  See their Fig. 6 for limits on cross section times branching ratios for mass(A0) = 800 -- 2500 GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2015R search for a narrow scalar resonance decaying to H H --> b bbar b bbar in 17.9  fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 5 (top) for limits on cross  section times branching ratios for mass(H_{{2}}()0) = 0.27 -- 1.1 TeV.


pdgid: S055H2O
text:
AAD 2014AP search for a second H state decaying to gamma gamma in addition to the state at about 125 GeV in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 4 for limits on cross section times branching ratio for mass(H) = 65 -- 600 GeV.


pdgid: S055H2O
text:
AAD 2014M search for the decay cascade H_2()0 --> H+- W-+ --> H W+- W-+, H decaying  to b bbar in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Table III  for limits on cross section times branching ratio for mass(H_{{2}}()0)= 325 -- 1025 GeV and  mass(H+)= 225 -- 925 GeV.


pdgid: S055H2O
text:
CHATRCHYAN 2014G search for a second H state decaying to W W^(*)() in addition to the observed signal at about 125 GeV using 4.9 fb**-1 of p p collisions at Ecm = 7 TeV and 19.4 fb**-1 at Ecm = 8 TeV. See their Fig. 21 (right) for cross section limits in the mass range 110 -- 600 GeV.


pdgid: S055H2O
text:
KHACHATRYAN 2014P search for a second H state decaying to gamma gamma in addition to the observed signal at about 125 GeV using 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. See their Figs. 27 and 28 for cross section limits in the mass range 110 -- 150 GeV.


pdgid: S055H2O
text:
AALTONEN 2013P search for production of a heavy Higgs boson H^'()0 that decays into a charged Higgs boson H+- and a lighter Higgs boson H via the decay chain H^'()0 --> H+- W-+, H+- --> W+- H, H --> b bbar in the final state lepton nu plus 4 jets in 8.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. See their Fig. 4 for limits on cross section times branching ratio in the mass(H+-)-mass(H^'()0) plane for mass(H) = 126 GeV.


pdgid: S055H2O
text:
CHATRCHYAN 2013BJ search for H production in the decay chain H --> A0 A0, A0 --> mu+ mu- in 5.3 fb**-1 of p p collisions at Ecm = 7 TeV. See their Fig. 2 for limits on cross section times branching ratio.


pdgid: S055H2O
text:
ABBIENDI 2010 search for e+ e- --> Z H with the decay chain H --> chitilde_1()0 chitilde_2()0, chitilde_2()0 --> chitilde_1()0 + (gamma or Z^*()), when chitilde_{{1}}()0 and chitilde_{{2}}()0 are nearly degenerate. For a mass difference of 2 (4) GeV, a lower limit on mass(H) of 108.4 (107.0) GeV (95% CL) is obtained for SM Z H cross section and B(H --> chitilde_1()0 chitilde_2()0) = 1.


pdgid: S055H2O
text:
SCHAEL 2010 search for the process e+ e- -->  H Z followed by the decay chain  H --> A0 A0 --> tau+ tau- tau+ tau- with Z --> lepton+ lepton-, nu nubar at Ecm = 183 -- 209 GeV. For a H Z Z coupling equal to the SM value, B(H --> A0 A0) = B(A0 --> tau+ tau-) = 1, and mass(A0) = 4 -- 10 GeV,  mass(H) up to 107 GeV is excluded at 95% CL.


pdgid: S055H2O
text:
ABAZOV 2009V search for H production followed by the decay chain H --> A0 A0 --> mu+ mu- mu+ mu- or mu+ mu- tau+ tau- in 4.2 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. See their Fig. 3 for limits on sigma(H).B(H --> A0 A0) for mass(A0) = 3.6 -- 19 GeV.


pdgid: S055H2O
text:
ABBIENDI 2004K search for e+ e- --> H Z with H decaying to two jets of any flavor including g g.  The limit is for SM production cross section with B(H --> j j) = 1.


pdgid: S055H2O
text:
ABDALLAH 2004 consider the full combined LEP and LEP2 datasets to set limits on the Higgs coupling to W or Z bosons, assuming SM decays of the Higgs. Results in Fig. 26.


pdgid: S055H2O
text:
ACHARD 2004B search for e+ e- --> H Z with H decaying to b bbar, c cbar, or g g.  The limit is for SM production cross section with B(H --> j j) = 1.


pdgid: S055H2O
text:
ACHARD 2004F search for H with anomalous coupling to gauge boson pairs in the processes e+ e- --> H gamma, e+ e- H, H Z with decays H --> f fbar, gamma gamma, Z gamma, and W^* W at Ecm = 189 -- 209 GeV. See paper for limits.


pdgid: S055H2O
text:
ABBIENDI 2003F search for H --> anything in e+ e- --> H Z, using the recoil mass spectrum of Z --> e+ e- or mu+ mu-. In addition, it searched for Z --> nu nubar and H --> e+ e- or photons. Scenarios with large width or continuum H mass distribution are considered. See their Figs. 11--14 for the results.


pdgid: S055H2O
text:
ABBIENDI 2003G search for e+ e- --> H_1()0 Z followed by H_1()0 --> A0 A0, A0 --> c cbar, g g, or tau+ tau- in the region mass(H_{{1}}()0) = 45-86 GeV and mass(A0) = 2-11 GeV. See their Fig. 7 for the limits.


pdgid: S055H2O
text:
Search for associated production of a gamma gamma resonance with a Zboson, followed by Z --> q qbar, lepton+ lepton-, or nu nubar, at Ecm<=209 GeV.  The limit is for a H with SM production cross section and B(H --> f fbar)=0 for all fermions f.


pdgid: S055H2O
text:
ACCIARRI 2000R search for e+ e- --> H gamma with H --> b bbar, Z gamma, or gamma gamma.  See their Fig.3 for limits on sigma.B.  Explicit limits within an effective interaction framework are also given, for which the Standard Model Higgs search results are used in addition.


pdgid: S055H2O
text:
ACCIARRI 2000R search for the two-photon type processes e+ e- --> e+ e- H with H --> b bbar or gamma gamma. See their Fig.4 for limits on Gamma(H --> gamma gamma).B(H --> gamma gamma  or  b bbar) for mass(H)=70 -- 170 GeV.


pdgid: S055H2O
text:
GONZALEZ-GARCIA 1998B use D0 limit for gamma gamma events with missing E(T) in p pbar collisions (ABBOTT 1998) to constrain possible Z H or W H production followed by unconventional H --> gamma gamma decay which is induced by higher-dimensional operators.  See their Figs.1 and2 for limits on the anomalous couplings.


pdgid: S055H2O
text:
KRAWCZYK 1997 analyse the muon anomalous magnetic moment in a two-doublet Higgs model (with typeII Yukawa couplings) assuming no H_1()0 Z Z  coupling and obtain mass(H_{{1}}()0)~>5 GeV or mass(A0)~>5 GeV for tan(beta)>50. Other Higgs bosons are assumed to be much heavier.


pdgid: S055H2O
text:
ALEXANDER 1996H give B(Z --> H gamma)*B(H --> q qbar) <1 -- 4E-5 (95%CL) and B(Z --> H gamma)*B(H --> b bbar) <0.7 -- 2E-5 (95%CL) in the range 20 <mass(H) <80 GeV.


pdgid: S055HEW
text:
HALLER 2018 make Standard Model fits to Z and neutral current parameters, mass(t),  mass(W), and width(W) measurements available in 2018. The direct mass measurement at the LHC is  not used in the fit.


pdgid: S055HEW
text:
BAAK 2012 make Standard Model fits to Z and neutral current parameters, mass(t), mass(W), and width(W)  measurements available in 2010 (using also preliminary data). The quoted result is obtained from a fit that does not include the limit from the direct Higgs searches. The result including direct search data from LEP2,  the Tevatron and the LHC is 120+12-5 GeV.


pdgid: S055HEW
text:
BAAK 2012A make Standard Model fits to Z and neutral current parameters, mass(t), mass(W), and width(W) measurements available in 2012 (using also preliminary data). The quoted result is obtained from a fit that does not include the measured mass value of the signal observed at the LHC and also no limits from direct Higgs searches.


pdgid: S055HEW
text:
ERLER 2010A makes Standard Model fits to Z and neutral current parameters, mass(t), mass(W) measurements available in 2009 (using also preliminary data). The quoted result is obtained from a fit that does not include the limits from the direct Higgs searches. With direct search data from LEP2 and Tevatron  added to the fit, the 90% CL (99% CL) interval is 115 -- 148 (114 -- 197) GeV.


pdgid: S055HEW
text:
LEP-SLC 2006 make Standard Model fits to Z parameters from LEP/SLC and mass(t), mass(W), and  Gamma(W) measurements available in 2005 with Deltaalpha(had)**(5)(mass(Z)) = 0.02758+-0.00035. The 95% CL limit is 285 GeV.


pdgid: S064HGC
text:
AAD 2015AF search for t tbar production followed by t --> b H+, H+ --> tau+ nu in 19.5 fb**-1 of p p collisions at Ecm = 8 TeV. Upper limits on B(t --> b H+) B(H+ --> tau nu) between 2.3E-3 and 1.3E-2 (95% CL) are given for mass(H+) = 80 -- 160 GeV. See their Fig. 8 for the excluded regions in different benchmark scenarios of the MSSM. The region mass(H+) < 140 GeV is excluded for tan(beta) > 1 in the considered scenarios.


pdgid: S064HGC
text:
KHACHATRYAN 2015AX search for t tbar production followed by t --> b H+, H+ --> tau+ nu in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. Upper limits on B(t --> b H+) B(H+ --> tau nu) between 1.2E-2 and 1.5E-3 (95% CL) are given for mass(H+) = 80 -- 160 GeV. See their Fig. 11 for the excluded regions in different benchmark scenarios of the MSSM. The region mass(H+) < 155 GeV is excluded for tan(beta) > 1 in the considered scenarios.


pdgid: S064HGC
text:
LEP 2013 give a limit that refers to the Type II scenario. The limit for B(H+ --> tau nu) = 1 is 94 GeV (95% CL), and for B(H+ --> c s) = 1 the region below 80.5 as well as the region 83 -- 88 GeV is excluded (95% CL). LEP 2013 also search for the decay mode H+ --> A0 W^*() with A0 --> b bbar, which is not negligible in Type I models. The limit in Type I models is 72.5 GeV (95% CL) if mass(A0) > 12 GeV.


pdgid: S064HGC
text:
AAD 2025 combine AAD 2023AH and AAD 2024AD and derive limits on the isotriplet  contribution to the gauge boson masses in the Georgi-Machacek model.  See their Fig. 5(c).


pdgid: S064HGC
text:
HAYRAPETYAN 2024AV search for production of scalar resonance decaying to W+- gamma with  W --> lepton nu in 138 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 7  for limits on cross section times branching ratio for the mass range 0.3 -- 2.0 TeV for a  narrow and a broad width. Combined limits with TUMASYAN 2022B are shown in Fig. 8.


pdgid: S064HGC
text:
AAD 2023AH search for vector boson fusion production of H+- decaying to H+- --> W+- Z --> lepton+- nu lepton+ lepton- in 139   fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 9 for limits on cross   section times branching ratio in the Georgi-Machacek model for mass(H+-) = 0.2 -- 1.0 TeV,  and also for limits on the  triplet vacuum expectation value fraction.


pdgid: S064HGC
text:
AAD 2023BB search for t tbar production followed by t --> b H+, H+ --> c bbar in  139 fb**-1 of p p collisions at Ecm = 13 TeV.  See their Fig. 8 for limits on the  product of branching ratios for mass(H+) = 60 -- 160 GeV.


pdgid: S064HGC
text:
AAD 2023BW search for t --> b H+ from pair produced top quarks, with the decay chain  H+ --> W+ A0, A0 --> mu+ mu- using 139 fb**-1 of p p collisions at Ecm = 13  TeV. See their Fig. 5(b)-(d) for limits on the product of branching ratios for mass(H+) = 120,  140, 160 GeV, and mass(A0) = 15 -- 72 GeV.


pdgid: S064HGC
text:
TUMASYAN 2023AV search for production of H+- in association with a top quark, decaying to  H_2()0 W+-, H_2()0 --> tau+ tau-, using 138 fb**-1 of p p collisions at Ecm =  13 TeV.  See their Fig. 9 for limits on production cross section times branching ratios for  mass(H+-) = 0.3 -- 0.7 TeV and mass(H_{{2}}()0) = 0.2 TeV.


pdgid: S064HGC
text:
TUMASYAN 2022B search for production of scalar resonance decaying to W+- gamma --> q q gamma in 137  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 5 for limits on cross  section times branching ratio for the mass range 0.7 -- 6.0 TeV, assuming narrow width or  Gamma/M = 0.05.


pdgid: S064HGC
text:
AAD 2021V search for tbar b H+ associated production followed by H+ --> t bbar in 139  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 6 for upper limits on cross  section times branching ratio for mass(H+) = 0.2 -- 2 TeV. See also their Fig. 7 for the  excluded region in the parameter space of the hMSSM and the following MSSM benchmark scenarios:  M_{{h}}^125, M_{{h}}^125(chitilde), M_{{h}}^125(tautilde), M_{{h}}^125(alignment),  M(h(1))**125(CPV).


pdgid: S064HGC
text:
SIRUNYAN 2021W search for vector boson fusion production of H+ decaying to H+ --> W+ Z --> lepton+ nu lepton+ lepton- in 137  fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for limits on cross  section times branching ratio for mass(H+) = 0.2 -- 3.0 TeV, and also for limits on the   fraction of the triplet vev contribution to the W mass in the Georgi-Machacek model.


pdgid: S064HGC
text:
AAD 2020W search for dijet resonances in events with isolated leptons using 139 fb**-1 of  p p collisions at Ecm = 13 TeV.  As a byproduct, H+ --> t bbar produced in  association with  tbar b is searched for. Limits on the product of cross section times  branching ratio for mass(H+) = 0.6 -- 2 TeV are given in their Fig. 5(c).


pdgid: S064HGC
text:
SIRUNYAN 2020AO search for H+ --> t bbar produced in association with  t(b) in  all jet final states in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.  See their  Fig. 6 for limits on the product of cross section times branching ratio for mass(H+) = 0.2 -- 3 TeV.   Limits for s-channel production are also given for  mass(H+) = 0.8 -- 3 TeV.  See also  Fig. 7 for the corresponding limits in scenarios in the minimal supersymmetric standard model.   Cross section limits from combined results with SIRUNYAN 2020AV are given in Fig. 8.


pdgid: S064HGC
text:
SIRUNYAN 2020AV search for H+ --> t bbar produced in association with t(b) in  final states with one or two leptons, in 35.9 fb**-1 of p p collisions at Ecm = 13  TeV.  See their Fig. 5 for limits on the product of cross section times branching ratio for  mass(H+) = 0.2 -- 3 TeV, and their Fig. 6 for the corresponding limits in scenarios in the  minimal supersymmetric standard model.


pdgid: S064HGC
text:
SIRUNYAN 2020BE search for t --> b H+ followed by the decay H+ --> c sbar in pair  produced top quark events using 35.9 fb**-1 of p p collisions at Ecm = 13 TeV.   Limits on the branching ratio in the range 1.68 -- 0.25% (95%CL) are given for  mass(H+) = 80 -- 160 GeV, see their Fig. 4.


pdgid: S064HGC
text:
SIRUNYAN 2019AH search for H+ in the decay of a pair-produced t quark, or in  associated t b H+ or nonresonant b bbar H+ W- production, followed by H+ --> tau+ nu,  in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. Upper limits on cross section times  branching ratio between 6 pb and 5 fb (95% CL) are given for mass(H+) = 80 -- 3000  GeV (including the non-resonant production near the top quark mass), see their Fig. 6 (left). See  their Fig. 6 (right) for the excluded regions in the m(h)**mod- scenario of  the MSSM.


pdgid: S064HGC
text:
SIRUNYAN 2019BP search for vector boson fusion production of H+ decaying to H+ --> W+ Z --> lepton+ nu lepton+ lepton- in  35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 7 for limits on cross  section times branching ratio for mass(H+) = 0.3 -- 2.0 TeV, and also for limits on the  fraction of the triplet vev contribution to the W mass in the Georgi-Machacek model.


pdgid: S064HGC
text:
SIRUNYAN 2019CC search for t --> b H+ from pair produced top quarks, with the decay chain  H+ --> W+ A0, A0 --> mu+ mu- in 35.9 fb**-1 of p p collisions at Ecm = 13  TeV.  See their Fig. 2 for limits on the product of branching ratios for mass(A0) = 15 -- 75 GeV.


pdgid: S064HGC
text:
SIRUNYAN 2019CQ search for vector boson fusion production of H+ decaying to H+ --> W+ Z --> lepton+ nu q qbar or  q qbar lepton+ lepton- in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See  their Fig. 5 for limits on cross section times branching ratio for mass(H+) = 0.6 -- 2.0  TeV, and also for limits on the triplet vacuum expectation value fraction in the Georgi-Machacek  model.


pdgid: S064HGC
text:
AABOUD 2018BW search for tbar b H+ associated production or the decay t --> b H+,  followed by H+ --> tau+ nu, in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See  their Fig. 8(a) for upper limits on cross section times branching ratio for mass(H+) = 90 -- 2000  GeV, and Fig. 8(b) for limits on B(t --> b H+) B(H+ --> tau+ nu) for mass(H+) =  90 -- 160 GeV.  See also their Fig. 9 for the excluded region in the hMSSM parameter space.


pdgid: S064HGC
text:
AABOUD 2018CD search for tbar b H+ associated production followed by H+ --> t bbar in  36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for upper limits on  cross section times branching ratio for mass(H+) = 0.2 -- 2 TeV.  See also their Fig. 9 for  the excluded region in the parameter space of the m(h)**mod- and hMSSM scenarios  of the MSSM. The theory predictions overlaid to the experimental limits to determine the excluded  mass(H+) range are shown without their respective uncertainty band.


pdgid: S064HGC
text:
AABOUD 2018CH search for vector boson fusion production of H+- decaying to H+- --> W+- Z --> lepton+- nu lepton+ lepton- in  36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 7 for limits on cross  section times branching ratio for mass(H+-) = 0.2 -- 0.9 TeV, and also for limits on the  triplet vacuum expectation value fraction in the Georgi-Machacek model.


pdgid: S064HGC
text:
HALLER 2018 give 95% CL lower limits on mass(H+) of 590 GeV in type II two Higgs  doublet model from combined data (including an unpublished BELLE result) for B(b --> s gamma).


pdgid: S064HGC
text:
SIRUNYAN 2018DO search for t tbar production followed by t --> b H+, H+ --> c bbar in 19.7  fb**-1 of p p collisions at Ecm = 8 TeV.  See their Fig. 3 for upper limits on  B(t --> b H+) for mass(H+) = 90 -- 150 GeV assuming that B(H+ --> c bbar) = 1  and B(t --> b H+) + B(t --> b W+) = 1.


pdgid: S064HGC
text:
MISIAK 2017 give 95% CL lower limits on mass(H+) between 570 and 800 GeV in type II  two Higgs doublet model from combined data (including an unpublished BELLE result) for B(b --> s ( d ) gamma).


pdgid: S064HGC
text:
SIRUNYAN 2017AE search for vector boson fusion production of H+- decaying to H+- --> W+- Z --> lepton+- nu lepton+ lepton- in  15.2 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 3 for limits on cross  section times branching ratio for mass(H+-) = 0.2 -- 2.0 TeV, and also for limits on the  triplet vacuum expectation value fraction in the Georgi-Machacek model.


pdgid: S064HGC
text:
AABOUD 2016A search for t(b) H+- associated production followed by H+ --> tau+ nu in  3.2 fb**-1 of p p collisions at Ecm = 13 TeV. Upper limits on CS(t(b) H+-)  B(H+ --> tau nu) between 1.9 pb and 15 fb (95% CL) are given for mass(H+) = 200 -- 2000  GeV, see their Fig. 6. See their Fig. 7 for the excluded regions in the hMSSM scenario.


pdgid: S064HGC
text:
AAD 2016AJ search for t(b) H+- associated production followed by H+- --> t b  in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 6 for upper limits on  CS(t(b) H+-) B(H+ --> t b) for mass(H+) = 200 -- 600 GeV.


pdgid: S064HGC
text:
AAD 2016AJ search for H+- production from quark-antiquark annihilation, followed by  H+- --> t b, in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 10  for upper limits on CS(H+-) B(H+ --> t b) for mass(H+) = 400 -- 3000 GeV.


pdgid: S064HGC
text:
AAD 2015AF search for t H+- associated production followed by H+- --> tau+- nu in 19.5 fb**-1 of p p collisions at Ecm = 8 TeV. Upper limits on CS(t H+-) B(H+ --> tau nu) between 760 and 4.5 fb (95% CL) are given for mass(H+) = 180 -- 1000 GeV. See their Fig. 8 for the excluded regions in different benchmark scenarios of the MSSM.


pdgid: S064HGC
text:
AAD 2015M search for vector boson fusion production of H+- decaying to H+- --> W+- Z --> q qbar lepton+ lepton- in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Fig. 2 for limits on cross section times branching ratio for mass(H+-) = 200 -- 1000 GeV, and Fig. 3 for limits on  thetriplet vacuum expectation value fraction in the Georgi-Machacek model.


pdgid: S064HGC
text:
KHACHATRYAN 2015AX search for t H+- associated production followed by H+- --> t b in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. Upper limits on CS(t H+-) B(H+ --> t bbar) between 2.0 and 0.13 pb (95% CL) are given for mass(H+) = 180 -- 600 GeV. See their Fig. 11 for the excluded regions in different benchmark scenarios of the MSSM.


pdgid: S064HGC
text:
KHACHATRYAN 2015AX search for t H+- associated production followed by H+- --> tau+- nu in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. Upper limits on CS(t H+-) B(H+ --> tau nu) between 380 and 25 fb (95% CL) are given for mass(H+) = 180 -- 600 GeV. See their Fig. 11 for the excluded regions in different benchmark scenarios of the MSSM.


pdgid: S064HGC
text:
KHACHATRYAN 2015BF search for t tbar production followed by t --> b H+, H+ --> c sbar in 19.7 fb**-1 of p p collisions at Ecm = 8 TeV. Upper limits on B(t --> b H+) B(H+ --> c sbar) between 1.2E-2 and 6.5E-2 (95% CL) are given for mass(H+) = 90 -- 160 GeV.


pdgid: S064HGC
text:
AAD 2014M search for the decay cascade H_2()0 --> H+- W-+ --> H0 W+- W-+, H0 decaying to b bbar in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. See their Table III for limits on cross section times branching ratio for mass(H_{{2}}()0)= 325 -- 1025 GeV and mass(H+)= 225 -- 925 GeV.


pdgid: S064HGC
text:
AALTONEN 2014A measure B(t --> b tau nu) = 0.096+-0.028 using 9 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. For mass(H+)= 80 -- 140 GeV, this measured value is translated to a limit B(t --> b H+) < 0.059 at 95% CL assuming B(H+ --> tau+ nu) = 1.


pdgid: S064HGC
text:
AAD 2013AC search for t tbar production followed by t --> b H+, H+ --> c sbar (flavor unidentified) in 4.7 fb**-1 of p p collisions at Ecm = 7 TeV. Upper limits on B(t --> b H+) between 0.05 and 0.01 (95%CL) are given for mass(H+)=90 -- 150 GeV and B(H+ --> c sbar)=1.


pdgid: S064HGC
text:
AAD 2013V search for t tbar production followed by t --> b H+, H+ --> tau+ nu through violation of lepton universality with 4.6 fb**-1 of p p collisions at Ecm = 7 TeV. Upper limits on B(t --> b H+) between 0.032 and 0.044 (95% CL) are given for mass(H+) = 90 -- 140 GeV and B(H+ --> tau+ nu) = 1. By combining with AAD 2012BH, the limits improve to 0.008 to 0.034 for mass(H+) = 90 -- 160 GeV. See their Fig. 7 for the excluded region in the m(h)**max scenario of the MSSM.


