# pdgreference

document_id: AAIJ 2023BB
publication_name: PRL 131 151801
doi: 10.1103/PhysRevLett.131.151801
inspire_id: 2633007
title:
Measurement of the $\Lambda_{b}^{0}\to \Lambda(1520) \mu^{+}\mu^{-}$ differential branching fraction


document_id: AAIJ 2020AB
publication_name: PR D102 051101
doi: 10.1103/PhysRevD.102.051101
inspire_id: 1773072
title:
Search for $C\!P$ violation and observation of $P$ violation in $\Lambda_b^0 \to p \pi^- \pi^+ \pi^-$ decays


document_id: AAIJ 2018AG
publication_name: JHEP 1808 039
doi: 10.1007/JHEP08(2018)039
inspire_id: 1672471
title:
Search for CP violation using triple product asymmetries in $\Lambda^{0}_{b}\to pK^{-}\pi^{+}\pi^{-}$, $\Lambda^{0}_{b}\to pK^{-}K^{+}K^{-}$ and $\Xi^{0}_{b}\to pK^{-}K^{-}\pi^{+}$ decays


document_id: AAIJ 2013AG
publication_name: PL B724 27
doi: 10.1016/j.physletb.2013.05.041
inspire_id: 1220792
title:
Measurements of the Lambda_b()0 --> J/psi Lambda Decay Amplitudes and the Lambda_{{b}}()0 Polarisation in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2014L
publication_name: PR D89 092009
doi: 10.1103/PhysRevD.89.092009
inspire_id: 1288490
title:
Measurement of the Parity-Violating Asymmetry Parameter alpha(b) and the Helicity Amplitudes for the Decay Lambda_b()0 --> J/psi + Lambda0 with the ATLAS Detector


document_id: SIRUNYAN 2018R
publication_name: PR D97 072010
doi: 10.1103/PhysRevD.97.072010
inspire_id: 1654926
title:
Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV


document_id: ABAZOV 2015I
publication_name: PR D91 072008
doi: 10.1103/PhysRevD.91.072008
inspire_id: 1352125
title:
Measurement of the Forward-Backward Asymmetry in Lambda_{{b}}()0 and Lambdabar_{{b}}()0 Baryon Production in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAIJ 2018AP
publication_name: JHEP 1809 146
doi: 10.1007/JHEP09(2018)146
inspire_id: 1684712
title:
Angular moments of the decay $\Lambda_b^0 \rightarrow \Lambda \mu^{+} \mu^{-}$ at low hadronic recoil


document_id: AAIJ 2018AO
publication_name: JHEP 1809 145 (errat.)
doi: 10.1007/JHEP09(2018)145
inspire_id: 1355377
title:
Differential branching fraction and angular analysis of $\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-$ decays


document_id: AAIJ 2021AJ
publication_name: JHEP 2110 060
doi: 10.1007/JHEP10(2021)060
inspire_id: 1888216
title:
Observation of a $\Lambda_b^0-\overline{\Lambda}_b^0$ production asymmetry in proton-proton collisions at $\sqrt{s} = 7 \textrm{ and } 8\,\textrm{TeV}$


document_id: SIRUNYAN 2020K
publication_name: PL B803 135345
doi: 10.1016/j.physletb.2020.135345
inspire_id: 1776599
title:
Study of excited $\Lambda_\mathrm{b}^0$ states decaying to $\Lambda_\mathrm{b}^0\pi^+\pi^-$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAIJ 2020Q
publication_name: JHEP 2006 136
doi: 10.1007/JHEP06(2020)136
inspire_id: 1779848
title:
Observation of a new baryon state in the $ {\Lambda}_{\mathrm{b}}^0{\pi}^{+}{\pi}^{-} $ mass spectrum


document_id: AAIJ 2019A
publication_name: PRL 122 012001
doi: 10.1103/PhysRevLett.122.012001
inspire_id: 1694807
title:
Observation of two resonances in the $\Lambda_b^0 \pi^\pm$ systems and precise measurement of $\Sigma_b^\pm$ and $\Sigma_b^{*\pm}$ properties


document_id: AALTONEN 2009AP
publication_name: PR D80 072003
doi: 10.1103/PhysRevD.80.072003
inspire_id: 820851
title:
Observation of the Omega_{{b}}()- Baryon and Measurement of the Properties of the Xi_{{b}}()- and Omega_{{b}}()- Baryons


document_id: HAYRAPETYAN 2024R
publication_name: PR D110 012002
doi: 10.1103/PhysRevD.110.012002
inspire_id: 2762139
title:
Observation of the $\Xi^-_\mathrm{b}$$\to$$\psi$(2S)$\Xi^-$ decay and studies of the $\Xi_\mathrm{b}^{\ast{}0}$ baryon in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: AAIJ 2020U
publication_name: PRL 124 111802
doi: 10.1103/PhysRevLett.124.111802
inspire_id: 1768478
title:
Isospin amplitudes in $\Lambda_b^0\to J/\psi \Lambda(\Sigma^0)$ and $\Xi_b^0\to J/\psi \Xi^0(\Lambda)$ decays