pdgid: S064HGC
text:
AAD 2012BH search for t tbar production followed by t --> b H+, H+ --> tau+ nu with 4.6 fb**-1 of p p collisions at Ecm = 7 TeV. Upper limits on B(t --> b H+) between 0.01 and 0.05 (95% CL) are given for mass(H+) = 90 -- 160 GeV and B(H+ --> tau+ nu) = 1. See their Fig.8 for the excluded region in the m(h)**max scenario of the MSSM.


pdgid: S064HGC
text:
CHATRCHYAN 2012AA search for t tbar production followed by t --> b H+, H+ --> tau+ nu with 2 fb**-1 of p p collisions at Ecm = 7 TeV. Upper limits on B(t --> b H+) between 0.019 and 0.041 (95% CL) are given for mass(H+) = 80 -- 160 GeV and B(H+ --> tau+ nu)=1.


pdgid: S064HGC
text:
AALTONEN 2011P search in 2.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV for the decay chain t --> b H+, H+ --> W+ A0, A0 --> tau+ tau- with mass(A0) between 4 and 9 GeV. See their Fig.4 for limits on B(t --> b H+) for 90 < mass(H+)< 160 GeV.


pdgid: S064HGC
text:
DESCHAMPS 2010 make Type II two Higgs doublet model fits to weak leptonic and semileptonic decays, b --> s gamma, B, B_{{s}}() mixings, and Z --> b bbar. The limit holds irrespective of tan(beta).


pdgid: S064HGC
text:
AALTONEN 2009AJ search for t --> b H+, H+ --> c sbar in t tbar events in 2.2 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. Upper limits on B(t --> b H+) between 0.08 and 0.32 (95% CL) are given for mass(H+) = 60 -- 150 GeV and B(H+ --> c sbar) = 1.


pdgid: S064HGC
text:
ABAZOV 2009AC search for t --> b H+, H+ --> tau+ nu in t tbar events in 0.9 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. Upper limits on B(t --> b H+) between 0.19 and 0.25 (95% CL) are given for mass(H+) = 80 -- 155 GeV and B(H+ --> tau+ nu) = 1. See their Fig.4 for an excluded region in a MSSM scenario.


pdgid: S064HGC
text:
ABAZOV 2009AG measure t tbar cross sections in final states with lepton + jets (lepton = e, mu), lepton lepton, and tau lepton in 1 fb**-1 of p pbar collisions at Ecm = 1.96 TeV, which constrains possible t --> b H+ branching fractions. Upper limits (95% CL) on B(t --> b H+) between 0.15 and 0.40 (0.48 and 0.57) are given for B(H+ --> tau+ nu) = 1 (B(H+ --> c sbar) = 1) for mass(H+) = 80 -- 155 GeV.


pdgid: S064HGC
text:
ABAZOV 2009AI search for t --> b H+ in t tbar events in 1 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. Final states with lepton + jets (lepton = e, mu), lepton lepton, and tau lepton are examined. Upper limits on B(t --> b H+) (95% CL) between 0.15 and 0.19 (0.19 and 0.22) are given for B(H+ --> tau+ nu) = 1 (B(H+ --> c sbar) = 1) for mass(H+) = 80 -- 155 GeV. For B(H+ --> tau+ nu) = 1 also a simultaneous extraction of B(t --> b H+) and the t tbar cross section is performed, yielding a limit on B(t --> b H+) between 0.12 and 0.26 for mass(H+) = 80 -- 155 GeV. See their Figs.5 -- 8 for excluded regions in several MSSM scenarios.


pdgid: S064HGC
text:
ABAZOV 2009P search for H+ production by q qbar^'() annihilation followed by H+ --> t bbar decay in 0.9 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. Cross section limits in several two-doublet models are given for mass(H+) = 180 -- 300 GeV. A region with 20 ~< tan(beta) ~< 70 is excluded (95% CL) for 180 GeV ~< mass(H+) ~< 184 GeV in type-I models.


pdgid: S064HGC
text:
ABULENCIA 2006E search for associated H0 W production in p pbar collisions at Ecm = 1.96 TeV. A fit is made for t tbar production processes in dilepton, lepton + jets, and lepton + tau final states, with the decays t --> W+ b and t --> H+ b followed by H+ --> tau+ nu, c sbar, t^* bbar, or W+ H0. Within the MSSM the search is sensitive to the region tan(beta)< 1 or > 30 in the mass range mass(H+) = 80 -- 160 GeV. See Fig. 2 for the excluded region in a certain MSSM scenario.


pdgid: S064HGC
text:
ABDALLAH 2004I search for e+ e- --> H+ H- with H+- decaying to tau nu, c s, or W^* A0 in Type-I two-Higgs-doublet models.


pdgid: S064HGC
text:
ABAZOV 2002B search for a charged Higgs boson in top decays with H+ --> tau+ nu at Ecm=1.8 TeV. For mass(H+)=75 GeV, the region tan(beta)>32.0 is excluded at 95%CL. The excluded mass region extends to over 140 GeV for tan(beta) values above 100.


pdgid: S064HGC
text:
BORZUMATI 2002 point out that the decay modes such as b bbar W, A0 W, and supersymmetric ones can have substantial branching fractions in the mass range explored at LEPII and Tevatron.


pdgid: S064HGC
text:
BARATE 2001E give a limit tan(beta)/mass(H+)<0.40 GeV**-1 (90% CL) in TypeII two-doublet models. An independent measurement of B --> tau nu_tau X gives tan(beta)/mass(H+)<0.49 GeV**-1 (90% CL).


pdgid: S064HGC
text:
GAMBINO 2001 use the world average data in the summer of 2001 B(b --> s gamma) = 3.23+-0.42E-4. The limit applies for Type-II two-doublet models.


pdgid: S064HGC
text:
AFFOLDER 2000I search for a charged Higgs boson in top decays with H+ --> tau+ nu in p pbar collisions at Ecm=1.8TeV. The excluded mass region extends to over 120GeV for tan(beta) values above 100 and B(tau nu) = 1. If B(t --> b H+)~>0.6, mass(H+) up to 160 GeV is excluded. Updates ABE 1997L.


pdgid: S064HGC
text:
ABBOTT 1999E search for a charged Higgs boson in top decays in p pbar collisions at Ecm=1.8 TeV, by comparing the observed t tbar cross section (extracted from the data assuming the dominant decay t --> b W+) with theoretical expectation. The search is sensitive to regions of the domains tan(beta)~<1, 50<mass(H+)(GeV) ~<120 and tan(beta)~>40, 50<mass(H+) (GeV) ~<160. See Fig.3 for the details of the excluded region.


pdgid: S064HGC
text:
ACKERSTAFF 1999D measure the Michel parameters rho, xi, eta, and xidelta in leptonic taudecays from Z --> tau tau. Assuming e-mu universality, the limit mass(H+)>0.97 tan(beta) GeV (95%CL) is obtained for two-doublet models in which only one doublet couples to leptons.


pdgid: S064HGC
text:
ACCIARRI 1997F give a limit mass(H+)>2.6 tan(beta) GeV (90% CL) from their limit on the exclusive B --> tau nu_tau branching ratio.


pdgid: S064HGC
text:
AMMAR 1997B measure the Michel parameterrho from tau --> e nu nu decays and assumes e/mu universality to extract the Michel etaparameter from tau --> mu nu nu decays. The measurement is translated to a lower limit on mass(H+) in a two-doublet model mass(H+)>0.97 tan(beta) GeV (90%CL).


pdgid: S064HGC
text:
COARASA 1997 reanalyzed the constraint on the (mass(H+-),tan(beta)) plane derived from the inclusive B --> tau nu_tau X branching ratio in GROSSMAN 1995B and BUSKULIC 1995. They show that the constraint is quite sensitive to supersymmetric one-loop effects.


pdgid: S064HGC
text:
GUCHAIT 1997 studies the constraints on mass(H+) set by Tevatron data on lepton tau final states in t tbar --> (W b) (H b), W --> lepton nu, H --> tau nu_tau. See Fig.2 for the excluded region.


pdgid: S064HGC
text:
MANGANO 1997 reconsiders the limit in ACCIARRI 1997F including the effect of the potentially large B_c --> tau nu_tau background to B_u --> tau nu_tau decays. Stronger limits are obtained.


pdgid: S064HGC
text:
STAHL 1997 fit tau lifetime, leptonic branching ratios, and the Michel parameters and derive limit mass(H+)>1.5 tan(beta) GeV (90%CL) for a two-doublet model. See also STAHL 1994.


pdgid: S064HGC
text:
ALAM 1995 measure the inclusive b --> s gamma branching ratio at Upsilon(4S) and give B(b --> s gamma)<4.2E-4 (95%CL), which translates to the limit mass(H+)>[244+63/(tan(beta))**1.3] GeV in the TypeII two-doublet model. Light supersymmetric particles can invalidate this bound.


pdgid: S064HGC
text:
BUSKULIC 1995 give a limit mass(H+)>1.9 tan(beta) GeV (90% CL) for Type-II models from b --> tau nu_tau X branching ratio, as proposed in GROSSMAN 1994.


pdgid: S064HGT
text:
AABOUD 2018BW search for tbar b H+ associated production in 36.1 fb**-1 of p p collisions at Ecm = 13 TeV. See also their Fig. 9 for the excluded region in the hMSSM parameter space.


pdgid: S064HD1
text:
AAD 2023AI search for H++ H-- production using 139 fb**-1 of p p collisions at    Ecm = 13 TeV.  Decay branching ratios B(H++ --> lepton+ lepton^'+) for the six flavor   combinations are assumed to be equal, adding up to unity.  If the T(3) = 0 states are   degenerate with the T(3)  = +-1 states, the limit becomes 1080 GeV.


pdgid: S064HD1
text:
AABOUD 2019K search for pair production of H++ H-- followed by the decay H+-+- --> W+- W+- in  36.1 fb**-1 of p p collisions at Ecm = 13 TeV.  The search is interpreted in a  doublet-triplet extension of the scalar sector with a vev of 0.1 GeV, leading to B(H+-+- --> W+- W+-) =  1.   See their Fig. 5 for limits on the cross section for mass(H++) between 200 and 700 GeV.


pdgid: S064HD1
text:
AAD 2015AG search for H++ H-- production in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. The limit assumes 100% branching ratio to the specified final state. See their Fig. 5 for limits for arbitrary branching ratios.


pdgid: S064HD1
text:
AAD 2015AP search for H()++ H()-- production in 20.3 fb**-1 of p p collisions at   Ecm = 8 TeV. The limit assumes 100% branching ratio to the specified final state.


pdgid: S064HD1
text:
CHATRCHYAN 2012AU search for H()++ H()-- production with 4.9 fb**-1 of p p collisions at Ecm = 7 TeV. The limit assumes 100% branching ratio to the specified final state. See their Table 6 for limits including associated H()++ H()- production or assuming different scenarios.


pdgid: S064HD1
text:
ABDALLAH 2003 search for H++ H-- pair production either followed by H++ --> tau+ tau+, or decaying outside the detector.


pdgid: S064HD1
text:
ABBIENDI 2002C searches for pair production of H++ H--, with H+-+- --> lepton+- lepton+- (lepton,lepton^' = e,mu,tau).  The limit holds for lepton=lepton^'=tau, and becomes stronger for other combinations of leptonic final states. To ensure the decay within the detector, the limit only applies for g(H lepton lepton)~>10**-7.


pdgid: S064HD1
text:
AAD 2024AD search for production of H+-+- by W+- W+- fusion, in the decay to W+- W+-, using  139 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 12 for limits on cross  section times branching ratio for mass(H+-+-) between 0.2 and 3.0 TeV.  Limits on the iso-triplet  contribution to the gauge-boson masses in the Georgi-Machacek model are also shown.


pdgid: S064HD1
text:
AAD 2021U search for pair production of H++ H-- followed by the decay H+-+- --> W+- W+- in 139   fb**-1 of p p collisions at Ecm = 13 TeV. The search is interpreted in a  triplet  extension of the SM Higgs sector with a triplet vev of 0.1 GeV, leading to B(H+-+- --> W+- W+-) =  1.  See their Fig. 9(a) for limits on the cross section for mass(H++) between 200 and 600 GeV.


pdgid: S064HD1
text:
AAD 2021U search for associated production of H+-+- H-+ followed by the decays H+-+- --> W+- W+-, H+- --> W+- Z   in 139 fb**-1 of p p collisions at Ecm = 13 TeV. H+-+- and H+- are assumed  to  be degenerate in mass within 5 GeV.  The search is interpreted in a triplet extension of the SM  Higgs sector with a triplet vev of 0.1 GeV, leading to B(H+-+- --> W+- W+-) = 1.  See their  Fig. 9(b) for limits on the cross section for mass(H++) between 200 and 600 GeV.


pdgid: S064HD1
text:
SIRUNYAN 2021W search for vector boson fusion production of H+-+- decaying to H+-+- --> W+- W+- --> lepton+- nu lepton+- nu  in 137 fb**-1 of p p collisions at Ecm = 13 TeV. See their Fig. 8 for limits on cross  section times branching ratio for mass(H++) = 0.2 -- 3.0 TeV.


pdgid: S064HD1
text:
SIRUNYAN 2019CQ search for H+-+- production by vector boson fusion followed by the decay  H+-+- --> W+- W+- --> q q lepton nu in 35.9 fb**-1 of p p collisions at Ecm = 13  TeV. See their Fig. 5 for limits on cross section times branching ratio for mass(H+-+-) between  0.6 and 2 TeV.


pdgid: S064HD1
text:
SIRUNYAN 2018CC search for H+-+- production by vector boson fusion followed by the decay  H+-+- --> W+- W+- in 35.9 fb**-1 of p p collisions at Ecm = 13 TeV. See their  Fig. 3 for limits on cross section times branching ratio for mass(H+-+-) between 200 and 1000 GeV.


pdgid: S064HD1
text:
KANEMURA 2015 examine the case where H++ decays preferentially to W^(*)() W^(*)() and   estimate that a lower mass limit of ~84 GeV can be derived from the same-sign dilepton data   of AAD 2015AG if H++ decays with 100% branching ratio to W^(*)() W^(*)().


pdgid: S064HD1
text:
KHACHATRYAN 2015D search for H+-+- production by vector boson fusion followed by the  decay  H+-+- --> W+- W+- in 19.4 fb**-1 of p p collisions at Ecm = 8 TeV.  See  their  Fig. 4 for limits on cross section times branching ratio for mass(H++) between 160 and 800  GeV.


pdgid: S064HD1
text:
KANEMURA 2014 examine the case where H++ decays preferentially to W^(*)() W^(*)() and estimate that a lower mass limit of ~60 GeV can be derived from the same-sign dilepton data of AAD 2012CY.


pdgid: S064HD1
text:
AAD 2013Y search for H()++ H()-- production in a generic search of events with three charged leptons in 4.6 fb**-1 of p p collisions at Ecm = 7 TeV. The limit assumes 100% branching ratio to the specified final state.


pdgid: S064HD1
text:
AAD 2012AY search for H()++ H()-- production with 1.6 fb**-1 of p p collisions at Ecm = 7 TeV. The limit assumes 100% branching ratio to the specified final state.


pdgid: S064HD1
text:
AAD 2012CQ search for H()++ H()-- production with 4.7 fb**-1 of p p collisions at Ecm = 7 TeV. The limit assumes 100% branching ratio to the specified final state. See their Table 1 for limits assuming smaller branching ratios.


pdgid: S064HD1
text:
ABAZOV 2012A search for H()++ H()-- production in 7.0 fb**-1 of p pbar collisions at Ecm = 1.96 TeV.


pdgid: S064HD1
text:
AALTONEN 2011AF search for H()++ H()-- production in 6.1 fb**-1 of p pbar collisions at Ecm = 1.96 TeV.


pdgid: S064HD1
text:
AALTONEN 2008AA search for H^++() H^--() production in p pbar collisions at Ecm= 1.96 TeV. The limit assumes 100% branching ratio to the specified final state.


pdgid: S064HD1
text:
ABAZOV 2008V search for H^++() H^--() production in p pbar collisions at Ecm= 1.96 TeV. The limit is for B(H --> mu mu) = 1. The limit is updated in ABAZOV 2012A.


pdgid: S064HD1
text:
AKTAS 2006A search for single H+-+- production in e p collisions at HERA. Assuming that H++  only couples to e+ mu+ with g(e mu) = 0.3 (electromagnetic strength), a limit mass(H++) > 141 GeV (95% CL) is derived.  For the case where H++ couples to e tau only the limit is 112 GeV.


pdgid: S064HD1
text:
ACOSTA 2005L search for H^++() H^--() pair production in p pbar collisions. The limit is valid for g(lepton lepton^'()) < 10**-8 so that the Higgs decays outside the detector.


pdgid: S064HD1
text:
ABAZOV 2004E search for H++ H-- pair production in H+-+- --> mu+- mu+-. The limit is valid for g(mu mu) ~> 10**-7.


pdgid: S064HD1
text:
ABBIENDI 2003Q searches for single H+-+- via  direct production in e+ e- --> e-+ e-+ H+-+-, and via t-channel exchange in e+ e- --> e+ e-. In the direct case, and assuming B( H+-+- --> lepton+- lepton+-) = 1, a 95% CL limit on h(ee) < 0.071 is set for mass( H+-+-) < 160 GeV (see Fig. 6). In the second case, indirect limits on h(ee) are set for mass( H+-+-) < 2 TeV (see Fig. 8).


pdgid: S064HD1
text:
GORDEEV 1997 search for muonium-antimuonium conversion and find G(M Mbar)/G(F)<0.14 (90% CL), where G(M Mbar) is the lepton-flavor violating effective four-fermion coupling.  This limit may be converted to mass(H++)>210 GeV if the Yukawa couplings of H++ to ee and mu mu are as large as the weak gauge coupling. For similar limits on muonium-antimuonium conversion, see the muon Particle Listings.


pdgid: S064HD1
text:
ASAKA 1995 point out that H++ decays dominantly to four fermions in a large region of parameter space where the limit of ACTON 1992M from the search of dilepton modes does not apply.


pdgid: S064HD1
text:
ACTON 1992M limit assumes H+-+- --> lepton+- lepton+- or H+-+- does not decay in the detector.  Thus the region g(lepton lepton)~~10**-7 is not excluded.


pdgid: S064HD1
text:
SWARTZ 1990 assume H+-+- --> lepton+- lepton+- (any flavor). The limits are valid for the Higgs-lepton coupling g(H lepton lepton) ~> 7.4E-7/[mass(H)/GeV]**1/2. The limits improve somewhat for e e and mu mu decay modes.


pdgid: S064HD0
text:
AAD 2023AI search for H++ H-- production using 139 fb**-1 of p p collisions at    Ecm = 13 TeV.  Decay branching ratios B(H++ --> lepton+ lepton^'+) for the six flavor   combinations are assumed to be equal, adding up to unity.


pdgid: S064HD0
text:
ACHARD 2003F search for e+ e- --> H++ H-- with H+-+- --> lepton+- lepton^'()+-. The limit holds for lepton = lepton^' = tau, and slightly different limits apply for other flavor combinations. The limit is valid for g(lepton lepton^') ~> 10**-7.


pdgid: S064HD0
text:
ABBIENDI 2002C searches for pair production of H++ H--, with H+-+- --> lepton+- lepton+- (lepton,lepton^' = e,mu,tau).  the limit holds for lepton=lepton^'=tau, and becomes stronger for other combinations of leptonic final states. To ensure the decay within the detector, the limit only applies for g(H lepton lepton)~>10**-7.


pdgid: S056W1C
text:
AAD 2024T limit is for W^' with SM-like coupling from p p collisions at sqrt(s) =1 3  TeV. Bosonic decays of W^' and W-W^' interference are neglected. See their Fig.  7a for limits on .


pdgid: S056W1C
text:
HAYRAPETYAN 2024X search for right-handed W^' decaying to t b in p p collisions  at sqrt(s) = 13 TeV. See their Fig. 7 for limits on .


pdgid: S056W1C
text:
AAD 2023AH search for resonances produced through Drell-Yan and vector-boson-fusion processes  in p p collisions at sqrt(s) = 13 TeV. See their Fig. 7 and Fig. 8 for limits on .    The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3 produced mainly via Drell-Yan.


pdgid: S056W1C
text:
AAD 2023CC search for resonances decaying to t b in p p collisions at sqrt(s) = 13  TeV. The limit quoted above is for right-handed W^' assuming a W^' coupling equal to the SM  W coupling. The limit becomes M(W^') > 4200 GeV for left-handed W^'. See  their Figs. 12 and 13 for limits on .


pdgid: S056W1C
text:
AAD 2023L perform a generic search for resonances with events containing a Z decaying   into e+ e- or mu+ mu- in p p collisions at sqrt(s) = 13 TeV. See their Figs. 6, 7, 8   for model independent limits on  for Gaussian-shaped resonances. The limit above is for   heavy-vector-triplet W^' decaying to W Z with g_{{V}} = 3 as well as with g_{{V}} = 1.


pdgid: S056W1C
text:
AAD 2023O search for resonances decaying to H W in p p collisions at sqrt(s) = 13  TeV. The  quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 2950 GeV for g_{{V}} = 1.


pdgid: S056W1C
text:
TUMASYAN 2023AP search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The  limit  becomes M(W^') > 4.8 TeV assuming M(W^') = M(Z^') and  combining W^' --> W Z, W^' --> W H, Z^' --> W W, Z^' --> Z H channels.


pdgid: S056W1C
text:
TUMASYAN 2023AP search for resonances decaying to W H in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit  becomes M(W^') > 4.8 TeV assuming M(W^') = M(Z^') and  combining W^' --> W Z, W^' --> W H, Z^' --> W W, Z^' --> Z H channels.


pdgid: S056W1C
text:
TUMASYAN 2023AW search for SSM W^' resonance decaying to tau nu in p p collisions  at sqrt(s) = 13 TeV. W-W^' intereference and bosonic decays of W^' are not  included. See their Fig. 6 for limits on .


pdgid: S056W1C
text:
TUMASYAN 2022AC search for W^' with SM-like couplings in p p collisions at sqrt(s) =  13 TeV. The diboson decays of W^' are assumed to be suppressed. See their Fig. 5 for limits on  .


pdgid: S056W1C
text:
TUMASYAN 2022D search for resonances produced through Drell-Yan and vector-boson-fusion processes  in p p collisions at sqrt(s) = 13 TeV. See their Fig. 8 for limits on . The quoted  limit is for heavy-vector-triplet W^' with g_{{V}} = 3 produced mainly via Drell-Yan.


pdgid: S056W1C
text:
TUMASYAN 2022J search for resonances produced through Drell-Yan and vector-boson-fusion processes  in p p collisions at sqrt(s) = 13 TeV. The quoted limit is for heavy-vector-triplet W^'  with g_{{V}} = 3, produced mainly via Drell-Yan. See their Fig. 9 for limits on .


pdgid: S056W1C
text:
TUMASYAN 2022R search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet W^' produced mainly via Drell-Yan. See  their Fig. 8 for limits on .


pdgid: S056W1C
text:
SIRUNYAN 2021Y search for resonances decaying to t b in p p collisions at sqrt(s) =  13 TeV. See  their Fig. 2 for limits on sigma. B(W^' --> t b).


pdgid: S056W1C
text:
AAD 2020AJ search for resonances decaying to H W in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 2900 GeV for g_{{V}} = 1. See their Fig. 6 for limits on .


pdgid: S056W1C
text:
AAD 2020AT search for resonances decaying to W Z in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 3900 GeV for g_{{V}} = 1. See their Fig. 13 for limits on .


pdgid: S056W1C
text:
AAD 2020T search for W^' with SM-like couplings in p p collisions at sqrt(s) = 13  TeV. See their Fig. 4(c) for limits on the product of the cross section, acceptance, and branching  fraction.


pdgid: S056W1C
text:
SIRUNYAN 2020Q search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3.


pdgid: S056W1C
text:
AABOUD 2019E search for right-handed W^' in p p collisions at sqrt(s) = 13 TeV. See  their Fig. 8 for limit on on sigma.B.


pdgid: S056W1C
text:
AAD 2019C search for W^' with SM-like couplings in p p collisions at sqrt(s) = 13  TeV. Bosonic decays and W-W^' interference are neglected. The limits on e and  mu separately are 6.0 and 5.1 TeV respectively.  See their Fig. 2 for limits on .


pdgid: S056W1C
text:
AAD 2019D search for resonances decaying to W Z in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 3400 GeV for g_{{V}} = 1. If we assume M(W^') =  M(Z^'), the limit increases M(W^') > 3800 GeV and  M(W^') > 3500 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their  Fig. 9 for limits on .


pdgid: S056W1C
text:
SIRUNYAN 2019AY limits shown for W^' with SM-like coupling using p p collisions at  sqrt(s) = 13 TeV. W-W^' interference and bosonic decays of W^' are not included.  See their Fig. 5 for limits on sigma.B. Limits in the context of a  nonuniversal gauge interaction are shown in Fig. 7. Model independent limits on sigma B A epsilon can be  seen in Fig. 8.


pdgid: S056W1C
text:
SIRUNYAN 2019CP present a statistical combinations of searches for W^' decaying to pairs  of bosons or leptons in p p collisions at sqrt(s) = 13 TeV. The quoted limit is for  heavy-vector-triplet W^' with g_{{V}} = 3. If we assume M(W^') =  M(Z^'), the limit becomes M(W^') > 4500 GeV for g_{{V}} = 3 and  M(W^') > 5000 GeV for g_{{V}} = 1. See their Figs. 2 and 3 for limits on  .


pdgid: S056W1C
text:
SIRUNYAN 2019I search for resonances decaying to H W in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 2800 GeV if we assume M(W^') =  M(Z^').


pdgid: S056W1C
text:
AABOUD 2018AF give the limit above for right-handed W^' using p p collisions at  sqrt(s) = 13 TeV. These limits also exclude W bosons with left-handed couplings with masses  below 2.9 TeV, at the 95% confidence level. W^' --> lepton nu_R is assumed to be  forbidden. See their Fig.5 for limits on sigma.B for both cases of left- and  right-handed W^'.


pdgid: S056W1C
text:
AABOUD 2018AI search for resonances decaying to H W in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 2670 GeV for g_{{V}} = 1. If we assume M(W^') =  M(Z^'), the limit increases M(W^') > 2930 GeV and  M(W^') > 2800 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their  Fig. 5 for limits on sigma.B.


pdgid: S056W1C
text:
AABOUD 2018AK search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit  becomes M(W^') > 2800 GeV for g_{{V}} = 1.


pdgid: S056W1C
text:
AABOUD 2018AL search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit  becomes M(W^') > 2900 GeV for g_{{V}} = 1.


pdgid: S056W1C
text:
AABOUD 2018BG limit is for W^' with SM-like couplings using p p collisions at  sqrt(s) = 13 TeV. Bosonic decays of W^' and W-W^' interference are neglected.  See Fig. 2 for limits on sigma.B.


pdgid: S056W1C
text:
AABOUD 2018CH search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit  becomes M(W^') > 2260 GeV for g_{{V}} = 1.


pdgid: S056W1C
text:
AABOUD 2018F search for resonances decaying to W Z in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 3000 GeV for g_{{V}} = 1. If we assume M(Z^') =  M(W^'), the limit increases M(W^') > 3500 GeV and  M(W^') > 3100 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their  Fig.5 for limits on sigma.B.


pdgid: S056W1C
text:
AABOUD 2018K limit is for W^' with SM-like coupling using p p collisions at sqrt(s)  = 13 TeV. W-W^' interference and bosonic decays of W^' are not included. See  their Fig. 4 for limit on sigma.B.


pdgid: S056W1C
text:
SIRUNYAN 2018 limit is for right-handed W^' using  $pp$ collisions at sqrt(s) = 13 TeV.  W^' --> lepton nu_R decay is assumed to be forbidden. The limit becomes M(W^')  > 3.4 TeV  if M(nu_{{R}}) << M(W^'). See their Fig. 5 for  exclusion limits on W^' models  having both left- and right-handed couplings.


pdgid: S056W1C
text:
SIRUNYAN 2018AX search for resonances decaying to W Z in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. See their Fig.6 for  limits on sigma.B.


pdgid: S056W1C
text:
SIRUNYAN 2018AZ limit is derived for W^' with SM-like coupling using p p collisions  at sqrt(s) = 13 TeV. No interference with SM W process is considered. The bosonic decays are  assumed to be negligible. See their Fig.6 for limits on .


pdgid: S056W1C
text:
SIRUNYAN 2018BK search for resonances decaying to W Z  in p p collisions at sqrt(s)  = 13 TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit  becomes M(W^')> 3100 GeV for g_{{V}} = 1.


pdgid: S056W1C
text:
SIRUNYAN 2018DJ search for resonances decaying to $WZ$ in p p collisions at sqrt(s) = 13  TeV. The limit quoted above is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes  M(W^') > 2270 GeV for g_{{V}} = 1.


pdgid: S056W1C
text:
SIRUNYAN 2018ED search for resonances decaying to H W in p p collisions at sqrt(s) =  13 TeV. The limit above is for heavy-vector-triplet W^' with g_{{V}} = 3. If we assume  M(W^') = M(Z^'), the limit increases M(W^')  > 2900 GeV and M(W^') > 2800 GeV for g_{{V}} = 3 and g_{{V}} = 1,  respectively.


pdgid: S056W1C
text:
SIRUNYAN 2018P give this limit for a heavy-vector-triplet W^' with g_{{V}} = 3. If they  assume M(Z^') = M(W^'), the limit increases to  M(W^') > 3800 GeV.


pdgid: S056W1C
text:
AABOUD 2017AK search for a new resonance decaying to dijets in p p collisions at sqrt(s)  = 13 TeV. The limit above is for a W^' boson having axial-vector SM couplings and decaying to  quarks with 75% branching fraction.


pdgid: S056W1C
text:
AABOUD 2017AO search for resonances decaying to H W in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for a W^' in the  heavy-vector-triplet model with g_{{V}} =  3. See their Fig.4 for limits on sigma.B.


pdgid: S056W1C
text:
AABOUD 2017B search for resonances decaying to H W (H --> b bbar, c cbar; W --> lepton nu) in  p p collisions at sqrt(s) = 13 TeV. The quoted limit is for heavy-vector-triplet W^' with  g_{{V}} = 3. The limit becomes M(W^') > 1750 GeV for g_{{V}} = 1. If we assume  M(W^') = M(Z^'), the limit increases M(W^')> 2310 GeV and  M(W^')> 1730 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their Fig.3  for limits on sigma.B.


pdgid: S056W1C
text:
KHACHATRYAN 2017J search for right-handed W_{{R}} in p p collisions at sqrt(s) = 13 TeV.  W_{{R}} is assumed to decay into tau and hypothetical heavy neutrino N_{{tau}}, with N_{{tau}}  decaying into tau j j. The quoted limit is for M(N_{{tau}}) =  M(W_{{R}})/2. The limit becomes M(W_{{R}}) > 2350 GeV (1630 GeV)  for M(W_{{R}})/M(N_{{tau}}) = 0.8 (0.2). See their Fig. 4 for excluded  regions in the M(W_{{R}})-M(N_{{tau}}) plane.


pdgid: S056W1C
text:
KHACHATRYAN 2017Z limit is for W^' with SM-like coupling using p p collisions at  sqrt(s) = 13 TeV.  The bosonic decays of W^' and the interference with SM W process are  neglected.


pdgid: S056W1C
text:
SIRUNYAN 2017A search for resonances decaying to W Z with W Z --> lepton nu q qbar,  q qbar q qbar in p p collisions at sqrt(s) = 13 TeV. The quoted limit is for  heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes M(W^') >  2000 GeV for g_{{V}} = 1. If we assume M(Z^') = M(W^'), the limit  increases M(W^') > 2400 GeV and M(W^') > 2300 GeV for  g_{{V}} = 3 and g_{{V}} = 1, respectively. See their Fig.6 for limits on  sigma.B.


pdgid: S056W1C
text:
SIRUNYAN 2017AK search for resonances decaying to W Z or H W in p p collisions at  sqrt(s) = 8 and 13 TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. The limit becomes M(W^') > 2300 GeV for g_{{V}} = 1. If we assume  M(W^') = M(Z^'), the limit increases M(W^')  > 2400 GeV for both g_{{V}} = 3 and g_{{V}} = 1. See their Fig.1 and 2 for limits on  sigma.B.


pdgid: S056W1C
text:
SIRUNYAN 2017H search for right-handed W^' in p p collisions at sqrt(s) = 13 TeV.  W^' is assumed to decay into tau and a heavy neutrino N, with N decaying to tau q qbar.  The limit above assumes M(N) = M(W^')/2.


pdgid: S056W1C
text:
SIRUNYAN 2017I limit is for a right-handed W^' using p p collisions at sqrt(s) = 13  TeV. The limit becomes M(W^') > 2400 GeV for M(nu_{{R}}) <<  M(W^').


pdgid: S056W1C
text:
SIRUNYAN 2017R search for resonances decaying to H W in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. Mass regions  M(W^') < 2370 GeV and 2870 < M(W^') < 2970 GeV  are excluded for g_{{V}} = 1. If we assume M(Z^') = M(W^'), the  excluded mass regions are 1000 < M(W^') < 2500 GeV and 2760 <  M(W^') < 3300 GeV for g_{{V}} = 3; 1000 < M(W^')  < 2430 GeV and 2810 < M(W^') < 3130 GeV for g_{{V}} = 1. See  their Fig.5 for limits on sigma.B.


pdgid: S056W1C
text:
AABOUD 2016AE search for resonances decaying to V V (V = W or Z) in p p  collisions at sqrt(s) = 13 TeV. Results from nu nu q q, nu lepton q q, lepton lepton q q and  q q q q final states are combined. The quoted limit is for a heavy-vector-triplet W^' with  g_{{V}} = 3 and M(W^') = M(Z^').


pdgid: S056W1C
text:
AABOUD 2016V limit is for W^' with SM-like coupling using p p collisions at sqrt(s)  = 13 TeV. The bosonic decays of W^' and the interference with SM W process are neglected.


pdgid: S056W1C
text:
AAD 2016R search for W^' --> W Z in p p collisions at sqrt(s) = 8 TeV. lepton nu lepton^' lepton^',  lepton lepton q qbar, lepton nu q qbar, and all hadronic channels are combined. The quoted  limit assumes g(W^' W Z)/g(W W Z) = (M_{{W}}/M(W^'))**2.


pdgid: S056W1C
text:
AAD 2016S search for a new resonance decaying to dijets in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for a W^' having SM-like  couplings to quarks.


pdgid: S056W1C
text:
KHACHATRYAN 2016AO limit is for a SM-like right-handed  using p p collisions at  sqrt(s) = 8 TeV. The quoted limit combines t --> q q b and t --> lepton nu b events.


pdgid: S056W1C
text:
KHACHATRYAN 2016AP search for a resonance decaying to H W in p p collisions at  sqrt(s) = 8 TeV. Both H and W are assumed to decay to fat jets. The quoted limit is for  heavy-vector-triplet W^' with g_{{V}} = 3.


pdgid: S056W1C
text:
KHACHATRYAN 2016BD search for resonance decaying to H W in p p collisions at sqrt(s)  = 8 TeV. The quoted limit is for heavy-vector-triplet (HVT) W^' with g_{{V}} = 3. The HVT model  mass(W^') = mass(Z^') > 1.8 TeV is also obtained by combining W^'/Z^' --> W H/Z H --> lepton nu b b, q q tau tau,  q q b b, and q q q q q q channels.


pdgid: S056W1C
text:
KHACHATRYAN 2016L search for resonances decaying to dijets in p p collisions at sqrt(s)  = 8 TeV with the data scouting technique, increasing the sensitivity to the low mass resonances.


pdgid: S056W1C
text:
KHACHATRYAN 2016O limit is for W^' having universal couplings. Interferences with the SM  amplitudes are assumed to be absent.


pdgid: S056W1C
text:
AAD 2015AU search for W^' decaying into the W Z final state with W --> q qbar^', Z --> lepton+ lepton- using p p collisions at sqrt(s) = 8 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2.


pdgid: S056W1C
text:
AAD 2015AV limit is for a SM like right-handed W^' using p p collisions at sqrt(s) = 8 TeV. W^' --> lepton nu decay is assumed to be  forbidden.


pdgid: S056W1C
text:
AAD 2015AZ search for W^' decaying into the W Z final state with W --> lepton nu, Z --> q qbar using p p collisions at sqrt(s) = 8 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2.


pdgid: S056W1C
text:
AAD 2015CP search for W^' decaying into the W Z final state with W --> q qbar, Z --> q qbar using p p collisions at sqrt(s) = 8 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2.


pdgid: S056W1C
text:
AAD 2015R limit is for a SM like right-handed W^' using p p collisions at sqrt(s) = 8 TeV. W^' --> lepton nu decay is assumed to be forbidden.


pdgid: S056W1C
text:
KHACHATRYAN 2015C search for W^' decaying via W Z to  fully leptonic final states using p p collisions at sqrt(s)=8 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = M(W) M(Z)/M(W^')**2.


pdgid: S056W1C
text:
KHACHATRYAN 2015T limit is for W^' with SM-like coupling which interferes the SM W boson  constructively using p p collisions at sqrt(s) = 8 TeV. For W^' without interference, the limit becomes > 3280 GeV.


pdgid: S056W1C
text:
KHACHATRYAN 2014O search for right-handed W_{{R}} in p p collisions at sqrt(s) = 8 TeV. W_{{R}} is assumed to decay  into lepton and hypothetical heavy neutrino N, with N decaying into lepton j  j. The quoted limit  is for M(nu_{{eR}}) = M(nu(mu R)) = M(W_{{R}})/2. See their Fig. 3 and Fig. 5 for excluded regions in the M(W_{{R}})-M(nu) plane.


pdgid: S056W1C
text:
AAD 2024AE search for resonances decaying to q q, t t, t b, V V, V H,  lepton lepton, lepton tau, tau nu, tau tau in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3. M(W^')  = M(Z^') is assumed. The limit becomes M(W^') > 5.8 TeV for  g_{{V}} = 1.


pdgid: S056W1C
text:
AAD 2024CM search for pair productions of dark pions pi_D()+- pi_D()0 in t t b b  events of p p collisions at sqrt(s) = 13 TeV. pi_D()+- --> t b and pi_D()0 --> t t  decays are assumed. The production cross section is computed in a model with dark rho_{{D}}()+-  assuming dark isospin symmetry mass(rho_{{D}}()+-) = mass(rho_{{D}}()0), mass(pi_{{D}}()+-) =  mass(pi_{{D}}()0). See their Fig. 12 for limits on the production cross sections.


pdgid: S056W1C
text:
HAYRAPETYAN 2024AV search for a spin-0 particle X decaying to W gamma in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 8 for limits on .


pdgid: S056W1C
text:
AAD 2023BF search for W^' decaying to W Z^' in p p collisions at sqrt(s) = 13  TeV. The mass difference between W^' and Z^' is assumed to be 250 GeV. See their Fig. 9(a)  for limits on  as a function of M(W^').


pdgid: S056W1C
text:
AAD 2023CG search for right-handed W_{{R}} in p p collisions at sqrt(s) = 13 TeV.  W_{{R}} is assumed to decay into lepton and hypothetical heavy neutrino N, with N  decaying into lepton j j. See their Fig. 9 for limits in mass(N)-mass(W_{{R}}) plane.


pdgid: S056W1C
text:
AAD 2023CK search for a new resonance decaying to H X (H --> b bbar, X --> q qbar^') in  p p collisions at sqrt(s) = 13 TeV. See their Fig. 12 for limits on .


pdgid: S056W1C
text:
AAD 2023U search for a narrow charged vector boson decaying to W gamma. See their Fig.  8(d) for the exclusion limit in mass(W^')- plane.


pdgid: S056W1C
text:
TUMASYAN 2022 search for KK excited W decaying in cascade to three W via a scalar  radion R. See their Fig. 4 for limits in M(W^')-M_{{R}} plane.


pdgid: S056W1C
text:
TUMASYAN 2022AL search for resonances decaying to t B or b T with vector-like quarks  B (T) subsequently decaying to b H or b Z (t H or t Z). See their Fig. 7  for limits on .


pdgid: S056W1C
text:
TUMASYAN 2022B search for a narrow charged vector boson decaying to W gamma. See their  Fig. 5 for limits on .


pdgid: S056W1C
text:
TUMASYAN 2022I search for KK excited W decaying in cascade to three W via a scalar   radion R. See their Fig. 10 for limits in M(W^')-M_{{R}} plane.


pdgid: S056W1C
text:
TUMASYAN 2022P search for right handed W_{{R}} in p p collisiions at sqrt(s) = 13 TeV.  W_{{R}} is  assumed to decay into lepton and hypothetical heavy neutrino N, with N  decaying to lepton j j. See their Fig. 7 for excluded regions in  M(W_{{R}})-M_{{N}} plane.


pdgid: S056W1C
text:
AAD 2020AD search for a narrow resonance decaying to a pair of large-radius-jets J_{{1}} and  J_{{2}} employing a machine-learning procedure. See their Fig. 3 for limits on  depending  on assumptions about invariant masses for J_{{1}}, J_{{2}}, and J_1 J_2.


pdgid: S056W1C
text:
AAD 2020W search for W^' decaying to W Z^' in p p collisions at sqrt(s) = 13 TeV.  See their Fig. 5(b) for limits on  as a function of mass(Z^'). The W^' --> W Z^'  branching fraction was chosen to be 0.5 and the mass difference between the W^' and Z^' was  set to 250 GeV.


pdgid: S056W1C
text:
AABOUD 2019B search for right-handed W_{{R}} in p p collisions at sqrt(s) = 13 TeV.  W_{{R}} is assumed to decay into lepton and hypothetical heavy neutrino N, with N  decaying to lepton j j. See their Figs. 7 and 8 for excluded regions in M(W_{{R}})  - M_{{N}} plane.


pdgid: S056W1C
text:
AABOUD 2019BB search for right handed W_{{R}} in p p collisions at sqrt(s) = 13 TeV.  W_{{R}} is assumed to decay into lepton and a boosted hypothetical heavy neutrino N, with  N decaying to lepton and a large radius jet j = q qbar. See their Fig. 7 for  excluded regions in M(W_{{R}})-M_{{N}} plane.


pdgid: S056W1C
text:
SIRUNYAN 2019V search for a new resonance decaying to a top quark and a heavy vector-like  bottom partner B decaying to H b (or a bottom quark and a heavy vector-like top partner  T decaying to H t) in p p collisions at sqrt(s) = 13 TeV. See their Fig. 8 for limits  on sigma.B.


pdgid: S056W1C
text:
AABOUD 2018AA search for a narrow charged vector boson decaying to W gamma. See their  Fig. 9 for the exclusion limit in M(W^') - sigmaB plane.


pdgid: S056W1C
text:
AABOUD 2018AD search for resonances decaying to H X (H --> b bbar, X --> q qbar^') in p p  collisions  at sqrt(s) = 13 TeV. See their Figs. 3 -- 5 for limits on  sigma.B.


pdgid: S056W1C
text:
AABOUD 2018CJ search for heavy-vector-triplet W^' in p p collisions at sqrt(s) = 13  TeV. The limit quoted above is for model with g_{{V}} = 3 assuming M(W^') =  M(Z^'). The limit becomes M(W^') > 5500 GeV for model with  g_{{V}} = 1.


pdgid: S056W1C
text:
SIRUNYAN 2018CV search for right-handed W_{{R}} in p p collisions at sqrt(s) = 13 TeV.  W_{{R}} is assumed to decay into lepton and hypothetical heavy neutrino N, with N  decaying to lepton j j. The quoted limit is for M_{{N}} = M(W_{{R}})/2. See their Fig.  6 for excluded regions in the M(W_{{R}})-M_{{N}} plane.


pdgid: S056W1C
text:
KHACHATRYAN 2017U search for resonances decaying to H W (H --> b bbar; W --> lepton nu) in  p p collisions at sqrt(s) = 13 TeV. The limit on the heavy-vector-triplet model is  M(Z^') = M(W^') > 2 TeV for g_{{V}} = 3, in which  constraints from the Z^' --> H Z (H --> b bbar; Z --> lepton+ lepton-, nu nubar)  are combined. See their Fig.3 and Fig.4 for limits on sigma.B.


pdgid: S056W1C
text:
AAD 2015BB search for W^' decaying into W H with W --> lepton nu, H --> b bbar. See their Fig. 4 for the exclusion limits in the heavy vector triplet benchmark model parameter space.


pdgid: S056W1C
text:
AALTONEN 2015C limit is for a SM-like right-handed W^' assuming W^' --> lepton nu decays are forbidden, using p pbar collisions at sqrt(s)=1.96 TeV. See their Fig. 3 for limit on g(W^')/g(W).


pdgid: S056W1C
text:
AAD 2014AT search for a narrow charged vector boson decaying to W gamma. See their Fig. 3a for the exclusion limit in mass(W^')-sigmaB plane.


pdgid: S056W1C
text:
using p p collisions at sqrt(s)=8 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2.


pdgid: S056W1C
text:
KHACHATRYAN 2014 search for W^' decaying into W Z final state with W --> q qbar, Z --> q qbar The quoted limit assumes g(W^' W Z)/g(W W Z) = (M_{{W}}/M(W^'))**2.


pdgid: S056W1C
text:
KHACHATRYAN 2014A search for W^' decaying into the W Z final state with W --> lepton nu, Z --> q qbar, or W --> q qbar, Z --> lepton lepton. p p collisions data at sqrt(s)=8 TeV are used for the search. See their Fig. 13 for the exclusion limit on the number of events in  the mass-width plane.


pdgid: S056W1C
text:
CHATRCHYAN 2013AJ search for resonances decaying to W Z pair, using the hadronic decay modes of W and Z, in p p collisions at sqrt(s)=7 TeV. See their Fig. 7 for the limit on the cross section.


pdgid: S056W1C
text:
CHATRCHYAN 2013E limit is for W^' with SM-like coupling which  intereferes with the SM W boson using p p collisions at sqrt(s)=7 TeV. For W^' with right-handed coupling, the bound becomes >1850 GeV (>1910 GeV) if W^' decays to both leptons and quarks (only to quarks).  If both left- and right-handed couplings are present,  the limit becomes >1640 GeV.


pdgid: S056W1C
text:
CHATRCHYAN 2013U search for W^' decaying to the W Z final state, with W decaying into jets, in p p collisions at sqrt(s)=7 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2.


pdgid: S056W1C
text:
The AAD 2012AV quoted limit is for a SM-like right-handed W^' using p p collisions at sqrt(s)=7 TeV. W^' --> lepton nu decay is assumed to be forbidden.


pdgid: S056W1C
text:
AAD 2012BB use p p collisions data at sqrt(s)=7 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2.


pdgid: S056W1C
text:
AAD 2012CK  search for p p --> t W^', W^' --> tbar q events in p p collisions.  See their Fig. 5 for the limit on sigma.B.


pdgid: S056W1C
text:
AAD 2012M search for right-handed W_{{R}} in p p collisions at sqrt(s) = 7 TeV. W_{{R}} is assumed to decay into lepton and hypothetical heavy neutrino N, with N decaying into lepton j j. See their Fig. 4 for the limit in the mass(N)-mass(W^') plane.


pdgid: S056W1C
text:
AALTONEN 2012N search for p pbar --> t W^', W^' --> tbar d events in p pbar collisions. See their Fig. 3 for the limit on sigma.B.


pdgid: S056W1C
text:
CHATRCHYAN 2012AR search for p p --> t W^', W^' --> tbar d events in p p collisions. See their Fig. 2 for the limit on sigma.B.


pdgid: S056W1C
text:
CHATRCHYAN 2012BG search for right-handed W_{{R}} in  collisions sqrt(s) = 7 TeV. W_{{R}} is assumed to decay into lepton and hypothetical heavy neutrino N, with N decaying into lepton j j. See their Fig. 3 for the limit in the mass(N)-mass(W^') plane.


pdgid: S056W1C
text:
ABAZOV 2011H use data from p pbar collisions at sqrt(s)=1.96 TeV. The quoted limit is obtained assuming W^' W Z coupling strength is the same as the ordinary W W Z coupling strength in the Standard Model.


pdgid: S056W1C
text:
ABAZOV 2011L limit is for W^' with SM-like coupling which interferes  with the SM W boson, using p pbar collisions at sqrt(s)=1.96 TeV.  For W^' with right-handed coupling, the bound becomes >885 GeV (>890 GeV) if W^' decays to  both leptons and quarks (only to quarks). If both left- and right-handed couplings present, the  limit becomes >916 GeV.


pdgid: S056W1C
text:
AALTONEN 2010N use p pbar collision data at sqrt(s)=1.96 TeV. The quoted limit assumes g(W^' W Z)/g(W W Z) = (M(W)/M(W^'))**2. See their Fig.4 for limits in mass-coupling plane.


pdgid: S056W1C
text:
AALTONEN 2009AC search for new particle decaying to dijets using p pbar collisions at sqrt(s)=1.96 TeV.


pdgid: S056W1C
text:
The ACOSTA 2003B  quoted limit is for M(W^')>>M(nu_{{R}}), using p pbar collisions at sqrt(s)=1.8 TeV. For M(W^')<M(nu_{{R}}), M(W^') between 225 and 566 GeV is excluded.


pdgid: S056W1C
text:
AFFOLDER 2001I combine a new bound on W^' --> e nu of 754 GeV, using p pbar collisions at sqrt(s)=1.8 TeV, with the bound of ABE 2000 on W^' --> mu nu to obtain quoted bound.


pdgid: S056W1C
text:
ABACHI 1995E assume that the decay W^' --> W Z is suppressed and that the neutrino from W^' decay is stable and has a mass significantly less mass(W^').


pdgid: S056W1C
text:
RIZZO 1993 analyses CDF limit on possible two-jet resonances.  The limit is sensitive to the inclusion of the assumed K factor.


pdgid: S056MR
text:
ALVES 2024 limit quoted above is from B(pi --> e nu)/B(pi --> mu nu) assuming  mass(nu_{{R}}) = 50 MeV in vanishing W_{{L}}-W_{{R}} mixing limit. g_{{L}} = g_{{R}} is assumed.  See their Fig. 2 for limits in mass(nu_{{R}})-mass(W_{{R}}) plane.


pdgid: S056MR
text:
PRIEELS 2014 limit is from mu+ --> e+ nu nubar decay  parameter xi^'', which is determined by the positron polarization measurement.


pdgid: S056MR
text:
WAUTERS 2010 limit is from a measurement of the asymmetry parameter of polarized Co60 beta decays. The listed limit assumes no mixing.


pdgid: S056MR
text:
ZHANG 2008 limit uses a lattice QCD calculation of the relevant hadronic matrix elements, while BEALL 1982 limit used the vacuum saturation approximation.


pdgid: S056MR
text:
MELCONIAN 2007 measure the neutrino angular asymmetry in beta+-decays of polarized K37, stored in a magneto-optical trap. Result is consistent with SM prediction and does not constrain the W_L - W_R mixing angle appreciably.


pdgid: S056MR
text:
SCHUMANN 2007 limit is from measurements of the asymmetry <pvector(nu).sigma_{{n}}> in the beta decay of polarized neutrons. Zero mixing is assumed.


pdgid: S056MR
text:
CYBURT 2005 limit follows by requiring that three light nu_{{R}}'s decouple when T_{{{dec}}}() > 140 MeV. For different T_{{{dec}}}(), the bound becomes M(W_{{R}}) > 3.3 TeV (T_{{{dec}}}() / 140 MeV)**3/4.


pdgid: S056MR
text:
THOMAS 2001 limit is from measurement of beta+ polarization in decay of polarized N12. The listed limit assumes no mixing.


pdgid: S056MR
text:
BARENBOIM 1998 assumes minimal left-right model with Higgs of SU(2)(R) in SU(2)(L) doublet.  For Higgs in SU(2)(L) triplet, mass(W_{{R}})>1100 GeV.  Bound calculated from effect of corresponding Z_{{LR}} on electroweak data through Z-Z_{{LR}} mixing.


pdgid: S056MR
text:
The quoted limit is from mu decay parameters.  BARENBOIM 1997 also evaluate limit from K_{{L}}-K_{{S}} mass difference.


pdgid: S056MR
text:
ALLET 1996 measured polarization-asymmetry correlation in  ^12N beta+ decay. The listed limit assumes zero L-R mixing.


pdgid: S056MR
text:
KUZNETSOV 1995 limit is from measurements of the asymmetry <pvector(nu).sigma_{{n}}> in the beta decay of polarized neutrons. Zero mixing assumed. See also KUZNETSOV 1994B.


pdgid: S056MR
text:
KUZNETSOV 1994B limit is from measurements of the asymmetry <pvector(nu).sigma_{{n}}> in the beta decay of polarized neutrons. Zero mixing assumed.


pdgid: S056MR
text:
BHATTACHARYYA 1993 uses Z-Z^' mixing limit from LEP '90 data, assuming a specific Higgs sector of SU(2)(L)xSU(2)(R)xU(1) gauge model.  The limit is for mass(t)=200 GeV and slightly improves for smaller mass(t).


pdgid: S056MR
text:
SEVERIJNS 1993 measured polarization-asymmetry correlation in  ^107In  beta+ decay. The listed limit assumes zero L-R mixing. Value quoted here is from SEVERIJNS 1994 erratum.


pdgid: S056MR
text:
IMAZATO 1992 measure positron asymmetry in K+ --> mu+ nu_mu decay and obtain xiP_{{mu}}>0.990 (90% CL). If W_{{R}} couples to u sbar with full weak strength (V(u s)**R=1), the result corresponds to mass(W_{{R}})>653 GeV.  See their Fig.4 for mass(W_{{R}}) limits for general |V(u s)**R|**2=1-|V(u d)**R|**2.


pdgid: S056MR
text:
POLAK 1992B limit is from fit to muon decay parameters and is essentially determined by JODIDIO 1986 data assuming zeta=0. Supersedes POLAK 1991.


pdgid: S056MR
text:
AQUINO 1991 limits obtained from neutron lifetime and asymmetries together with unitarity of the CKM matrix. Manifest left-right symmetry assumed. Stronger of the two limits also includes muon decay results.


pdgid: S056MR
text:
COLANGELO 1991 limit uses hadronic matrix elements evaluated by QCD sum rule and is less restrictive than BEALL 1982 limit which uses vacuum saturation approximation.  Manifest left-right symmetry assumed.


pdgid: S056MR
text:
POLAK 1991 limit is from fit to muon decay parameters and is essentially determined by JODIDIO 1986 data assuming zeta=0. Superseded by POLAK 1992B.


pdgid: S056MR
text:
LANGACKER 1989B limit is for any nu_{{R}} mass (either Dirac or Majorana) and for a general class of right-handed quark mixing matrices.


pdgid: S056MR
text:
BALKE 1988 limit is for mass(nu(e R)) = 0 and mass(nu(mu R)) <= 50 MeV. Limits come from precise measurements of the muon decay asymmetry as a function of the positron energy.


pdgid: S056MR
text:
JODIDIO 1986 is the same TRIUMF experiment as STOKER 1985 (and CARR 1983); however, it uses a different technique.  The results given here are combined results of the two techniques.  The technique here involves precise measurement of the end-point e+ spectrum in the decay of the highly polarized mu+.


pdgid: S056MR
text:
STOKER 1985 is same TRIUMF experiment as CARR 1983.  Here they measure the decay e+ spectrum asymmetry above 46 MeV/c using a muon-spin-rotation technique.  Assumed a light right-handed neutrino. Quoted limits are from combining with CARR 1983.


pdgid: S056MR
text:
CARR 1983 is TRIUMF experiment with a highly polarized mu+ beam. Looked for deviation from V-A at the high momentum end of the decay e+ energy spectrum.  Limit from previous world-average muon polarization parameter is mass(W_{{R}}) >240 GeV.  Assumes a light right-handed neutrino.


pdgid: S056MR
text:
BEALL 1982 limit is obtained assuming that W_{{R}} contribution to K(L)0-K(S)0 mass difference is smaller than the standard one, neglecting the top quark contributions. Manifest left-right symmetry assumed.


pdgid: S056WRZ
text:
MISHRA 1992 limit is from the absence of extra large-x, large-y nubar_mu N --> nubar_mu X events at Tevatron, assuming left-handed nu and right-handed nubar in the neutrino beam.  The result gives zeta**2(1-2mass**2(W_{{1}})/mass**2(W_{{2}}))<0.0015. The limit is independent of nu_{{R}} mass.


pdgid: S056WRZ
text:
AQUINO 1991 limits obtained from neutron lifetime and asymmetries together with unitarity of the CKM matrix. Manifest left-right asymmetry is assumed.


pdgid: S056Z1C
text:
TUMASYAN 2023AF search for resonance decaying to b bbar in p p collisions at sqrt(s)  = 13 TeV. See their Fig. 4 for limits on .


pdgid: S056Z1C
text:
TUMASYAN 2022AE set limits on Z^' from the measurements of the forward-backward asymmetry  in e+ e- and mu+ mu- events in p p collisions at sqrt(s) = 13 TeV. The quoted limit is  for the sequential SM Z^'. See their Fig. 6 for limits in mass-coupling plane.


pdgid: S056Z1C
text:
SIRUNYAN 2021N search for resonance decaying to e+ e-, mu+ mu- in p p collisions  at sqrt(s) = 13 TeV.


pdgid: S056Z1C
text:
AAD 2020T search for resonances decaying to b bbar in p p collisions at sqrt(s) = 13  TeV. See their Fig. 7(b) for limits on the product of the cross section, acceptance, b-tagging  efficiency, and branching fraction.


pdgid: S056Z1C
text:
SIRUNYAN 2018BB search for resonances decaying to lepton+ lepton- in p p collisions  at sqrt(s) = 13 TeV. See their Fig.5 for limits on the Z^' coupling strengths with light  quarks.


pdgid: S056Z1C
text:
AABOUD 2017AT search for resonances decaying to lepton+ lepton- in p p collisions at  sqrt(s) = 13 TeV.


pdgid: S056Z1C
text:
KHACHATRYAN 2017H search for resonances decaying to tau+ tau- in p p collisions at  sqrt(s) = 13 TeV.


pdgid: S056Z1C
text:
KHACHATRYAN 2017T search for resonances decaying to e+ e-, mu+ mu- in p p  collisions at sqrt(s) = 8, 13 TeV.


pdgid: S056Z1C
text:
AABOUD 2016U search for resonances decaying to lepton+ lepton- in p p collisions at  sqrt(s) = 13 TeV.


pdgid: S056Z1C
text:
KHACHATRYAN 2015AE search for resonances decaying to e+ e-, mu+ mu- in p p collisions at sqrt(s) = 8 TeV.


pdgid: S056Z1C
text:
BOBOVNIKOV 2018 use the ATLAS limits on sigma(p p --> Z^').B(Z^' --> W+ W-)  to constrain the Z-Z^' mixing parameter xi.   See their Fig. 11 for limits in  M(Z^')-xi plane.


pdgid: S056Z1C
text:
CHATRCHYAN 2013AF search for resonances decaying to e+ e-, mu+ mu- in p p collisions at sqrt(s) = 7 TeV and 8 TeV.


pdgid: S056Z1C
text:
AALTONEN 2011I search for resonances decaying to mu+ mu- in  p pbar collisions at sqrt(s) = 1.96 TeV.


pdgid: S056Z1C
text:
The quoted limit assumes g(W W Z^')/g(W W Z) = (M(W)/M(Z^'))**2. See their Fig.4 for limits in mass-coupling plane.


pdgid: S056Z1C
text:
ACOSTA 2005R search for resonances decaying to tau lepton pairs in pbar p collisions at sqrt(s) = 1.96 TeV.


pdgid: S056Z1C
text:
ABAZOV 2001B search for resonances in p pbar --> e+ e- at sqrt(s)=1.8 TeV. They find sigma.B(Z^' --> e e)<0.06pb for M(Z^')>500 GeV.


pdgid: S056Z1C
text:
BARATE 2000I search for deviations in cross section and asymmetries in e+ e- --> fermions at sqrt(s)=90 to 183 GeV.  Assume theta=0. Bounds in the mass-mixing plane are shown in their Figure18.


pdgid: S056Z1C
text:
ALITTI 1993 search for resonances in the two-jet invariant mass.  The limit assumes B(Z^' --> q qbar)=0.7.  See their Fig.5 for limits in the mass(Z^')-B(q qbar) plane.


pdgid: S056Z1C
text:
ABE 1990F use data for R, R(lepton lepton), and A(lepton lepton). They fix mass(W) = 80.49+-0.43+-0.24 GeV and mass(Z) = 91.13+-0.03 GeV.


pdgid: S056ZLR
text:
TUMASYAN 2023BE search for pair production of heavy Majorana neutrinos via the decay of a  Z^' boson in a final state with lepton+ lepton- and at least two jets. For cases with  mass(N) = M(Z^')/4, their 95% CL limits are M(Z^') > 3.59 TeV  (> 4.10 TeV) in the dielectron (dimuon) channel. See their Fig. 5 for limits on .


pdgid: S056ZLR
text:
BOBOVNIKOV 2018 use the ATLAS limits on sigma(p p --> Z^').B(Z^' --> W+ W-)  to constrain the Z-Z^' mixing parameter xi. See their Fig. 10 for limits in  M(Z^')-xi plane.


pdgid: S056ZLR
text:
ABDALLAH 2006C give 95% CL limit |theta|< 0.0028. See their Fig. 14 for limit contours in the mass-mixing plane.


pdgid: S056ZLR
text:
ABBIENDI 2004G give 95% CL limit on Z-Z^' mixing -0.00098 <theta< 0.00190. See their Fig. 20 for the limit contour in the mass-mixing plane.  sqrt(s) = 91 to 207GeV.


pdgid: S056ZLR
text:
ABREU 2000S give 95% CL limit on Z-Z^' mixing |theta|<0.0018. See their Fig.6 for the limit contour in the mass-mixing plane. sqrt(s)=90 to 189 GeV.


pdgid: S056ZLR
text:
ERLER 2000 discuss the possibility that a discrepancy between the observed and predicted values of Q_{{W}}(Cs) is due to the exchange of Z^'.  The data are better described in a certain class of the Z^' models including Z(LR) and Z_{{chi}}.


pdgid: S056ZLR
text:
CASALBUONI 1999 discuss the discrepancy between the observed and predicted values of Q_{{W}}(Cs).  It is shown that the data are better described in a class of models including the Z(LR) model.


pdgid: S056ZLR
text:
CZAKON 1999 perform a simultaneous fit to charged and neutral sectors. Assumes manifest left-right symmetric model.  Finds |theta|<0.0042.


pdgid: S056ZLR
text:
BARENBOIM 1998 also gives 68% CL limits on the Z-Z^' mixing -0.0005<theta<0.0033. Assumes Higgs sector of minimal left-right model.


pdgid: S056ZLR
text:
VILAIN 1994B assume mass(t) = 150 GeV and theta=0.  See Fig.2 for limit contours in the mass-mixing plane.


pdgid: S056ZLR
text:
GRIFOLS 1990 limit holds for mass(nu_{{R}}) ~<1 MeV.  A specific Higgs sector is assumed.  See also GRIFOLS 1990D, RIZZO 1991.


pdgid: S056ZLR
text:
BARBIERI 1989B limit holds for mass(nu_{{R}})<=10 MeV. Bounds depend on assumed supernova core temperature.


pdgid: S056ZCH
text:
BOBOVNIKOV 2018 use the ATLAS limits on sigma(p p --> Z^').B(Z^' --> W+ W-)  to constrain the Z-Z^' mixing parameter xi. See their Fig. 9 for limits in  M(Z^')-xi plane.


pdgid: S056ZCH
text:
AALTONEN 2009V search for resonances decaying to mu+ mu- in p pbar collisions at sqrt(s) = 1.96TeV.


pdgid: S056ZCH
text:
ABDALLAH 2006C give 95% CL limit |theta|< 0.0031. See their Fig. 14 for limit contours in the mass-mixing plane.


pdgid: S056ZCH
text:
ABULENCIA 2005A search for resonances decaying to electron or muon pairs in p pbar collisions at sqrt(s) = 1.96 TeV.


pdgid: S056ZCH
text:
ABBIENDI 2004G give 95% CL limit on Z-Z^' mixing -0.00099 <theta< 0.00194. See their Fig. 20 for the limit contour in the mass-mixing plane.  sqrt(s) = 91 to 207GeV.


pdgid: S056ZCH
text:
BARGER 2003B limit is from the nucleosynthesis bound on the effective number of light neutrino deltaN(nu)<1.  The quark-hadron transition temperature T(c)=150 MeV is assumed. The limit with T(c)=400 MeV is >4300 GeV.


pdgid: S056ZCH
text:
ABREU 2000S give 95% CL limit on Z-Z^' mixing |theta|<0.0017. See their Fig.6 for the limit contour in the mass-mixing plane. sqrt(s)=90 to 189 GeV.


pdgid: S056ZCH
text:
CHO 2000 use various electroweak data to constrain Z^' models assuming mass(H)=100 GeV.  See Fig.3 for limits in the mass-mixing plane.


pdgid: S056ZCH
text:
ERLER 2000 discuss the possibility that a discrepancy between the observed and predicted values of Q_{{W}}(Cs) is due to the exchange of Z^'.  The data are better described in a certain class of the Z^' models including Z_{{LR}} and Z_{{chi}}.


pdgid: S056ZCH
text:
ROSNER 2000 discusses the possibility that a discrepancy between the observed and predicted values of Q_{{W}}(Cs) is due to the exchange of Z^'.  The data are better described in a certain class of the Z^' models including Z_{{chi}}.


pdgid: S056ZCH
text:
FARAGGI 1991 limit assumes the nucleosynthesis bound on the effective number of neutrinos DeltaN_{{nu}} < 0.5 and is valid for mass(nu_{{R}}) < 1 MeV.


pdgid: S056ZCH
text:
ABE 1990F use data for R, R(lepton lepton), and A(lepton lepton). ABE 1990F fix mass(W) = 80.49+-0.43+-0.24 GeV and mass(Z) = 91.13+-0.03 GeV.


pdgid: S056ZCH
text:
Assumes  the nucleosynthesis bound on the effective number of light neutrinos (deltaN(nu) <1) and that  nu_{{R}} is light (~<1 MeV).


pdgid: S056ZPS
text:
SIRUNYAN 2018BB search for resonances decaying to lepton+ lepton- in p p collisions  at sqrt(s) = 13 TeV.


pdgid: S056ZPS
text:
CHATRCHYAN 2012M search for resonances decaying to e+ e- or mu+ mu- in p p collisions at sqrt(s) = 7 TeV.


pdgid: S056ZPS
text:
ABDALLAH 2006C give 95% CL limit |theta|< 0.0027. See their Fig. 14 for limit contours in the mass-mixing plane.


pdgid: S056ZPS
text:
ABBIENDI 2004G give 95% CL limit on Z-Z^' mixing -0.00129 <theta< 0.00258. See their Fig. 20 for the limit contour in the mass-mixing plane.  sqrt(s) = 91 to 207GeV.


pdgid: S056ZPS
text:
BARGER 2003B limit is from the nucleosynthesis bound on the effective number of light neutrino deltaN(nu)<1.  The quark-hadron transition temperature T(c)=150 MeV is assumed. The limit with T(c)=400 MeV is >1100 GeV.


pdgid: S056ZPS
text:
Assumes the nucleosynthesis bound on the effective number of light neutrinos (deltaN(nu) <1) and that nu_{{R}} is light (~<1 MeV).


pdgid: S056ZET
text:
ABDALLAH 2006C give 95% CL limit |theta|< 0.0092. See their Fig. 14 for limit contours in the mass-mixing plane.


pdgid: S056ZET
text:
ABBIENDI 2004G give 95% CL limit on Z-Z^' mixing -0.00447 <theta<0.00331. See their Fig. 20 for the limit contour in the mass-mixing plane.  sqrt(s) = 91 to 207GeV.


pdgid: S056ZET
text:
BARGER 2003B limit is from the nucleosynthesis bound on the effective number of light neutrino deltaN(nu)<1.  The quark-hadron transition temperature T(c)=150 MeV is assumed. The limit with T(c)=400 MeV is >3300 GeV.


pdgid: S056ZET
text:
ABREU 2000S give 95% CL limit on Z-Z^' mixing |theta|<0.0024. See their Fig.6 for the limit contour in the mass-mixing plane. sqrt(s)=90 to 189 GeV.


pdgid: S056ZET
text:
These authors claim that the nucleosynthesis bound on the effective number of light neutrinos (deltaN(nu) <1) constrains Z^' masses if nu_{{R}} is light (~<1 MeV).


pdgid: S056ZOT
text:
AAD 2023O search for resonances decaying to H Z in p p collisions at sqrt(s) = 13  TeV. The  quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 2800 GeV for g_{{V}} = 1.


pdgid: S056ZOT
text:
TUMASYAN 2023AF search for resonance decaying to b bbar in p p collisions at sqrt(s)  = 13 TeV. The limit quoted above is for heavy-vector-triplet Z^' with g_{{V}} = 1. See their   Fig. 4 for limits on .


pdgid: S056ZOT
text:
TUMASYAN 2023AP search for resonances decaying to W W in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit   becomes M(Z^') > 4.8 TeV assuming M(W^') =   M(Z^') and  combining W^' --> W Z, W^' --> W H, Z^' --> W W, Z^' --> Z H   channels.


pdgid: S056ZOT
text:
TUMASYAN 2023AP search for resonances decaying to $ZH$ in $pp$ collisions at  $sqrt{s}=13,$TeV.  The limit quoted above is for heavy-vector-triplet $Z'$ with $g_V=3$. The  limit becomes  $M_{Z'}>4.8$~TeV assuming $M_{W'}=M_{Z'}$ and combining $W'to WZ$, $W'to WH$,  $Z'to WW$, $Z'to ZH$  channels.


pdgid: S056ZOT
text:
TUMASYAN 2022D search for resonances produced through Drell-Yan and vector-boson-fusion  processes in p p collisions at sqrt(s) = 13 TeV. See their Fig. 8 for limits on . The  quoted limit is for heavy-vector-triplet W^' with g_{{V}} = 3 produced mainly via Drell-Yan.


pdgid: S056ZOT
text:
SIRUNYAN 2021X search for resonances decaying to H Z in p p collisions at sqrt(s) =  13 TeV. The  limit quoted above is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit  becomes  M(Z^') > 3500 GeV for g_{{V}} = 1.


pdgid: S056ZOT
text:
AAD 2020AJ search for resonances decaying to H Z in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 2200 GeV for g_{{V}} = 1. See their Fig. 6 for limits on .


pdgid: S056ZOT
text:
AAD 2020AM search for a resonance decaying to t tbar in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for a leptophobic top-color Z^' with  width(Z^')/M(Z^') = 0.01. The limit becomes M(Z^') > 4700 GeV for  width(Z^')/M(Z^') = 0.03.


pdgid: S056ZOT
text:
AAD 2020AT search for resonances decaying to W W in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 3500 GeV for g_{{V}} = 1. See their Fig. 14 for limits on .


pdgid: S056ZOT
text:
SIRUNYAN 2020Q search for resonances decaying to W W in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3.


pdgid: S056ZOT
text:
AABOUD 2019AS search for a resonance decaying to t tbar in p p collisions at sqrt(s)  = 13 TeV. The quoted limit is for a top-color Z^' with  Gamma(Z^')/M(Z^') = 0.01. Limits are also set on Z^' masses in  simplified Dark Matter models.


pdgid: S056ZOT
text:
AAD 2019D search for resonances decaying to W W in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 2900 GeV for g_{{V}} = 1. If we assume M(Z^') =  M(W^'), the limit increases M(Z^') > 3800 GeV and  M(Z^') > 3500 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their  Fig. 9 for limits on .


pdgid: S056ZOT
text:
SIRUNYAN 2019AA search for a resonance decaying to t tbar in p p collisions at  sqrt(s) = 13 TeV. The quoted limit is for a leptophobic top-color Z^' with  Gamma(Z^')/M(Z^') = 0.01.


pdgid: S056ZOT
text:
SIRUNYAN 2019CP present a statistical combinations of searches for Z^' decaying to pairs  of bosons or leptons in p p collisions at sqrt(s) = 13 TeV. The quoted limit is for  heavy-vector-triplet Z^' with g_{{V}} = 3. If we assume M(Z^') =  M(W^'), the limit becomes M(Z^') > 4500 GeV for g_{{V}} = 3 and  M(Z^') > 5000 GeV for g_{{V}} = 1. See their Figs. 2 and 3 for limits on  .


pdgid: S056ZOT
text:
SIRUNYAN 2019I search for resonances decaying to Z W in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 2800 GeV if we assume M(Z^') =  M(W^').


pdgid: S056ZOT
text:
AABOUD 2018AB search for resonances decaying to b bbar in p p collisions at sqrt(s)  = 13 TeV. The limit quoted above is for a leptophobic Z^' with SM-like couplings to quarks. See  their Fig. 6 for limits on . Additional limits on a Z^' axial-vector mediator in a  simplified dark-matter model are shown in Fig. 7.


pdgid: S056ZOT
text:
AABOUD 2018AI search for resonances decaying to H Z in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 2650 GeV for g_{{V}} = 1. If we assume M(W^') =  M(Z^'), the limit increases M(Z^') > 2930 GeV and  M(Z^') > 2800 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their  Fig. 5 for limits on sigma.B.


pdgid: S056ZOT
text:
AABOUD 2018AK search for resonances decaying to W W in p p collisions at sqrt(s) =1  3 TeV. The limit quoted above is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit  becomes M(Z^') > 2750 GeV for g_{{V}} = 1.


pdgid: S056ZOT
text:
AABOUD 2018B search for resonances decaying to W W in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 1. See their Fig.11 for  limits on sigma.B.


pdgid: S056ZOT
text:
AABOUD 2018BI search for a resonance decaying to t tbar in p p collisions at sqrt(s)  = 13 TeV. The quoted limit is for a top-color assisted TC Z^' with Gamma(Z^')/M(Z^') = 0.01. The limits for wider resonances are  available. See their Fig. 14 for limits on sigma.B.


pdgid: S056ZOT
text:
AABOUD 2018F search for resonances decaying to W W in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes  M(Z^') > 2200 GeV for g_{{V}} = 1. If we assume M(Z^') =  M(W^'), the limit increases M(Z^') > 3500 GeV and  M(Z^') > 3100 GeV for g_{{V}} = 3 and g_{{V}} = 1, respectively. See their  Fig.5 for limits on sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2018ED search for resonances decaying to H Z in p p collisions at sqrt(s) =  13 TeV. The limit above is for heavy-vector-triplet Z^' with g_{{V}} = 3. If we assume  M(Z^') = M(W^'), the limit increases M(Z^')  > 2900 GeV and M(Z^') > 2800 GeV for g_{{V}} = 3 and g_{{V}} = 1,  respectively.


pdgid: S056ZOT
text:
SIRUNYAN 2018P give this limit for a heavy-vector-triplet Z^' with g_{{V}} = 3. If they  assume M(Z^') = M(W^'), the limit increases to  M(Z^') > 3800 GeV.


pdgid: S056ZOT
text:
AABOUD 2017AK search for a new resonance decaying to dijets in $pp$ collisions at  sqrt(s) = 13 TeV. The limit quoted above is for a leptophobic Z^' boson having axial-vector  coupling strength with quarks g_{{q}} = 0.2. The limit is 2100 GeV if g_{{q}} = 0.1.


pdgid: S056ZOT
text:
AABOUD 2017AO search for resonances decaying to H Z in p p collisions at sqrt(s) =  13 TeV. The limit quoted above is for a Z^' in the heavy-vector-triplet model with g_{{V}} = 3.  See their Fig.4 for limits on sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2017AK search for resonances decaying to W W or H Z in p p collisions at  sqrt(s) = 8 and 13 TeV.   The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes M(Z^') > 2200 GeV for g_{{V}} =1. If we assume  M(Z^') = M(W^'), the limit increases M(Z^')  > 2400 GeV for both g_{{V}} = 3 and g_{{V}} = 1. See their Fig.1 and 2 for limits on  sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2017Q search for a resonance decaying to t tbar in p p collisions at  sqrt(s) = 13 TeV. The limit quoted above is for a resonance with relative width  Gamma(Z^') / M(Z^') = 0.01. Limits for wider resonances are  available. See their Fig.6 for limits on sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2017R search for resonances decaying to H Z in p p collisions at sqrt(s) =  13 TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. Mass regions  M(Z^') < 1150 GeV and 1250 GeV < M(Z^') < 1670  GeV are excluded for g_{{V}} = 1. If we assume M(Z^') = M(W^'),  the excluded mass regions are 1000 < M(Z^') < 2500 GeV and 2760  < M(Z^') < 3300 GeV for g_{{V}} = 3; 1000 <  M(Z^') < 2430 GeV and 2810 < M(Z^') < 3130 GeV  for g_{{V}} = 1. See their Fig.5 for limits on sigma.B.


pdgid: S056ZOT
text:
AAD 2024AA search for Z^' production in p p collisions at sqrt(s) = 13 TeV. Z^'  is assumed to decay into a pair of dark quarks which hadronise into dark hadrons before promptly  decaying back as SM particles. The dark pions are either assumed to decay directly to SM quarks or  through dark photons. See their Fig. 7 for limits on .


pdgid: S056ZOT
text:
AAD 2024AE search for resonances decaying to q q, t t, t b, V V, V H,  lepton lepton, lepton tau, tau nu, tau tau in p p collisions at sqrt(s) = 13  TeV. The quoted limit is for heavy-vector-triplet Z^' with g_{{V}} = 3. M(Z^')  = M(W^') is assumed. The limit becomes M(Z^') > 5.8 TeV for  g_{{V}} = 1.


pdgid: S056ZOT
text:
AAD 2024AY search for a low-mass leptophobic Z^' produced in association of high pT  ISR photon or jet in p p collisions at sqrt(s) = 13 TeV. The Z^' coupling with quarks  g_{{q}} is constrained below 0.07 for 250 < M(Z^') < 650 GeV. See  their Fig. 8 for exclusion limit in the mass-coupling plane.


pdgid: S056ZOT
text:
AAD 2024BJ search for top-philic Z^' in p p collisions at sqrt(s) = 13 TeV. See  their Fig. 9 for limits on CS(p p --> t ( tbar ) Z^').B(Z^' --> t tbar).


pdgid: S056ZOT
text:
AAD 2024BR search for L_{{mu}}-L_{{tau}} Z^' in 3 mu final states in p p  collisions at sqrt(s) = 13 TeV. Limits are combined with previous search results in the 4 mu  final states reported in AAD 2023X. See their Fig. 4 for limits in mass-coupling plane.


pdgid: S056ZOT
text:
AAD 2024CD search for a DM simplified Z^' produced in association with W or Z in  p p collisions at sqrt(s) = 13 TeV. Z^' is assumed to decay invisibly. See their Fig. 13  for limits in M(Z^')-M_{{DM}} plane.


pdgid: S056ZOT
text:
AAD 2024CI give a summary of searches for DM simplified Z^' in p p collisions at  sqrt(s) = 13 TeV. See their Figs. 6 -- 11 for the limits.


pdgid: S056ZOT
text:
AAD 2024CM search for pair productions of dark pions pi_D()+ pi_D()- in t t b b  events of p p collisions at sqrt(s) = 13 TeV. pi_D()+- --> t b decay is assumed. The  production cross section is computed in a model with dark rho_{{D}}()0 assuming dark isospin  symmetry mass(rho_{{D}}()+-) = mass(rho_{{D}}()0), mass(pi_{{D}}()+-) = mass(pi_{{D}}()0). See their Fig. 12  for limits on the production cross sections.


pdgid: S056ZOT
text:
ABLIKIM 2024G search for a muonphilic Z^' and a muonphilic scalar X_{{0}}() in decays of  J/psi --> mu+ mu- + invisible. See their Fig. 3 for limits in the mass coupling plane.


pdgid: S056ZOT
text:
ADACHI 2024F for a muonphilic Z^' and a muonphilic scalar X_{{0}}() in mu+ mu- mu+ mu- events  of e+ e- collisions at sqrt(s) = 10.58 GeV. See their Fig. 14 for limits in mass-coupling  plane.


pdgid: S056ZOT
text:
AKITA 2024 limit is from no events of high-energy SN1987A neutrinos. The Z^' coupling  down to g ~3E-10 is excluded for M(Z^') < 400 MeV in the  L_{{mu}}-L_{{tau}} Z^' model. See their Fig. 3 and Fig. 4 for exclusion limits in  mass-coupling plane.


pdgid: S056ZOT
text:
ANDREEV 2024 search for Z^' production in mu-nucleus scattering. Z^' is assumed  to decay invisibly. See their Fig. 4 for limits in mass-coupling plane.


pdgid: S056ZOT
text:
ANDREEV 2024B search for Z^' production in e+--nucleus scattering. Z^' is assumed  to decay invisibly. See their Fig. 4 for limits in mass-coupling plane.


pdgid: S056ZOT
text:
ANDREEV 2024E search for Z^' production in mu-nucleus scattering. Invisible decays of  Z^' are assumed. See their Fig. 17 and Fig. 19 for limits in mass-coupling plane for Z^'  masses from 0.001 to 1 GeV.


pdgid: S056ZOT
text:
BISWAS 2024 search for leptophilic scalar X_{{0}}() produced in association with tau+ tau- in e+ e-  collisions near sqrt(s) = 10.58 GeV. X_{{0}}() is assumed to decay into e+ e- or mu+ mu-.  See their Fig. 7 for limits in mass-coupling plane.


pdgid: S056ZOT
text:
HAYRAPETYAN 2024AZ search for Z^' resonances produced via kinetic mixing parameter  epsilon and decaying to s_D sbar_D in p p collisions at sqrt(s) = 13 TeV. Both s_{{D}}  and sbar_{{D}} are assumed to decay into mu+ mu-. See their Fig. 7 for limits on  epsilon^2B(Z^' --> s_D sbar_D)B**2(s_D --> mu+ mu-).


pdgid: S056ZOT
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. 2 for limits on .


pdgid: S056ZOT
text:
HAYRAPETYAN 2024W search for W+ W- + notET events in p p collisions at sqrt(s)  = 13 TeV. Z^' is assumed to decay into dark Higgs S (--> W+ W-) and DM particles chi chi. See  their Fig. 5 for exclusion limits on the production cross section.


pdgid: S056ZOT
text:
AAD 2023BF search for a Dark Matter (DM) simplified Z^' produced in association with  W   in p p collisions at sqrt(s) = 13 TeV. See their Fig. 9(c) for limits on  as  a   function  of M(Z^').


pdgid: S056ZOT
text:
AAD 2023W set limits on a dark Higgs model with a spin-1 mediator Z^' and a dark Higgs  s.  Dark  Higgs s is assumed to decay into W W. See their Fig. 9 for limits in  M(Z^')-M_{{s}} plane.


pdgid: S056ZOT
text:
AAD 2023X set limits on L_{{mu}}-L_{{tau}} of Z^' using four-muon final states in  p p collisions at sqrt(s) = 13 TeV. See their Fig. 7 for limits in mass-coupling plane.


pdgid: S056ZOT
text:
ADACHI 2023B search for Z^' produced in association with mu+ mu- and decaying  invisibly in e+ e- collisions at sqrt(s) = 10.58 GeV. See their Fig. 3 and Fig. 4 for limits  in mass-coupling plane.


pdgid: S056ZOT
text:
ADACHI 2023F search for resonances decaying to tau+ tau- in mu+ mu- tau+ tau- events  in e+ e- collisions at sqrt(s) = 10.58 GeV. See their Fig. 3 for limits on .


pdgid: S056ZOT
text:
HAYRAPETYAN 2023D search for mu+ mu- resonance produced in association with one or more  b-jets in p p collisions at sqrt(s) = 13 TeV. See their Fig. 8 for limits in the  mass-coupling plane of the B_{{3}}-L_{{2}} Z^' model.


pdgid: S056ZOT
text:
HAYRAPETYAN 2023G search for spin-0 and spin-1 resonances decaying to mu+ mu- in $pp$  collisions at sqrt(s) = 13 TeV in the mass ranges of 1.1 -- 2.6 GeV and 4.2 -- 7.9  GeV. See their Fig. 5 for limits on .


pdgid: S056ZOT
text:
LI 2023I limits on light Z^' couplings are dervied from the steller cooling bounds in the  mass range of E4 -- E6 eV. See their Fig. 4 for limits on dark photon,  B-L, L_{{mu}}-L_{{tau}}, and  L_{{e}}-L(mu(tau)) models.


pdgid: S056ZOT
text:
MANZARI 2023 study supernova cooling induced by the emission of light dark fermions chi  assumed to couple with leptons via a new massive vector boson Z^'. See their Figs. 4 and 5 for  limits in mass-coupling plane.


pdgid: S056ZOT
text:
AAD 2022 search for b bbar Z^' productions in p p collisions at sqrt(s) = 13 TeV.  Z^' is assumed to decay into b bbar. See their Fig.4 for limits on .


pdgid: S056ZOT
text:
AAD 2022D search for DM mediator Z^' produced in association with a Z boson in $pp$  collisions at sqrt(s) = 13 TeV. Z^' is assumed to decay invisibly Z^' --> chi chi. See  their Fig. 4 for limits in M(Z^')-M(chi) plane.


pdgid: S056ZOT
text:
ANDREEV 2022 search for missing energy in CERN NA64-e experiment. See their Fig. 7 for limits  on   couplings of U(1) gauge L_{{mu}}-L_{{tau}} Z^' models, in the mass range of  1 MeV < M(Z^') < 600 MeV   with the kinetic Z^'-gamma  mixing being determined by mu and tau loops.


pdgid: S056ZOT
text:
BONET 2022 obtain limits on Z^' coupling from nu-nucleus scattering data collected by  the CONUS experiment at the nuclear power plant in Brokdorf. See their Fig. 5 for limits in  mass-coupling plane.


pdgid: S056ZOT
text:
COLOMA 2022 set limits on Z^' coupling from nu-nucleus and nu-e scattering  data collected by a  Ge detector at the Dresden-II power reactor and the COHERENT  experiment. See their Fig.  6 for limits in mass-coupling plane in the mass range of 1 keV <  M(Z^')  < 5 GeV.


pdgid: S056ZOT
text:
COLOMA 2022A use Borexino Phase-II spectral data to constrain Z^' couplings. See their  Fig. 5 for limits in mass-coupling plane in the mass range of 10 keV <  M(Z^') < 100 MeV.


pdgid: S056ZOT
text:
CZANK 2022 search for Z^' produced in association with mu+ mu- in e+ e-  collisions at and near Upsilon resonances. Z^' is assumed to decay into mu+ mu-. See  their Fig. 8 for limits on Z^' mu mu couplings.


pdgid: S056ZOT
text:
TUMASYAN 2022AA search for Z^' production in p p collisions at sqrt(s) = 13 TeV.  Z^' is assumed to decay into two "semivisible" jets (SVJ), i.e., collimated mixtures of visible  and invisible particles. See their Fig. 7 and 8 for limits on .


pdgid: S056ZOT
text:
AAD 2021AQ limits are for a B - L gauge boson model derived from their  measurements on four-lepton differential cross sections. See their Fig. 13 for exclusion limits on  the B - L breaking Higgs boson mass.


pdgid: S056ZOT
text:
AAD 2021AZ search for DM mediator Z^' produced in association with a SM Higgs boson in  p p collisions at sqrt(s) = 13 TeV. Z^' is assumed to decay invisibly Z^' --> chi chi.  See their Fig.7 for limits in M(Z^')-M_{{chi}} plane.


pdgid: S056ZOT
text:
AAD 2021BB search for Z^' productions in p p collisions at sqrt(s) = 13 TeV. Z^'    is assumed to  decay into a SM Higgs boson H and an invisible particle A. See their Fig.7    for limits in  M(Z^')-M_{{A}} plane.


pdgid: S056ZOT
text:
AAD 2021D set limits on a dark Higgs model with a spin-1 mediator  Z^' and a scalar dark   Higgs boson s. Dark Higgs s is assumed to decay into W W or  Z Z. See their Fig.4   for limits in M(Z^')-M_{{s}} plane.


pdgid: S056ZOT
text:
AAD 2021K search for gamma + notET events in p p collision at sqrt(s) = 13  TeV. See  their Fig. 5 for limits on Z^' particle invisibly decaying to chi chi.


pdgid: S056ZOT
text:
CADEDDU 2021 obtain limits on Z^' coupling g(Z^') from coherent  nu-nucleus scattering data collected by COHERENT experiment. For limits in the   M(Z^')-g(Z^') plane, see their Figures 3 and 4 for the universal  Z^' model and Figures 5 and 6 for the B-L model.


pdgid: S056ZOT
text:
COLARESI 2021 obtain limits on Z^' coupling from coherent nu-nucleus scattering data  collected  by a Ge detector at the Dresden-II power reactor. See their Fig.7 for limits  in  mass-coupling plane.


pdgid: S056ZOT
text:
KRIBS 2021 set decay-agnostic limits on kinetic mixing parameter between U(1)(Y) field   and new heavy abelian vector boson (dark photon) field using the HERA e p collision data. See   their Fig. 3 for limits in mass-mixing plane.


pdgid: S056ZOT
text:
TUMASYAN 2021D search for energetic jets + notET events in p p collisions at  sqrt(s) = 13 TeV. Z^' is assumed to decay into a pair of invisible particles chi chi. See  their Fig. 7 for limits on signal strength in M(Z^')-M_{{chi}} plane, and Fig. 8  for limits on signal strength in quark and dark matter coupling vs mediator mass.


pdgid: S056ZOT
text:
AAD 2020AF search for resonances decaying to H gamma in p p collisions at sqrt(s) =  13 TeV. See their Fig. 1c for limits on  for the mass range 0.7 < mass(Z^') <  4 TeV.


pdgid: S056ZOT
text:
AAD 2020T search for Dark Matter mediator Z^' decaying invisibly or decaying to q qbar in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 5 for limits in  M(Z^')-g_{{q}} plane from the inclusive category. See their Fig. 7(a) for  limits on the product of the cross section, acceptance, b-tagging efficiency, and branching  fraction from the 2 b-tag category.


pdgid: S056ZOT
text:
AAD 2020W search for a Dark Matter (DM) simplified model Z^' produced in association with  W in p p collisions at sqrt(s) = 13 TeV. See their Fig. 5 for limits on Z^' production  cross section.


pdgid: S056ZOT
text:
AAIJ 2020AL search for spin-0 and spin-1 resonances  decaying to mu+ mu-  in p p  collisions at sqrt(s) = 13 TeV in the mass regions M(Z^') < 60 GeV, with  non-negligible widths considered above 20 GeV. See their Figs. 7, 8, and 9 for limits on .


pdgid: S056ZOT
text:
ADACHI 2020 search for production of Z^'  in e+ e- collisions. The Z^' is assume  to decay invisibly. See their Fig. 3 and Fig. 5 for limits on Z^' coupling and CS(e+ e- --> e+- mu-+ Z^').


pdgid: S056ZOT
text:
SIRUNYAN 2020AI search for broad resonances decaying  into  dijets in p p collisions at  sqrt(s) = 13 TeV. See their Fig. 11 for exclusion limits in mass-coupling plane.


pdgid: S056ZOT
text:
SIRUNYAN 2020AQ search for a narrow resonance lighter than 200 GeV decaying to mu+ mu- in  p p collisions at sqrt(s) = 13 TeV. See their Fig. 3 for limits on Z^' kinetic mixing  coefficient.


pdgid: S056ZOT
text:
SIRUNYAN 2020M search for a narrow resonance with a  mass between 350 and 700 GeV in p p  collisions at sqrt(s) = 13 TeV. See their Fig.3 for exclusion limits in mass-coupling plane.


pdgid: S056ZOT
text:
AABOUD 2019AJ search in p p collisions at sqrt(s) = 13 TeV for a new resonance decaying  to q qbar and produced in association with a high pT photon. For a leptophobic  axial-vector Z^' in the mass region 250 GeV < M(Z^') < 950 GeV,  the Z^' coupling with quarks g_{{q}} is constrained below 0.18. See their Fig.2 for limits in  M(Z^')-g_{{q}} plane.


pdgid: S056ZOT
text:
AABOUD 2019D search in p p collisions at sqrt(s) = 13 TeV for a new resonance decaying  to q qbar and produced in association with a high-pT photon or jet. For a leptophobic  axial-vector Z^' in the mass region 100 GeV < M(Z^') < 220 GeV, the Z^' coupling with quarks g_{{q}} is constrained below 0.23. See their Fig. 6 for limits in  M(Z^')-g_{{q}} plane.


pdgid: S056ZOT
text:
AABOUD 2019V search for Dark Matter simplified Z^' decaying invisibly  or decaying to  fermion pair in p p collisions at sqrt(s) = 13 TeV.


pdgid: S056ZOT
text:
AAD 2019L search for resonances decaying to lepton+ lepton- in p p collisions at  sqrt(s) = 13 TeV. See their Fig. 4 for limits in the heavy vector triplet model couplings.


pdgid: S056ZOT
text:
LONG 2019 uses the weak charge data of Cesium and proton to constrain mass of Z^' in the  3-3-1 models.


pdgid: S056ZOT
text:
PANDEY 2019 obtain limits on Z^' induced neutrino non-standard interaction (NSI)  parameter epsilon from LHC and IceCube data. See their Fig.2 for limits in  M(Z^')-epsilon plane, where epsilon = g_{{q}} g(nu)  v**2 / (2 M(Z^')**2).


pdgid: S056ZOT
text:
SIRUNYAN 2019AL search for a new resonance decaying to a  top quark and a heavy vector-like  top partner in  p p collisions at sqrt(s) = 13 TeV. See their Fig. 8 for limits on Z^'  production cross section.


pdgid: S056ZOT
text:
SIRUNYAN 2019AN search for a Dark Matter (DM) simplified model Z^' decaying  to H DM  DM in p p collisions at sqrt(s) = 13 TeV. See their Fig. 7 for limits on the signal strength  modifiers.


pdgid: S056ZOT
text:
SIRUNYAN 2019CB search in p p collisions at sqrt(s) = 13 TeV for a new resonance  decaying to q qbar. For a leptophobic Z^' in the mass region 50 -- 300 GeV,  the  Z^' coupling with quarks g_{{q}}^' is constrained below 0.2. See their Figs. 4 and 5 for limits  on g_{{q}}^' in the mass range 50 < M(Z^') < 450 GeV.


pdgid: S056ZOT
text:
SIRUNYAN 2019CD search in p p collisions at sqrt(s)=13 TeV for a leptophobic Z^'  produced in association of high pT ISR photon and decaying to q qbar. See their Fig. 2  for limits on the Z^' coupling strength g_{{q}}^' to q qbar in the mass range between 10  and 125 GeV.


pdgid: S056ZOT
text:
SIRUNYAN 2019D search for a narrow neutral vector resonance decaying to H gamma. See  their Fig. 3 for exclusion limit in M(Z^')-sigma B plane. Upper  limits on the production of H gamma resonances are set as a function of the resonance mass in  the range of 720 -- 3250 GeV.


pdgid: S056ZOT
text:
AABOUD 2018AA search for a narrow neutral vector boson decaying to H gamma.  See their Fig. 10 for the exclusion limit in M(Z^') - sigmaB plane.


pdgid: S056ZOT
text:
AABOUD 2018CJ search for heavy-vector-triplet $Z'$ in $pp$ collisions  at $sqrt{s}=13$ TeV.  The limit quoted above is for model with $g_V=3$ assuming $M_{Z'}=M_{W'}$. The limit becomes  $M_{Z'}>5500$ GeV for model with $g_V=1$.


pdgid: S056ZOT
text:
AABOUD 2018N search for a narrow resonance decaying to q qbar in p p collisions at  sqrt(s) = 13 TeV using  trigger level analysis to improve the low mass region sensitivity. See  their Fig. 5 for limits in the mass-coupling plane in the Z^' mass range 450 -- 1800 GeV.


pdgid: S056ZOT
text:
AAIJ 2018AQ search for spin-0 and spin-1 resonances decaying to mu+ mu- in p p  collisions at sqrt(s) = 7 and 8 TeV in the mass region near 10 GeV. See their Figs. 4 and 5 for  limits on sigma B.


pdgid: S056ZOT
text:
SIRUNYAN 2018DR searches for mu+ mu- resonances produced in association with b-jets  in the p p collision data with sqrt(s) = 8 TeV and 13 TeV. An excess of events near  mass(mu mu) = 28 GeV is observed in the 8 TeV data. See their Fig. 3 for the measured  fiducial signal cross sections  at sqrt(s) = 8 TeV and the 95% CL upper limits at sqrt(s) =  13 TeV.


pdgid: S056ZOT
text:
SIRUNYAN 2018G search for a new resonance decaying to dijets in p p collisions at  sqrt(s) = 13 TeV in the mass range 50 -- 300 GeV. See their Fig.7 for limits in the  mass-coupling plane.


pdgid: S056ZOT
text:
SIRUNYAN 2018I search for a narrow resonance decaying to b bbar in p p collisions at  sqrt(s) = 8 TeV using dedicated b-tagged dijet triggers to improve the sensitivity in the low mass  region. See their Fig. 3 for limits on sigma.B in the Z^' mass range  325 -- 1200 GeV.


pdgid: S056ZOT
text:
AABOUD 2017B search for resonances decaying to H Z (H --> b bbar, c cbar; Z --> lepton+ lepton-,  nu nubar) in p p collisions at sqrt(s) = 13 TeV. The quoted limit is for  heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes M(Z^')> 1490 GeV  for g_{{V}} = 1. If we assume M(Z^') = M(W^'), the limit increases  M(Z^')> 2310 GeV and M(Z^')> 1730 GeV for g_{{V}} = 3 and  g_{{V}} = 1, respectively. See their Fig.3 for limits on sigma.B.


pdgid: S056ZOT
text:
KHACHATRYAN 2017AX search for lepto-phobic resonances decaying to four leptons in p p  collisions at sqrt(s) = 8 TeV.


pdgid: S056ZOT
text:
KHACHATRYAN 2017U search for resonances decaying to H Z (H --> b bbar; Z --> lepton+ lepton-, nu nubar) in  p p collisions at sqrt(s) = 13 TeV. The limit on the heavy-vector-triplet model is  M(Z^') = M(W^') > 2 TeV for g_{{V}} = 3, in which  constraints from the W^' --> H W (H --> b bbar; W --> lepton nu) are combined. See  their Fig.3 and Fig.4 for limits on sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2017A search for resonances decaying to W W with W W --> lepton nu q qbar,  q qbar q qbar in p p collisions at sqrt(s) = 13 TeV. The quoted limit is for  heavy-vector-triplet Z^' with g_{{V}} = 3. The limit becomes M(Z^') >  1600 GeV for g_{{V}} = 1. If we assume M(Z^') = M(W^'), the limit  increases M(Z^') > 2400 GeV and M(Z^') > 2300 GeV for  g_{{V}} = 3 and g_{{V}} = 1, respectively. See their Fig.6 for limits on  sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2017AP search for resonances decaying into a SM-like Higgs scalar H and a light  pseudo scalar A. A is assumed to decay invisibly. See their Fig.9 for limits on sigma.B.


pdgid: S056ZOT
text:
SIRUNYAN 2017T search for a new resonance decaying to dijets in $pp$ collisions at  sqrt(s) = 13 TeV in the mass range 100 -- 300 GeV. See their Fig.3 for limits in the  mass-coupling plane.


pdgid: S056ZOT
text:
SIRUNYAN 2017V search for a new resonance decaying to a top quark and a heavy vector-like top  partner T in p p collisions at sqrt(s) = 13 TeV. See their table 5 for limits on the  Z^' production cross section for various values of M(Z^') and  M(T) in the range of M(Z^') = 1500 -- 2500 GeV and  M(T) = 700 -- 1500 GeV.


pdgid: S056ZOT
text:
AABOUD 2016 search for a narrow resonance decaying into b bbar in p p collisions at  sqrt(s) = 13 TeV. The limit quoted above is for a leptophobic Z^' with SM-like  couplings to  quarks. See their Fig.6 for limits on sigma.B.


pdgid: S056ZOT
text:
AAD 2016L search for Z^' --> a gamma , a --> gamma gamma in p p collisions at  sqrt(s) = 8 TeV. See their Table 6 for limits on sigma.B.


pdgid: S056ZOT
text:
AAD 2016S search for a new resonance decaying to dijets  in p p collisions at sqrt(s) = 13 TeV. The limit quoted above is for a leptophobic Z^' having  coupling strength with quark g_{{q}} = 0.3 and is  taken from their Figure 3.


pdgid: S056ZOT
text:
KHACHATRYAN 2016AP search for a resonance decaying to H Z in p p collisions at  sqrt(s) = 8 TeV. Both H and Z are assumed to decay to fat jets. The quoted limit is for  heavy-vector-triplet Z^' with g_{{V}} = 3.


pdgid: S056ZOT
text:
KHACHATRYAN 2016E search for a leptophobic top-color Z^' decaying to t tbar using p p collisions at sqrt(s) = 8 TeV. The quoted limit assumes that width(Z^')/mass(Z^') = 0.012. Also mass(Z^') < 2.9 TeV is excluded for wider topcolor Z^' with width(Z^')/mass(Z^') = 0.1.


pdgid: S056ZOT
text:
<a class=a  href='https://inspirehep.net/literature/1373299' target='_blank'>AAD 2015AO</a> search for narrow resonance decaying to t tbar using p p collisions at sqrt(s) = 8 TeV. See Fig. 11 for limit on sigmaB.


pdgid: S056ZOT
text:
AAD 2015AT search for monotop production plus large missing E(T) events in p p collisions at sqrt(s) = 8 TeV and give constraints on a Z^' model having Z^' u tbar coupling. Z^' is assumed to decay invisibly. See their Fig. 6 for limits on  sigma.B.


pdgid: S056ZOT
text:
AAD 2015CD search for decays of Higgs bosons to 4 lepton states via Z^' bosons, H --> Z Z^' --> 4 lepton or H --> Z^' Z^' --> 4 lepton. See Fig. 5 for the limit on the signal strength of the H --> Z Z^' --> 4 lepton process and Fig. 16 for the limit on H --> Z^' Z^' --> 4 lepton.


pdgid: S056ZOT
text:
KHACHATRYAN 2015F search for monotop production plus large missing E(T) events in p p collisions at sqrt(s) = 8 TeV and give constraints on a Z^' model having Z^' u tbar coupling. Z^' is assumed to decay invisibly. See Fig. 3 for limits on sigmaB.


pdgid: S056ZOT
text:
KHACHATRYAN 2015O search for narrow Z^' resonance decaying to Z H in p p collisions at sqrt(s) = 8 TeV. See their Fig. 6 for limit on sigmaB.


pdgid: S056ZOT
text:
AAD 2014AT search for a narrow neutral vector boson decaying to Z gamma. See their Fig. 3b for the exclusion limit in mass(Z^')-sigmaB plane.


pdgid: S056ZOT
text:
KHACHATRYAN 2014A search for new resonance in the W W (lepton nu q qbar) and the Z Z (lepton lepton q qbar) channels using p p collisions at sqrt(s)=8 TeV. See their Fig.13 for the exclusion limit on the number of events in the mass-width plane.


pdgid: S056ZOT
text:
AAD 2013AQ search for a leptophobic top-color Z^' decaying to t tbar. The quoted limit assumes that width(Z^')/mass(Z^') = 0.012.


pdgid: S056ZOT
text:
CHATRCHYAN 2013BM search for top-color Z^' decaying to t tbar using p p collisions at sqrt(s)=8 TeV. The quoted limit is for width(Z^')/mass(Z^') = 0.012.


pdgid: S056ZOT
text:
CHATRCHYAN 2013AP search for top-color leptophobic Z^' decaying to t tbar using p p collisions at sqrt(s)=7 TeV. The quoted limit is for width(Z^')/mass(Z^') = 0.012.


pdgid: S056ZOT
text:
AAD 2012BV search for narrow resonance decaying to t tbar using p p collisions at sqrt(s)=7 TeV. See their Fig. 7 for limit on sigma.B.


pdgid: S056ZOT
text:
AAD 2012K search for narrow resonance decaying to t tbar using p p collisions at sqrt(s)=7 TeV. See their Fig. 5 for limit on sigma.B.


pdgid: S056ZOT
text:
AALTONEN 2012AR search for chromophilic Z^' in p pbar collisions at sqrt(s) = 1.96 TeV. See their Fig. 5 for limit on sigma.B.


pdgid: S056ZOT
text:
AALTONEN 2012N search for p pbar --> t Z^', Z^' --> tbar u events in p pbar collisions. See their Fig. 3 for the limit on sigma.B.


pdgid: S056ZOT
text:
ABAZOV 2012R search for top-color Z^' boson decaying exclusively to t tbar. The quoted limit is for width(Z^')/mass(Z^')= 0.012.


pdgid: S056ZOT
text:
CHATRCHYAN 2012AI search for p p --> t t events and give constraints on a Z^' model having Z^' ubar t coupling. See their Fig. 4 for the limit in mass-coupling plane.


pdgid: S056ZOT
text:
CHATRCHYAN 2011O search for same-sign top production in p p collisions induced by a hypothetical FCNC Z^'() at sqrt(s) = 7 TeV. See their Fig. 3 for limit in mass-coupling plane.


pdgid: S056ZOT
text:
BARGER 2003B use the nucleosynthesis bound on the effective number of light neutrino deltaN(nu). See their Figs.4 -- 5 for limits in general E(6) motivated models.


pdgid: S056ZOT
text:
CHO 2000 use various electroweak data to constrain Z^' models assuming mass(H)=100 GeV. See Fig.2 for limits in general E(6)-motivated models.


pdgid: S056ZOT
text:
CHO 1998 study constraints on four-Fermi contact interactions obtained from low-energy electroweak experiments, assuming no Z-Z^' mixing.


pdgid: S056ZOT
text:
Search for Z^' decaying to dijets at sqrt(s)=1.8 TeV. For Z^' with electromagnetic strength coupling, no bound is obtained.


pdgid: S056ZLF
text:
CABARCAS 2024 use constraints on the non-standard neutrino interactions reported by ANTARES  and IceCube expreriments to constrain Z^' models with mu tau coupling.  See their Figs. 1  and 2 for limits in mass-coupling plane.


pdgid: S056ZLF
text:
AAD 2023CB search for a new particle with lepton-flavor violating decay in p p collisions  at sqrt(s) = 13 TeV. See their Figs.4, 5, and 6 for limits on .


pdgid: S056ZLF
text:
TUMASYAN 2023H search for a new particle with lepton-flavor violating decay in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 4 for limits on .


pdgid: S056ZLF
text:
AABOUD 2018CM search for a new particle with lepton-flavor violating decay in p p  collisions at sqrt(s) = 13 TeV. See their Figs. 4, 5, and 6 for limits on sigma B.


pdgid: S056ZLF
text:
SIRUNYAN 2018AT search for a narrow resonance Z^' decaying  into e mu in p p  collisions at sqrt(s) = 13 TeV. See their Fig.5 for limit on sigma.B in the  range of 600 GeV < M(Z^') < 5000 GeV.


pdgid: S056ZLF
text:
AABOUD 2016P search for new particle with lepton flavor violating decay in p p collisions  at sqrt(s) = 13 TeV. See their Figs.2, 3, and 4 for limits on sigma.B.


pdgid: S056ZLF
text:
KHACHATRYAN 2016BE search for new particle Z^' with lepton flavor violating decay in p p  collisions atsqrt(s) = 8 TeV in the range of 200 GeV < M(Z^')< 2000 GeV. See  their Fig.4 for limits on sigma.B and their Table 5 for bounds on various  masses.


pdgid: S056ZLF
text:
AAD 2015O search for new particle Z^' with lepton flavor violating decay in p p  collisions at sqrt(s) = 8 TeV in the range of 500 GeV < M(Z^') < 3000 GeV. See  their Fig. 2 for limits on sigmaB.


pdgid: S056ZLF
text:
AAD 2011H search for new particle Z^' with lepton flavor violating decay in p p  collisions at sqrt(s) = 7 TeV in the range of 700 GeV < M(Z^') < 1000 GeV. See  their Fig. 3 for limits on sigma.B.


pdgid: S056ZLF
text:
AAD 2011Z search for new particle Z^' with lepton flavor violating decay in p p  collisions at sqrt(s) = 7 TeV in the range 700 GeV < M(Z^') < 2000 GeV. See  their Fig. 3 for limits on sigma.B.


pdgid: S056ZLF
text:
ABULENCIA 2006M search for new particle Z^' with lepton flavor violating decay in p pbar  collisions at sqrt(s) = 1.96TeV in the range of 100 GeV < M(Z^') <  800 GeV. See their Fig.4 for limits in the mass-coupling plane.


pdgid: S056KKI
text:
MUECK 2002 limit is 2sigma and is from global electroweak fit ignoring correlations among observables.  Higgs is assumed to be confined on the brane and its mass is fixed.  For scenarios of bulk Higgs, of brane-SU(2)(L), bulk-U(1)(Y), and of bulk-SU(2)(L), brane-U(1)(Y), the corresponding limits are >4.6 TeV, >4.3 TeV and >3.0 TeV, respectively.


pdgid: S056KKI
text:
Bound is derived from limits on e nu q q^' contact interaction, using data from HERA and the Tevatron.


pdgid: S056KKI
text:
Bound holds only if first two generations of quarks lives on separate branes.  If quark mixing is not complex, then bound lowers to 400TeV from Deltamass(K).


pdgid: S056KKI
text:
See Figs.1 and 2 of DELGADO 2000 for several model variations. Special boundary conditions can be found which permit KK states down to 950GeV and that agree with the measurement of Q(W)(Cs).  Quoted bound assumes all Higgs bosons confined to brane; placing one Higgs doublet in the bulk lowers bound to 2.3TeV.


pdgid: S056KKI
text:
Bound is derived from global electroweak analysis assuming the Higgs field is trapped on the matter brane. If the Higgs propagates in the bulk, the bound increases to 3.8TeV.


pdgid: S056KKI
text:
Global electroweak analysis used to obtain bound independent of position of Higgs on brane or in bulk.


pdgid: S056KKI
text:
Bounds from effect of KK states on G(F), alpha, M(W), and M(Z).  Hard cutoff at string scale determined using gauge coupling unification.  Limits for d=2,3,4 rise to 3.5, 5.7, and 7.8 TeV.


pdgid: S056KKI
text:
Bound obtained for Higgs confined to the matter brane with mass(H)=500 GeV. For Higgs in the bulk, the bound increases to 3.5TeV.


pdgid: S056EGT
text:
AAD 2024AV search for scalar leptoquarks decaying to t e in p p collisions at  sqrt(s) = 13 TeV. See their Fig. 9 for exclusion limit on sigma.


pdgid: S056EGT
text:
AAD 2024AV search for scalar leptoquarks decaying to t mu in p p collisions at  sqrt(s) = 13 TeV. See their Fig. 9 for exclusion limit on sigma.


pdgid: S056EGT
text:
AAD 2024AV search for kappa = 1 vector leptoquarks decaying to t e in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 11 for exclusion limit on sigma. The limit  becomes M(LQ) > 1.67 TeV for minimal coupling vector LQ with kappa = 0.


pdgid: S056EGT
text:
AAD 2024AV search for kappa = 1 vector leptoquarks decaying to t mu in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 11 for exclusion limit on sigma. The limit  becomes M(LQ) > 1.67 TeV for minimal coupling vector LQ with kappa = 0.


pdgid: S056EGT
text:
AAD 2024O search for scalar leptoquarks decaying to b tau or t nu. See their Fig. 2a for  exclusion limit on M_{{LQ}} as function of B(b tau).


pdgid: S056EGT
text:
AAD 2024O search for scalar leptoquarks decaying to t tau or b nu. See their Fig. 2b for  exclusion limit on M_{{LQ}} as function of B(t tau).


pdgid: S056EGT
text:
AAD 2024O search for scalar leptoquarks decaying to b mu or t nu. See their Fig. 3a for exclusion  limit on M_{{LQ}} as function of B(b mu).


pdgid: S056EGT
text:
AAD 2024O search for scalar leptoquarks decaying to t mu or b nu. See their Fig.4 a for exclusion  limit on M_{{LQ}} as function of B(t mu).


pdgid: S056EGT
text:
AAD 2024O search for scalar leptoquarks decaying to b e or t nu. See their Fig. 3b for exclusion  limit on M_{{LQ}} as function of B(b e).


pdgid: S056EGT
text:
AAD 2024O search for scalar leptoquarks decaying to t e or b nu. See their Fig. 4b for exclusion  limit on M_{{LQ}} as function of B(t e).


pdgid: S056EGT
text:
AAD 2024O search for vector leptoquarks decaying to t nu or b tau with kappa = 1. The limit  becomes > 1580 GeV for kappa = 0.


pdgid: S056EGT
text:
AAD 2024O search for vector leptoquarks decaying to t nu or b mu with kappa = 1. The limit  becomes > 1710 GeV for kappa = 0.


pdgid: S056EGT
text:
AAD 2024O search for vector leptoquarks decaying to t nu or b e with kappa = 1. The limit  becomes > 1620 GeV for kappa = 0.


pdgid: S056EGT
text:
HAYRAPETYAN 2024O search for scalar leptoquarks decaying to b mu. See their Fig. 7 for  exclusion limit on leptoquark pair production cross section as function of M_{{LQ}}.


pdgid: S056EGT
text:
HAYRAPETYAN 2024O search for kappa = 1 vector leptoquarks decaying to b mu. The limit  becomes M_{{LQ}} > 2120 GeV for kappa = 0.


pdgid: S056EGT
text:
HAYRAPETYAN 2024Z search for scalar and vector leptoquarks decaying to b tau and produced through  single, pair, and nonresonantly in p p collisions at sqrt(s) = 13 TeV. The limit quoted above  assumes scalar leptoquarks with B(b tau) = 1 and leptoquark coupling strength lambda = 0. See  their Fig. 7 for limits in mass-coupling plane.


pdgid: S056EGT
text:
HAYRAPETYAN 2024Z search for scalar and vector leptoquarks decaying to b tau and produced through  single, pair, and nonresonantly in p p collisions at sqrt(s) = 13 TeV. The limit quoted above  assumes kappa = 1 vector leptoquarks with B(b tau) = 1 and leptoquark coupling strength  lambda = 0. See their Fig. 8 for limits in mass-coupling plane and for limits with kappa = 0.


pdgid: S056EGT
text:
AAD 2023BJ search for scalar leptoquarks decaying to c tau in p p collisions at  sqrt(s) = 13 TeV. See their Fig. 8 for exclusion limit on sigma as function of M_{{LQ}}.


pdgid: S056EGT
text:
AAD 2023CF search for scalar and vector leptoquarks decaying to b tau. The limit quoted  above is for scalar leptoquark. See their Fig. 9 for limits on leptoquark pair production cross  sections.


pdgid: S056EGT
text:
AAD 2023CF search for scalar and vector leptoquarks decaying to b tau. The limit quoted  above is for vector leptoquark with kappa = 1. The limit becomes M_{{LQ}} > 1650 for  vector leptoquark with kappa = 0. See their Fig. 9 for limits on leptoquark pair production  cross sections.


pdgid: S056EGT
text:
AAD 2023F search for scalar leptoquarks decaying to t nu and b mu in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 9 for exclusion contour in B(b mu)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2023F search for scalar leptoquarks decaying to t nu and b e in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 9 for exclusion contour in B(b e)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2023F search for scalar leptoquarks decaying to t mu and b nu in p p   collisions at sqrt(s) = 13 TeV. See their Fig. 9 for exclusion contour in B(t mu)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2023F search for scalar leptoquarks decaying to t e and b nu in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 9 for exclusion contour in B(t e)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2023F search for kappa = 1 (YM coupling) vector leptoquarks decaying  to t nu and  b mu in p p collisions at sqrt(s) = 13 TeV. If kappa = 0 (minimal  coupling) is  assumed, the  limit  becomes M_{{LQ}} > 1710 GeV. See their Fig. 10 for  exclusion contour in  B(b mu)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2023F search for kappa = 1 (YM coupling) vector leptoquarks decaying to t nu and  b e in p p collisions at sqrt(s) = 13 TeV. If kappa = 0 (minimal coupling) is assumed,  the limit   becomes M_{{LQ}} > 1620 GeV. See their Fig. 10 for exclusion contour in B(b e)-M_{{LQ}}  plane.


pdgid: S056EGT
text:
TUMASYAN 2022H search for scalar leptoquarks decaying to t e. See their Fig. 27 for  exclusion limit on leptoquark pair production cross section as function of M_{{LQ}}.


pdgid: S056EGT
text:
TUMASYAN 2022H search for scalar leptoquarks decaying to t mu. See their Fig. 27 for  exclusion limit on leptoquark pair production cross section as function of M_{{LQ}}.


pdgid: S056EGT
text:
TUMASYAN 2022H search for scalar leptoquarks decaying to t tau. See their Fig. 27 for  exclusion limit on leptoquark pair production cross section as function of M_{{LQ}}.


pdgid: S056EGT
text:
AAD 2021AG search for scalar leptoquarks decaying to t e. See their Fig. 6 for exclusion  limit on B(t e) as function of M_{{LQ}}.


pdgid: S056EGT
text:
AAD 2021AG search for scalar leptoquarks decaying to t mu. See their Fig. 6 for exclusion  limit on B(t mu) as function of M_{{LQ}}.


pdgid: S056EGT
text:
AAD 2021AW search for scalar leptoquarks decaying to b tau. See their Fig. 9 for  exclusion contour in B(b tau)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2021AW search for scalar leptoquarks decaying to t tau. See their Fig. 9 for  exclusion contour in B(t tau)-M_{{LQ}} plane.


pdgid: S056EGT
text:
AAD 2021AW search for kappa = 1 vector leptoquarks decaying to b tau. See their Fig.  10 for  exclusion contour in B(b tau)-M_{{LQ}} plane and for limit on kappa = 0  vector  leptoquarks.


pdgid: S056EGT
text:
AAD 2021S search for scalar leptoquarks decaying to b nu in p p collisions at  sqrt(s) = 13 TeV.  The limit above assumes B(b nu) = 1. For B(b nu) = 0.05, the limit  becomes 400 GeV.


pdgid: S056EGT
text:
AAD 2021T search for scalar leptoquarks decaying to t tau in p p collisions at   sqrt(s) = 13 TeV. The limit above assumes B(t tau) = 1. For B(t tau) = 0.5, the   limit becomes 1220 GeV. See their Fig. 15b for limits on B(t tau) as a function of  leptoquark mass.


pdgid: S056EGT
text:
SIRUNYAN 2021J search for scalar leptoquarks decaying to t tau and b nu in p p  collisions at sqrt(s) = 13 TeV.


pdgid: S056EGT
text:
SIRUNYAN 2021J search for vector leptoquarks decaying to t nu and b tau in p p   collisions at sqrt(s) = 13 TeV. The limit quoted above assumes kappa = 1. If we assume   kappa = 0, the limit  becomes M_{{LQ}} > 1290 GeV.


pdgid: S056EGT
text:
AAD 2020AK search for scalar leptoquarks decaying to e q, e b, e c, mu q,  mu b, mu c. The quoted limit assumes B(e q) = 1. See their Fig. 9 for limits on  B(e q), B(e b), B(e c), B(mu q), B(mu b), B(mu c) as a function  of leptoquark mass.


pdgid: S056EGT
text:
AAD 2020AK search for scalar leptoquarks decaying to e q, e b, e c, mu q,  mu b, mu c. The quoted limit assumes B(mu q) = 1. See their Fig. 9 for limits on  B(e q), B(e b), B(e c), B(mu q), B(mu b), B(mu c) as a function  of leptoquark mass.


pdgid: S056EGT
text:
SIRUNYAN 2020A search for scalar and vector leptoquarks decaying to t nu, b nu, and  q nu (q = u, d, s, c). The limit quoted above assumes scalar leptoquark  with B(nu b) = 1.


pdgid: S056EGT
text:
SIRUNYAN 2020A search for scalar and vector leptoquarks decaying to t nu, b nu, and  q nu (q = u, d, s, c). The limit quoted above assumes scalar leptoquark  with B(nu t) = 1.


pdgid: S056EGT
text:
SIRUNYAN 2020A search for scalar and vector leptoquarks decaying to t nu, b nu, and  q nu (q = u, d, s, c). The limit quoted above assumes scalar leptoquark  with B(nu q) = 1.


pdgid: S056EGT
text:
SIRUNYAN 2020A search for scalar and vector leptoquarks decaying to t nu, b nu, and  q nu (q = u, d, s, c). The limit quoted above assumes vector leptoquark  with B(nu b) = 1 and kappa = 1. If we assume kappa = 0, the limit becomes M_{{LQ}}  > 1560 GeV.


pdgid: S056EGT
text:
SIRUNYAN 2020A search for scalar and vector leptoquarks decaying to t nu, b nu, and  q nu (q = u, d, s, c). The limit quoted above assumes vector leptoquark  with B(nu t) = 1 and kappa = 1. If we assume kappa = 0, the limit becomes M_{{LQ}}  > 1475 GeV.


pdgid: S056EGT
text:
SIRUNYAN 2020A search for scalar and vector leptoquarks decaying to t nu, b nu, and  q nu (q = u, d, s, c). The limit quoted above assumes vector leptoquark  with B(nu q) = 1 and kappa = 1. If we assume kappa = 0, the limit becomes M_{{LQ}}  > 1560 GeV.


pdgid: S056EGT
text:
AABOUD 2019AX search for leptoquarks using e e j j events in p p collisions at  sqrt(s) = 13 TeV. The limit above assumes B(e q) = 1.


pdgid: S056EGT
text:
AABOUD 2019AX search for leptoquarks using mu mu j j events in p p collisions at  sqrt(s) = 13 TeV. The limit above assumes B(mu q) = 1.


pdgid: S056EGT
text:
AABOUD 2019X search for scalar leptoquarks decaying to b tau in p p collisions at  sqrt(s) = 13 TeV.


pdgid: S056EGT
text:
AABOUD 2019X search for scalar leptoquarks decaying to t tau in p p collisions at  sqrt(s) = 13 TeV.


pdgid: S056EGT
text:
SIRUNYAN 2019BI search for a pair of scalar leptoquarks decaying to mu mu j j and to  mu nu j j final states in p p collisions at sqrt(s) = 13 TeV. Limits are shown as a  function of beta where beta is the branching fraction to a muon and a quark. For beta =  1.0 (0.5) LQ masses up to 1530 (1285) GeV are excluded. See Fig. 9 for exclusion limits in the  plane of beta and LQ mass.


pdgid: S056EGT
text:
SIRUNYAN 2019BJ search for a pair of scalar leptoquarks decaying to e e j j and e nu j j final  states in p p collisions at sqrt(s) = 13 TeV. Limits are shown as a function of the branching  fraction beta to an electron and a quark. For beta = 1.0 (0.5) LQ masses up to 1435  (1270) GeV are excluded. See Fig. 9 for exclusion limits in the plane of beta and LQ mass.


pdgid: S056EGT
text:
SIRUNYAN 2019Y search for a pair of third generation scalar leptoquarks, each decaying to  tau and a jet. Assuming B(tau b) = 1, leptoquark masses below 1.02 TeV are excluded.


pdgid: S056EGT
text:
SIRUNYAN 2018CZ search for scalar leptoquarks decaying to tau t in p p collisions at  sqrt(s) = 13 TeV. The limit above assumes B(tau t) = 1.


pdgid: S056EGT
text:
SIRUNYAN 2018EC set limits for scalar and vector leptoquarks decaying to mu t, tau t,  and nu b. The limit quoted above assumes scalar leptoquark with B(mu t) = 1.


pdgid: S056EGT
text:
SIRUNYAN 2018EC set limits for scalar and vector leptoquarks decaying to mu t, tau t,  and nu b. The limit quoted above assumes vector leptoquark with all possible combinations of  branching fractions to mu t, tau t, and nu b.


pdgid: S056EGT
text:
SIRUNYAN 2018U set limits for scalar and vector leptoquarks decaying to t nu, b nu,  and q nu. The limit quoted above assumes scalar leptoquark with B(b nu) = 1. Vector  leptoquarks with kappa = 1 are excluded below masses of 1810 GeV.


pdgid: S056EGT
text:
SIRUNYAN 2018U set limits for scalar and vector leptoquarks decaying to t nu, b nu,  and q nu. The limit quoted above assumes scalar leptoquark with B(q nu) = 1. Vector  leptoquarks with kappa = 1 are excluded below masses of 1790 GeV.


pdgid: S056EGT
text:
SIRUNYAN 2018U set limits for scalar and vector leptoquarks decaying to t nu, b nu,  and q nu. The limit quoted above assumes scalar leptoquark with B(nu t) = 1. Vector  leptoquarks with kappa = 1 are excluded below masses of 1780 GeV.


pdgid: S056EGT
text:
SIRUNYAN 2018U set limits for scalar and vector leptoquarks decaying to t nu, b nu,  and q nu.  kappa = 1 and LQ --> b nu are assumed.


pdgid: S056EGT
text:
SIRUNYAN 2018U set limits for scalar and vector leptoquarks decaying to t nu, b nu,  and q nu. kappa = 1 and LQ --> q nu with q =  u,d,s,c are assumed.


pdgid: S056EGT
text:
SIRUNYAN 2018U set limits for scalar and vector leptoquarks decaying to t nu, b nu,  and q nu. kappa = 1 and LQ --> t nu are assumed.


pdgid: S056EGT
text:
KHACHATRYAN 2017J search for scalar leptoquarks decaying to tau b using p p  collisions at sqrt(s) = 13 TeV. The limit above assumes B(tau b) = 1.


pdgid: S056EGT
text:
SIRUNYAN 2017H search for scalar leptoquarks using tau tau b b events in p p  collisions at sqrt(s) = 8 TeV. The limit above assumes B(tau b) = 1.


pdgid: S056EGT
text:
AAD 2016G search for scalar leptoquarks using e e j j events in collisions at sqrt(s) = 8 TeV. The limit above assumes B(e q) = 1.


pdgid: S056EGT
text:
AAD 2016G search for scalar leptoquarks using mu mu j j events in collisions at sqrt(s) = 8 TeV. The limit above assumes B(mu q) = 1.


pdgid: S056EGT
text:
KHACHATRYAN 2016AF search for scalar leptoquarks using e e j j and e nu j j events in  p p collisions at sqrt(s) = 8 TeV. The limit above assumes B(e q)= 1. For B(e q) =  0.5, the limit becomes 850 GeV.


pdgid: S056EGT
text:
KHACHATRYAN 2016AF search for scalar leptoquarks using mu mu j j and mu nu j j events  in p p collisions at sqrt(s) = 8 TeV. The limit above assumes B(mu q) = 1. For B(mu q) =  0.5, the limit becomes 760 GeV.


pdgid: S056EGT
text:
KHACHATRYAN 2015AJ search for scalar leptoquarks using tau tau t t  events in p p collisions at sqrt(s) = 8 TeV. The limit above assumes B(tau t) = 1.


pdgid: S056EGT
text:
KHACHATRYAN 2014T search for scalar leptoquarks decaying to tau b using p p  collisions at sqrt(s) = 8 TeV. The limit above assumes B(tau b) = 1. See their Fig. 5 for  the exclusion limit as function of B(tau b).


pdgid: S056EGT
text:
SIRUNYAN 2019BC search for scalar leptoquark (LQ) pair production in p p collisions at  sqrt(s) = 13 TeV. One LQ is assumed to decay to mu q, while the other decays to dark matter  pair and SM particles. See their Fig. 4 for limits in  M(LQ)-M(DM) plane.


pdgid: S056EGT
text:
AAD 2013AE search for scalar leptoquarks using tau tau b b events in p p collisions at Ecm = 7TeV. The limit above assumes B(tau b) = 1.


pdgid: S056EGT
text:
CHATRCHYAN 2013M search for scalar and vector leptoquarks decaying to tau b in p p collisions at Ecm = 7 TeV. The limit above is for scalar leptoquarks with B(tau b) = 1.


pdgid: S056EGT
text:
AAD 2012H search for scalar leptoquarks using e e  j j and e nu j j events in p p collisions at Ecm = 7 TeV. The limit above assumes B(e q) = 1. For B(e q) = 0.5, the limit becomes 607 GeV.


pdgid: S056EGT
text:
AAD 2012O search for scalar leptoquarks using mu mu j j and mu nu j j events in p p collisions at Ecm = 7 TeV.  The limit above assumes B(mu q) = 1. For B(mu q) = 0.5, the limit becomes 594 GeV.


pdgid: S056EGT
text:
CHATRCHYAN 2012AG search for scalar leptoquarks using e e j j and e nu j j events in p p collisions at Ecm = 7 TeV.  The  limit above assumes B(e q) = 1. For B(e q) = 0.5, the limit becomes 640 GeV.


pdgid: S056EGT
text:
CHATRCHYAN 2012AG search for scalar leptoquarks using mu mu j j and mu nu j j events in p p collisions at Ecm = 7 TeV.  The  limit above assumes B(mu q) = 1. For B(mu q) = 0.5, the limit becomes 650 GeV.


pdgid: S056EGT
text:
CHATRCHYAN 2012BO search for scalar leptoquarks decaying to  nu b in p p collisions at sqrt(s) = 7 TeV.  The limit above assumes B(nu b) = 1.


pdgid: S056EGT
text:
AAD 2011D search for scalar leptoquarks using e e j j and e nu j j events in p p collisions  at Ecm = 7 TeV.The limit above assumes B(e q) = 1. For B(e q) = 0.5, the limit becomes 319 GeV.


pdgid: S056EGT
text:
AAD 2011D search for scalar leptoquarks using mu mu j j and mu nu j j events in p p collisions at Ecm = 7 TeV. The limit above assumes B(mu q) = 1. For B(mu q) = 0.5, the limit becomes 362 GeV.


pdgid: S056EGT
text:
ABAZOV 2011V search for scalar leptoquarks using e nu j j events in p pbar collisions at Ecm = 1.96 TeV. The limit above assumes B(e q) = 0.5.


pdgid: S056EGT
text:
CHATRCHYAN 2011N search for scalar leptoquarks using e nu j j events in p p collisions at Ecm = 7 TeV.  The limit above assumes B(e q) = 0.5.


pdgid: S056EGT
text:
KHACHATRYAN 2011D search for scalar leptoquarks using e e j j events in p p collisions at Ecm = 7 TeV. The limit above assumes B(e q) = 1.


pdgid: S056EGT
text:
KHACHATRYAN 2011E search for scalar leptoquarks using mu mu j j events in p p collisions at Ecm = 7 TeV.  The limit above assumes B(mu q) = 1.


pdgid: S056EGT
text:
ABAZOV 2010L search for pair productions of scalar leptoquark state decaying to nu b in p pbar collisions at Ecm = 1.96 TeV. The limit above assumes B(nu b) = 1.


pdgid: S056EGT
text:
ABAZOV 2009 search for scalar leptoquarks using mu mu j j and mu nu j j events in p pbar collisions at Ecm = 1.96 TeV. The limit above assumes B(mu q) = 1. For B(mu q) = 0.5, the limit becomes 270 GeV.


pdgid: S056EGT
text:
ABAZOV 2009AF search for scalar leptoquarks using e e j j and e nu j j events in p pbar collisions at Ecm = 1.96 TeV. The limit above assumes B(e q) = 1. For B(e q) = 0.5 the bound becomes 284 GeV.


pdgid: S056EGT
text:
AALTONEN 2008P search for vector leptoquarks using tau+ tau- b bbar events in p pbar collisions at Ecm = 1.96 TeV. Assuming Yang-Mills (minimal) couplings, the mass limit is >317 GeV (251 GeV) at 95% CL for B(tau b) = 1.


pdgid: S056EGT
text:
Search for pair production of scalar leptoquark state decaying to tau b in p pbar collisions at Ecm= 1.96 TeV. The limit above assumes B(tau b) = 1.


pdgid: S056EGT
text:
Search for scalar leptoquarks using nu nu j j events in pbar p collisions at Ecm = 1.96 TeV. The limit above assumes B(nu q) = 1.


pdgid: S056EGT
text:
ABAZOV 2007J search for pair productions of scalar leptoquark state decaying to nu b in p pbar collisions at Ecm = 1.96 TeV. The limit above assumes B(nu b) = 1.


pdgid: S056EGT
text:
ABAZOV 2006A search for scalar leptoquarks using mu mu j j events in p pbar collisions at Ecm = 1.8 TeV and 1.96 TeV.  The limit above assumes B(mu q) = 1.  For B(mu q) = 0.5, the limit becomes 204 GeV.


pdgid: S056EGT
text:
ABAZOV 2006L search for scalar leptoquarks using nu nu j j events in p pbar collisions at Ecm = 1.8TeV and at 1.96TeV. The limit above assumes B(nu q) = 1.


pdgid: S056EGT
text:
ABULENCIA 2006T search for scalar leptoquarks using mu mu j j, mu nu j j, and nu nu j j events in p pbar collisions at Ecm = 1.96TeV. The quoted limit assumes B(mu q) = 1. For B(mu q) = 0.5 or 0.1, the bound becomes 208GeV or 143GeV, respectively. See their Fig.4 for the exclusion limit as a function of B(mu q).


pdgid: S056EGT
text:
ABAZOV 2005H search for scalar leptoquarks using e e j j and e nu j j events in pbar p collisions at Ecm = 1.8 TeV and 1.96 TeV. The limit above assumes B(e q) = 1.  For B(e q) = 0.5 the bound becomes 234 GeV.


pdgid: S056EGT
text:
ACOSTA 2005P search for scalar leptoquarks using e e j j, e nu j j events in pbar p collisions at Ecm = 1.96TeV. The limit above assumes B(e q) = 1. For B(e q) = 0.5 and 0.1, the bound becomes 205 GeV and  145 GeV, respectively.


pdgid: S056EGT
text:
ABBIENDI 2003R search for scalar/vector leptoquarks in e+ e- collisions at sqrt(s) = 189 -- 209 GeV. The quoted limits are for charge -4/3 isospin 0 scalar-leptoquark with B(lepton q) = 1. See their table 12 for other cases.


pdgid: S056EGT
text:
ABAZOV 2002 search for scalar leptoquarks using nu nu j j events in pbar p collisions at Ecm=1.8 TeV.  The bound holds for all leptoquark generations. Vector leptoquarks are likewise constrained to lie above 200 GeV.


pdgid: S056EGT
text:
ABAZOV 2001D search for scalar leptoquarks using e nu j j, e e j j, and nu nu j j events in p pbar collisions at Ecm=1.8 TeV.  The limit above assumes B(e q)=1. For B(e q)=0.5 and 0, the bound becomes 204 and 79GeV, respectively. Bounds for vector leptoquarks are also given. Supersedes ABBOTT 1998E.


pdgid: S056EGT
text:
ABBIENDI 2000M search for scalar/vector leptoquarks in e+ e- collisions at sqrt(s)=183 GeV.  The quoted limits are for charge -4/3 isospin0 scalar-leptoquarks with B(lepton q)=1.  See their Table8 and Figs.6 -- 9 for other cases.


pdgid: S056EGT
text:
ABBOTT 2000C search for scalar leptoquarks using mu mu j j, mu nu j j, and nu nu j j events in p pbar collisions at Ecm=1.8 TeV.  The limit above assumes B(mu q)=1. For B(mu q)=0.5 and 0, the bound becomes 180 and 79 GeV respectively.  Bounds for vector leptoquarks are also given.


pdgid: S056EGT
text:
AFFOLDER 2000K search for scalar leptoquark using nu nu c c events in p pbar collisions at Ecm=1.8TeV. The quoted limit assumes B(nu c)=1. Bounds for vector leptoquarks are also given.


pdgid: S056EGT
text:
AFFOLDER 2000K search for scalar leptoquark using nu nu b b events in p pbar collisions at Ecm=1.8TeV. The quoted limit assumes B(nu b)=1. Bounds for vector leptoquarks are also given.


pdgid: S056EGT
text:
ABBOTT 1999J search for leptoquarks using mu nu j j events in p pbar collisions at Ecm= 1.8TeV.  The quoted limit is for a scalar leptoquark with B(mu q) = B(nu q) = 0.5. Limits on vector leptoquarks range from 240 to 290 GeV.


pdgid: S056EGT
text:
ABBOTT 1998E search for scalar leptoquarks using e nu j j, e e j j, and nu nu j j events in p pbar collisions at Ecm=1.8 TeV. The limit above assumes B(e q)=1. For B(e q)=0.5 and 0, the bound becomes 204 and 79 GeV, respectively.


pdgid: S056EGT
text:
ABBOTT 1998J search for charge -1/3 third generation scalar and vector leptoquarks in p pbar collisions at Ecm= 1.8 TeV. The quoted limit is for scalar leptoquark with B(nu b)=1.


pdgid: S056EGT
text:
ABE 1998S search for scalar leptoquarks using mu mu j j events in p pbar collisions at Ecm= 1.8TeV. The limit is for B(mu q)= 1.  For B(mu q)=B(nu q)=0.5, the limit is >160 GeV.


pdgid: S056EGT
text:
GROSS-PILCHER 1998 is the combined limit of the CDF and D0 Collaborations as determined by a joint CDF/D0 working group and reported in this FNAL Technical Memo.  Original data published in ABE 1997X and ABBOTT 1998E.


pdgid: S056EGT
text:
ABE 1997F search for third generation scalar and vector leptoquarks in p pbar collisions at Ecm = 1.8 TeV.  The quoted limit is for scalar leptoquark with B(tau b) = 1.


pdgid: S056EGT
text:
ABE 1997X search for scalar leptoquarks using e e j j events in p pbar collisions at Ecm=1.8 TeV. The limit is for B(e q)=1.


pdgid: S056EGT
text:
First and second generation leptoquarks are assumed to be degenerate.  The limit is slightly lower for each generation.


pdgid: S056EGT
text:
Limits are for charge -1/3, isospin-0 scalar leptoquarks decaying to lepton- q or nu q with any branching ratio.  See paper for limits for other charge-isospin assignments of leptoquarks.


pdgid: S056EGT
text:
KIM 1990 assume pair production of charge 2/3 scalar-leptoquark via photon exchange.  The decay of the first (second) generation leptoquark is assumed to be any mixture of d e+ and u nubar (s mu+ and c nubar). See paper for limits for specific branching ratios.


pdgid: S056EGT
text:
BARTEL 1987B limit is valid when a pair of charge 2/3 spinless leptoquarks X is produced with point coupling, and when they decay under the constraint B(X --> c nubar_mu) + B(X --> s mu+) = 1.


pdgid: S056EGT
text:
BEHREND 1986B assumed that a charge 2/3 spinless leptoquark, chi, decays either into s mu+ or c nubar:  B(chi --> s mu+) + B(chi --> c nubar) = 1.


pdgid: S056ESP
text:
HAYRAPETYAN 2024C search for single production of scalar leptoquarks decaying to q tau+  (q = u ,d , s , b) in p p collisions at sqrt(s) = 13 TeV. The limit quoted above is  for a leptoquark produced in tau u collisions and the leptoquark coupling strength lambda =  1.  See their Fig. 4 for limits in mass-coupling plane.


pdgid: S056ESP
text:
HAYRAPETYAN 2024C search for single production of scalar leptoquarks decaying to q tau+   (q = u ,d , s , b) in p p collisions at sqrt(s) = 13 TeV.  The limit quoted above is  for a leptoquark produced in tau d collisions and the leptoquark coupling strength lambda =  1. See their Fig. 4 for limits in mass-coupling plane.


pdgid: S056ESP
text:
HAYRAPETYAN 2024Z search for scalar and vector leptoquarks decaying to b tau and produced  through single, pair, and nonresonantly in p p collisions at sqrt(s) = 13 TeV. The limit  quoted above is derived solely from single production limit and assumes scalar leptoquark decaying  to b tau. The leptoquark coupling strength lambda = 1 is assumed. See their Fig. 7 and Fig.  8 for combined limits in mass-coupling plane.


pdgid: S056ESP
text:
AAD 2023BZ search for single production of charge 4/3 scalar leptoquarks decaying to b tau-, and  charge 2/3 vector leptoquarks decaying to bbar tau- in p p collisions at sqrt(s) = 13 TeV.  The limit quoted above assumes a scalar leptoquark with B(b tau) = 1 and the leptoquark  coupling strength lambda = 1.0.  The limit becomes M_{{LQ}} > 1530 GeV for lambda =  2.5.


pdgid: S056ESP
text:
SIRUNYAN 2021J search for single production of charge -1/3 scalar leptoquarks decaying   to t tau- and b nu, and charge 2/3 vector leptoquarks decaying to t nu and b tau+   in p p collisions at sqrt(s) = 13 TeV. The limit quoted above assumes a scalar leptoquark with   B(t tau) = B(b nu) = 0.5 and the leptoquark coupling strength lambda = 1.5. The   limit becomes M_{{LQ}} > 750 GeV for lambda = 2.5.


pdgid: S056ESP
text:
SIRUNYAN 2018BJ search for single production of charge 2/3 scalar leptoquarks decaying to  tau b in p p collisions at sqrt(s) = 13 TeV. The limit above assumes B(tau b) = 1  and the leptoquark coupling strength lambda = 1.


pdgid: S056ESP
text:
KHACHATRYAN 2016AG search for single production of charge +-1/3 scalar leptoquarks  using e e j events in p p collisions at sqrt(s) = 8 TeV. The limit above assumes B(e q) = 1  and the leptoquark coupling strength lambda = 1.


pdgid: S056ESP
text:
KHACHATRYAN 2016AG search for single production of charge +-1/3 scalar leptoquarks  using mu mu j events  in p p collisions at sqrt(s) = 8 TeV. The limit above assumes  B(mu q) = 1 and the leptoquark coupling strength lambda = 1.


pdgid: S056ESP
text:
ABRAMOWICZ 2012A limit is for a scalar, weak isoscalar, charge -1/3 leptoquark  coupled with e_{{R}}. See their Figs. 12 -- 17 and Table 4 for states with different quantum numbers.


pdgid: S056ESP
text:
Limit from single production in Z decay. The limit is for a leptoquark coupling of electromagnetic strength and assumes B(lepton q) = 2/3. The limit is 77 GeV if first and second leptoquarks are degenerate.


pdgid: S056ESP
text:
AAD 2022E leptoquarks decaying both to u e- and c mu- are constrained from the  comparison of the  production cross sections for e+ mu- and e- mu+ in p p collisions at  sqrt(s) = 13 TeV.  Scalar leptoquarks with M(LQ) < 1880 GeV are excluded for  g^eu =  g**mu c = 1.


pdgid: S056ESP
text:
TUMASYAN 2021D search for energetic jets + notET events in p p collisions at  sqrt(s) = 13 TeV. The branching fraction for the decay of the leptoquark into an electron neutrino  and up quark is assumed to be 100% (beta = 0). See their Fig. 12 for exclusion limits  in mass-coupling plane.


pdgid: S056ESP
text:
DEY 2016 use the 2010-2012 IceCube PeV energy data set to  constrain the leptoquark  production cross section through the nu q --> LQ --> nu q process. See their Figure 4  for the exclusion limit in the mass-coupling plane.


pdgid: S056ESP
text:
AARON 2011A search for various leptoquarks with lepton-flavor violating couplings.  See their Figs.2 -- 3 and Tables1 -- 4 for detailed limits.


pdgid: S056ESP
text:
The quoted limit is for a scalar, weak isoscalar, charge -1/3 leptoquark coupled with e_{{R}}. See  their Figs. 3 -- 5 for limits on states with different quantum numbers.


pdgid: S056ESP
text:
ABAZOV 2007E search for leptoquark single production through q g fusion process in p pbar collisions. See their Fig. 4 for exclusion plot in mass-coupling plane.


pdgid: S056ESP
text:
AKTAS 2005B limit is for a scalar, weak isoscalar, charge -1/3 leptoquark coupled with e_{{R}}. See their Fig. 3 for limits on states with different quantum numbers.


pdgid: S056ESP
text:
CHEKANOV 2005 search for various leptoquarks with lepton-flavor violating couplings. See their Figs.6--10 and Tables 1--8 for detailed limits.


pdgid: S056ESP
text:
CHEKANOV 2003B limit is for a scalar, weak isoscalar, charge -1/3 leptoquark coupled with e_{{R}}.  See their Figs.11 -- 12 and Table5 for limits on states with different quantum numbers.


pdgid: S056ESP
text:
For limits on states with different quantum numbers and the limits in the mass-coupling plane, see their Fig.4 and Fig.5.


pdgid: S056ESP
text:
CHEKANOV 2002 search for various leptoquarks with lepton-flavor violating couplings.  See their Figs.6 -- 7 and Tables5 -- 6 for detailed limits.


pdgid: S056ESP
text:
For limits on states with different quantum numbers and the limits in the mass-coupling plane, see their Fig.3.


pdgid: S056ESP
text:
BREITWEG 2000E search for F=0 leptoquarks in e+ p collisions. For limits in mass-coupling plane, see their Fig.11.


pdgid: S056ESP
text:
ABREU 1999G limit obtained from process e gamma --> LQ+q. For limits on vector and scalar states with different quantum numbers and the limits in the coupling-mass plane, see their Fig.4 and Table2.


pdgid: S056ESP
text:
For limits on states with different quantum numbers and the limits in the mass-coupling plane, see their Fig.13 and Fig.14. ADLOFF 1999 also search for leptoquarks with lepton-flavor violating couplings. ADLOFF 1999 supersedes AID 1996B.


pdgid: S056ESP
text:
DERRICK 1997 search for various leptoquarks with lepton-flavor violating couplings.  See their Figs.5--8 and Table1 for detailed limits.


pdgid: S056ESP
text:
DERRICK 1993 search for single leptoquark production in e p collisions with the decay e q and nu q. The limit is for leptoquark coupling of electromagnetic strength and assumes B(e q) = B(nu q) = 1/2. The limit for B(e q) = 1 is 176 GeV. For limits on states with different quantum numbers, see their Table3.


pdgid: S056LQI
text:
AAD 2024W search for leptoquark induced mu tau q t (q = u, c) contact  interaction in p p collisions at sqrt(s) = 13 TeV. See their Fig. 7b for limits in  mass-coupling plane.


pdgid: S056LQI
text:
CALABRESE 2023 obtain limits on leptoquark coupling from coherent nu-nucleus scattering  data  collected by COHERENT experiment. See their Fig. 3 for limits in mass-coupling plane.


pdgid: S056LQI
text:
TUMASYAN 2023AW search for tau nu events mediated by t-channel leptoquark exchange in  p p collisions at sqrt(s) = 13 TeV. See their Fig. 10 for limits in mass-coupling plane.


pdgid: S056LQI
text:
TUMASYAN 2023S search for leptoquark induced b bbar --> tau+ tau- process in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 12 for limits on a vector b tau leptoquark in  mass-coupling plane.


pdgid: S056LQI
text:
CRIVELLIN 2021A set limits on coupling strengths of scalar and vector leptoquarks using K --> pi nu nu, K --> pi e+ e-,    K0-Kbar0 and D0-Dbar0 mixings, and weak neutral current measurements.   See  their Fig. 2 and Fig. 3 for the limits in mass-coupling plane.


pdgid: S056LQI
text:
AEBISCHER 2020 explain the B decay anomalies using four-fermion operator Wilson  coefficents. See their Table 1. These Wilson coefficients may be generated by a U_{{1}} vector  leptoquark with U_{{1}} transforming as (3,1)(2/3) under the SM gauge group. See their Figures  6, 7, 8 for the regions of the LQ parameter space which explains the B anomalies and avoids the  indirect low energy constraints.


pdgid: S056LQI
text:
DEPPISCH 2020 limits on the lepton-number-violating higher-dimensional-operators are derived  from K --> pi nu nu in the standard model effective field theory. These  higher-dimensional-operators may be induced from leptoquark-exchange diagrams.


pdgid: S056LQI
text:
ABRAMOWICZ 2019 obtain a limit on lambda/M_{{LQ}} > 1.16 TeV**-1 for weak  isotriplet spin-0 leptoquark S_{{1}}^L. We obtain the limit quoted above by converting the limit on  lambda/M_{{LQ}} for S_{{1}}^L assuming lambda = sqrt(4 pi). See their  Table 5 for the limits of leptoquarks with different quantum numbers. These limits are derived from  bounds of e q contact interactions.


pdgid: S056LQI
text:
MANDAL 2019 give bounds on leptoquarks from  tau-decays, leptonic dipole moments,  lepton-flavor-violating processes, and K decays.


pdgid: S056LQI
text:
ZHANG 2018A give bounds on leptoquark induced four-fermion interactions from D --> K lepton nu. The authors inform us that the shape parameter of the vector form factor in both the abstract and  the conclusions of ZHANG 2018A should be r(+1) = 2.16+-0.07 rather than  +-0.007. The numbers listed in their Table 7 are correct.


pdgid: S056LQI
text:
BARRANCO 2016 give bounds on leptoquark induced four-fermion interactions from D --> K lepton nu  and D_s --> lepton nu.


pdgid: S056LQI
text:
KUMAR 2016 gives bound on SU(2) singlet scalar leptoquark with chrge -1/3 from  K0-Kbar0 mixing, K --> pi nu nubar, K0L --> mu+ mu-, and K0L --> mu+- e-+  decays.


pdgid: S056LQI
text:
BESSAA 2015 obtain limit on leptoquark induced four-fermion interactions from the ATLAS and CMS limit on the  qbar q ebar e  contact interactions.


pdgid: S056LQI
text:
SAHOO 2015A obtain limit on leptoquark induced four-fermion interactions from B_s,d --> mu+ mu- for lambda ~ O(1).


pdgid: S056LQI
text:
SAKAKI 2013 explain the B --> D^(*)() tau nubar anomaly using Wilson coefficients of leptoquark-induced four-fermion operators.


pdgid: S056LQI
text:
KOSNIK 2012 obtains limits on leptoquark induced four-fermion interactions from b --> s lepton+ lepton- decays.


pdgid: S056LQI
text:
AARON 2011C limit is for weak isotriplet spin-0 leptoquark at strong coupling lambda = sqrt(4pi). For the limits of leptoquarks with different quantum numbers, see their Table 3. Limits are derived from bounds of e q contact intereractions.


pdgid: S056LQI
text:
DORSNER 2011 give bounds on scalar, weak singlet, charge 4/3 leptoquark from K, B, tau decays, meson mixings, LFV, g-2 and Z --> b bbar.


pdgid: S056LQI
text:
AKTAS 2007A search for lepton-flavor violation in e p collision. See their Tables 4 -- 7 for limits on lepton-flavor violating four-fermion interactions induced by various leptoquarks.


pdgid: S056LQI
text:
SCHAEL 2007A limit is for the weak-isoscalar spin-0 left-handed leptoquark with the coupling of electromagnetic strength. For the limits of leptoquarks with different quantum numbers, see their Table 35.


pdgid: S056LQI
text:
SMIRNOV 2007 obtains mass limits for the vector and scalar chiral leptoquark states from K --> e mu, B --> e tau decays.


pdgid: S056LQI
text:
ADLOFF 2003 limit is for the weak isotriplet spin-0 leptoquark at strong coupling lambda=sqrt(4pi). For the limits of leptoquarks with different quantum numbers, see their Table3. Limits are derived from bounds on e+- q contact interactions.


pdgid: S056LQI
text:
CHEKANOV 2002 search for lepton-flavor violation in e p collisions. See their Tables1 -- 4 for limits on lepton-flavor violating and four-fermion interactions induced by various leptoquarks.


pdgid: S056LQI
text:
CHEUNG 2001B quoted limit is for a scalar, weak isoscalar, charge -1/3 leptoquark with a coupling of electromagnetic strength. The limit is derived from bounds on contact interactions in a global electroweak analysis. For the limits of leptoquarks with different quantum numbers, see Table5.


pdgid: S056LQI
text:
ACCIARRI 2000P limit is for the weak isoscalar spin-0 leptoquark with the coupling of electromagnetic strength. For the limits of leptoquarks with different quantum numbers, see their Table4.


pdgid: S056LQI
text:
ADLOFF 2000 limit is for the weak isotriplet spin-0 leptoquark at strong coupling, lambda=sqrt(4pi). For the limits of leptoquarks with different quantum numbers, see their Table2. ADLOFF 2000 limits are from the Q**2 spectrum measurement of e+ p --> e+ X.


pdgid: S056LQI
text:
BARATE 2000I search for deviations in cross section and jet-charge asymmetry in e+ e- --> qbar q due to t-channel exchange of a leptoquark at sqrt(s)=130 to 183 GeV. Limits for other scalar and vector leptoquarks are also given in their Table22.


pdgid: S056LQI
text:
BARGER 2000 explain the deviation of atomic parity violation in cesium atoms from prediction is explained by scalar leptoquark exchange.


pdgid: S056LQI
text:
ZARNECKI 2000 limit is derived from data of HERA, LEP, and Tevatron and from various low-energy data including atomic parity violation. Leptoquark coupling with electromagnetic strength is assumed.


pdgid: S056LQI
text:
ABBIENDI 1999 limits are from e+ e- --> q qbar cross section at 130 -- 136, 161 -- 172, 183 GeV. See their Fig.8 and Fig.9 for limits in mass-coupling plane.


pdgid: S056LQI
text:
ABE 1998V quoted limit is from B(B_s --> e+- mu-+)<8.2E-6. ABE 1998V also obtain a similar limit on M(LQ)>20.4 TeV from B(B_d --> e+- mu-+)<4.5E-6. Both bounds assume the non-canonical association of the bquark with electrons or muons under SU(4).


pdgid: S056LQI
text:
ACCIARRI 1998J limit is from e+ e- --> q qbar cross section at sqrt(s)= 130 -- 172 GeV which can be affected by the t-and u-channel exchanges of leptoquarks. See their Fig.4 and Fig.5 for limits in the mass-coupling plane.


pdgid: S056LQI
text:
ACKERSTAFF 1998V limits are from e+ e- --> q qbar and e+ e- --> b bbar cross sections at sqrt(s) = 130 -- 172 GeV, which can be affected by the t- and u-channel exchanges of leptoquarks. See their Fig.21 and Fig.22 for limits of leptoquarks in mass-coupling plane.


pdgid: S056LQI
text:
DEANDREA 1997 limit is for Rtilde_{{2}} leptoquark obtained from atomic parity violation (APV). The coupling of leptoquark is assumed to be electromagnetic strength. See Table2 for limits of the four-fermion interactions induced by various scalar leptoquark exchange. DEANDREA 1997 combines APV limit and limits from Tevatron and HERA. See Fig.1 -- 4 for combined limits of leptoquark in mass-coupling plane.


pdgid: S056LQI
text:
DERRICK 1997 search for lepton-flavor violation in e p collision. See their Tables2--5 for limits on lepton-flavor violating four-fermion interactions induced by various leptoquarks.


pdgid: S056LQI
text:
GROSSMAN 1997 estimate the upper bounds on the branching fraction B --> tau+ tau- (X) from the absence of the B decay with large missing energy. These bounds can be used to constrain leptoquark induced four-fermion interactions.


pdgid: S056LQI
text:
JADACH 1997 limit is from e+ e- --> q qbar cross section at sqrt(s)=172.3 GeV which can be affected by the t- and u-channel exchanges of leptoquarks. See their Fig.1 for limits on vector leptoquarks in mass-coupling plane.


pdgid: S056LQI
text:
KUZNETSOV 1995B use pi, K, B, tau decays and mu e conversion and give a list of bounds on the leptoquark mass and the fermion mixing matrix in the Pati-Salam model. The quoted limit is from K_L --> mu e decay assuming zero mixing.


pdgid: S056LQI
text:
MIZUKOSHI 1995 calculate the one-loop radiative correction to the Z-physics parameters in various scalar leptoquark models. See their Fig.4 for the exclusion plot of third generation leptoquark models in mass-coupling plane.


pdgid: S056LQI
text:
BHATTACHARYYA 1994 limit is from one-loop radiative correction to the leptonic decay width of the Z. mass(H)=250 GeV, alpha_{{s}}(mass(Z))=0.12, mass(t)=180 GeV, and the electroweak strength of leptoquark coupling are assumed. For leptoquark coupled to ebar_L t_R, mubar t, and taubar t, see Fig.2 in BHATTACHARYYA 1994B erratum and Fig.3.


pdgid: S056LQI
text:
DAVIDSON 1994 gives an extensive list of the bounds on leptoquark-induced four-fermion interactions from pi, K, D, B, mu, tau decays and meson mixings, etc. See Table15 of DAVIDSON 1994 for detail.


pdgid: S056LQI
text:
KUZNETSOV 1994 gives mixing independent bound of the Pati-Salam leptoquark from the cosmological limit on pi0 --> nubar nu.


pdgid: S056LQI
text:
LEURER 1994, LEURER 1994B limits are obtained from atomic parity violation and apply to any chiral leptoquark which couples to the first generation with electromagnetic strength. For a nonchiral leptoquark, universality in pi(lepton2) decay provides a much more stringent bound.


pdgid: S056LQI
text:
MAHANTA 1994 gives bounds of P- and T-violating scalar-leptoquark couplings from atomic and molecular experiments.


pdgid: S056LQI
text:
From (pi --> e nu)/(pi --> mu nu) ratio. SHANKER 1982 assumes the leptoquark induced four-fermion coupling 4g**2/M**2 (nubar(eL) u(R)) (dbar_L e_R)with g=0.004 for spin-0 leptoquark and g**2/M**2 (nubar(eL) gamma_mu u_L) (dbar_{{R}} gamma^mu e_R) with g~=0.6 for spin-1 leptoquark.


pdgid: S056DQ
text:
ABREU 1994O limit is from e+ e- --> cbar sbar c s. Range extends up to 43 GeV if diquarks are degenerate in mass.


pdgid: S056AXG
text:
KHACHATRYAN 2017Y search for pair production of color-octet gauge boson g_{{A}} each decaying  to 4j in p p collisions at sqrt(s) = 8 TeV.


pdgid: S056AXG
text:
AAD 2016W search for a new resonance decaying to a pair of b and B_{{H}} in p p  collisions at sqrt(s) = 8 TeV. The vector-like quark B_{{H}} is assumed to decay to . See  their Fig. 3 and Fig. 4 for limits on sigma.B.


pdgid: S056AXG
text:
KHACHATRYAN 2015AV search for pair productions of neutral color-octet weak-triplet scalar  particles (Theta0), decaying to b bbar, Z g or gamma g, in p p collisions at  sqrt(s) = 8 TeV. The Theta0 particle is often predicted in coloron (G^', color-octet gauge  boson) models and appear in the p p collisions through G^' --> Theta0 Theta0 decays.  Assuming B(Theta0 --> b bbar) = 0.5, they give limits mass(Theta0) > 623 GeV (426 GeV)  for mass(G^') = 2.3 mass(Theta0) (mass(G^') = 5 mass(Theta0)).


pdgid: S056AXG
text:
AALTONEN 2013R search for new resonance decaying to sigma sigma, with hypothetical strongly  interacting sigma particle subsequently decaying to 2 jets, in p pbar collisions at sqrt(s) = 1.96 TeV, using data corresponding to an integrated luminosity of 6.6 fb**-1. For 50 GeV < mass(sigma) < mass(g_{{A}}())/2, axigluons in mass range 150 -- 400 GeV are excluded.


pdgid: S056AXG
text:
CHATRCHYAN 2013AU search for the pair produced color-octet vector bosons decaying to q qbar pairs in p p collisions. The quoted limit is for B(g_A --> q qbar) = 1.


pdgid: S056AXG
text:
ABAZOV 2012R search for massive color octet vector particle decaying to t tbar. The quoted limit assumes g_{{A}} couplings with light quarks are suppressed by 0.2.


pdgid: S056AXG
text:
AALTONEN 2010L search for massive color octet non-chiral vector particle decaying into t tbar pair with mass in the range 400 GeV < M < 800 GeV. See their Fig.6 for limit in the mass-coupling plane.


pdgid: S056AXG
text:
DONCHESKI 1998 compare alpha(s) derived from low-energy data and that from Gamma(Z --> hadrons)/Gamma(Z --> leptons).


pdgid: S056AXG
text:
ABE 1990H assumes Gamma(g_{{A}}) = Nalpha_{{s}}mass(g_{{A}})/6 with N = 5(Gamma(g_{{A}}) = 0.09mass(g_{{A}})). For N = 10, the excluded region is reduced to 120-150 GeV.


pdgid: S056AXG
text:
ROBINETT 1989 result demands partial-wave unitarity of J = 0 t tbar --> t tbar scattering amplitude and derives a limit mass(g_{{A}}) > 0.5 mass(t).  Assumes mass(t) > 56 GeV.


pdgid: S056AXG
text:
ALBAJAR 1988B result is from the nonobservation of a peak in two-jet invariant mass distribution. Gamma(g_{{A}}) < 0.4 mass(g_{{A}}) assumed. See also BAGGER 1988.


pdgid: S056AXG
text:
CUYPERS 1988 requires Gamma(Upsilon --> g g_A)<Gamma(Upsilon --> g g g ). A similar result is obtained by DONCHESKI 1988.


pdgid: S056AXG
text:
DONCHESKI 1988B requires Gamma(Upsilon --> g q qbar)/Gamma(Upsilon --> g g g ) < 0.25, where the former decay proceeds via axigluon exchange.  A more conservative estimate of < 0.5 leads to mass(g_{{A}}) > 21 GeV.


pdgid: S056COS
text:
SIRUNYAN 2020AI search for resonances decaying into  dijets in p p collisions at sqrt(s)  = 13 TeV. The limit above assumes S_{{8gg}} coupling k_{{s}}^2 = 1/2.


pdgid: S056COS
text:
SIRUNYAN 2018BO search for color octet scalar boson produced  through gluon fusion process in  p p collisions at sqrt(s) = 13 TeV. The limit above assumes S_{{8gg}} coupling k_{{s}}^2 = 1/2.


pdgid: S056COS
text:
KHACHATRYAN 2015AV search for pair productions of neutral color-octet weak-triplet scalar  particles (Theta0), decaying to b bbar, Z g or gamma g, in p p collisions at    sqrt(s) = 8 TeV. The Theta0 particle is often predicted in coloron (G^', color-octet  gauge boson) models and appear in the p p collisions through G^' --> Theta0 Theta0 decays.  Assuming B(Theta0 --> b bbar) = 0.5, they give limits mass(Theta0) > 623 GeV (426 GeV) for mass(G^') = 2.3 mass(Theta0) (mass(G^') = 5 mass(Theta0)).


pdgid: S056COS
text:
AAD 2013K search for pair production of color-octet scalar particles in p p collisions at sqrt(s) = 7 TeV. Cross section limits are interpreted as mass limits on scalar partners of a Dirac gluino.


pdgid: S056ZXG
text:
RAINBOLT 2019 limits are from B(Z --> lepton+ lepton- lepton+ lepton-). See their Figs.  5 and 6 for  limits in mass-coupling plane.


pdgid: S056ZXG
text:
SIRUNYAN 2019AZ search for p p --> Z --> X0 mu+ mu- --> mu+ mu- mu+ mu- events in p p  collisions at sqrt(s) = 13 TeV. See their Fig. 5 for limits on CS(p p --> X0 mu+ mu-).B(X0 --> mu+ mu-).


pdgid: S056ZXG
text:
BARATE 1998U obtain limits on B(Z --> gamma X0)B(X0 --> lepton leptonbar ,  q qbar ,  g g ,  gamma gamma , nu nubar). See their Fig.17.


pdgid: S056ZXG
text:
See Fig.4 of ACCIARRI 1997Q for the upper limit on B(Z --> gamma X0; E(gamma)>E(min)) as a function of E(min).


pdgid: S056ZXG
text:
ACTON 1993E give sigma(e+ e- --> X0 gamma).B(X0 --> gamma gamma)<0.4pb (95%CL) for mass(X0)=60+-2.5 GeV.  If the process occurs via s-channel gamma exchange, the limit translates to Gamma(X0).B(X0 --> gamma gamma)**2<20 MeV for mass(X0) = 60+-1 GeV.


pdgid: S056ZXG
text:
ABREU 1992D give sigma_{{Z}} . B(Z --> gamma X0) . B(X0 --> hadrons) <(3 -- 10)pb for mass(X0) = 10 -- 78 GeV.  A very similar limit is obtained for spin-1 X0.


pdgid: S056ZXG
text:
ADRIANI 1992F search for isolated gamma in hadronic Z decays.  The limit sigma_{{Z}} . B(Z --> gamma X0) . B(X0 --> hadrons) <(2 -- 10)pb (95%CL) is given for mass(X0) = 25 -- 85 GeV.


pdgid: S056ZXG
text:
ACTON 1991 searches for Z --> Z^* X0, Z^* --> e+ e-, mu+ mu-, or nu nubar. Excludes any new scalar X0 with mass(X0)<9.5 GeV/c if  it has the same coupling to Z Z^* as the MSM Higgs boson.


pdgid: S056ZXG
text:
AKRAWY 1990J give Gamma(Z --> gamma X0).B(X0 --> hadrons) <1.9 MeV (95%CL) for mass(X0) = 32 -- 80 GeV. We divide by Gamma(Z) = 2.5 GeV to get product of branching ratios. For nonresonant transitions, the limit is B(Z --> gamma q qbar) <8.2 MeV assuming three-body phase space distribution.


pdgid: S056HEE
text:
ODAKA 1989 looked for a narrow or wide scalar resonance in e+ e- --> hadrons at Ecm = 55.0-60.8 GeV.


pdgid: S056HEE
text:
DERRICK 1986 found no deviation from the Standard Model Bhabha scattering at Ecm= 29 GeV and set limits on the possible scalar boson e+ e- coupling.  See their figure 4 for excluded region in the Gamma(X0 --> e+ e-)-mass(X0) plane.  Electronic chiral invariance requires a parity doublet of X0, in which case the limit applies for Gamma(X0 --> e+ e-) = 3 MeV.


pdgid: S056HEE
text:
ADEVA 1985 first limit is from 2gamma, mu+ mu-, hadrons assuming X0 is a scalar.  Second limit is from e+ e- channel. Ecm = 40-47 GeV.  Supersedes ADEVA 1984.