document_id: AAIJ 2023BD
publication_name: PR D108 052008
doi: 10.1103/PhysRevD.108.052008
inspire_id: 2662328
title:
Measurement of the mass difference and relative production rate of the $\Omega^-_b$ and $\Xi^-_b$ baryons


document_id: ABBIENDI 1999L
publication_name: EPJ C9 1
doi: 10.1007/s100520050508
inspire_id: 480942
title:
A Measurement of the Product Branching Ratio f(b --> Lambda_b) * B(Lambda_b --> Lambda X) in Z0 Decays


document_id: AAIJ 2019W
publication_name: PRL 122 222001
doi: 10.1103/PhysRevLett.122.222001
inspire_id: 1728691
title:
Observation of a narrow pentaquark state, $P_c(4312)^+$, and of two-peak structure of the $P_c(4450)^+$


document_id: AAIJ 2022H
publication_name: PRL 128 062001
doi: 10.1103/PhysRevLett.128.062001
inspire_id: 1903743
title:
Evidence for a new structure in the $J/\psi p$ and $J/\psi \bar{p}$ systems in $B_s^0 \to J/\psi p \bar{p}$ decays


document_id: AAIJ 2015P
publication_name: PRL 115 072001
doi: 10.1103/PhysRevLett.115.072001
inspire_id: 1382595
title:
Observation of J/psip Resonances Consistent with Pentaquark States in Lambda_b()0 --> J/psi K- p Decays


document_id: ZRELOV 1976
publication_name: CZJP B26 1306
doi: 10.1007/BF01589843
inspire_id: 90229
title:
Search for the Dirac Monopole over the Vavilov-Cherenkov Radiation using the 70 GeV IHEP Proton Synchrotron


document_id: KALBFLEISCH 2004
publication_name: PR D69 052002
doi: 10.1103/PhysRevD.69.052002
inspire_id: 621725
title:
Limits on Production of Magnetic Monopoles Utilizing Samples from the D0 and CDF Detectors at the Tevatron


document_id: AAD 2016AB
publication_name: PR D93 052009
doi: 10.1103/PhysRevD.93.052009
inspire_id: 1395092
title:
Search for Magnetic Monopoles and Stable Particles with High Electric Charges in 8 TeV pp Collisions with the ATLAS Detector


document_id: ACHARYA 2016
publication_name: JHEP 1608 067
doi: 10.1007/JHEP08(2016)067
inspire_id: 1451639
title:
Search for Magnetic Monopoles with the MoEDAL Prototype Trapping Detector in 8 TeV Proton-Proton Collisions at the LHC


document_id: ACHARYA 2017
publication_name: PRL 118 061801
doi: 10.1103/PhysRevLett.118.061801
inspire_id: 1499483
title:
Search for Magnetic Monopoles with the MoEDAL Forward Trapping Detector in 13 TeV Proton-Proton Collisions at the LHC


document_id: ACHARYA 2018A
publication_name: PL B782 510
doi: 10.1016/j.physletb.2018.05.069
inspire_id: 1645247
title:
Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb$^{-1}$ of 13 TeV proton-proton collisions at the LHC


document_id: ACHARYA 2019B
publication_name: PRL 123 021802
doi: 10.1103/PhysRevLett.123.021802
inspire_id: 1725935
title:
Magnetic Monopole Search with the Full MoEDAL Trapping Detector in 13 TeV pp Collisions Interpreted in Photon-Fusion and Drell-Yan Production


document_id: AAD 2020G
publication_name: PRL 124 031802
doi: 10.1103/PhysRevLett.124.031802
inspire_id: 1736730
title:
Search for Magnetic Monopoles and Stable High-Electric-Charge Objects in 13 Tev Proton-Proton Collisions with the ATLAS Detector


document_id: ACHARYA 2022A
publication_name: EPJ C82 694
doi: 10.1140/epjc/s10052-022-10608-2
inspire_id: 1988975
title:
Search for highly-ionizing particles in $pp$ collisions at the LHC’s Run-1 using the prototype MoEDAL detector


document_id: AAD 2023CO
publication_name: JHEP 2311 112
doi: 10.1007/JHEP11(2023)112
inspire_id: 2686746
title:
Search for magnetic monopoles and stable particles with high electric charges in $\sqrt{s}=$13 TeV $pp$ collisions with the ATLAS detector


document_id: BERMON 1985
publication_name: PRL 55 1850
doi: 10.1103/PhysRevLett.55.1850
inspire_id: 221933
title:
Flux Limit of Cosmic Ray Magnetic Monopoles from a Fully Coincident Superconducting Induction Detector


document_id: KAJINO 1984
publication_name: PRL 52 1373
doi: 10.1103/PhysRevLett.52.1373
inspire_id: 204272
title:
First Results from a Search for Magnetic Monopoles by a Detector Utilizing the Drell Mechanism and the Penning Effect


document_id: ANDERSON 1983
publication_name: PR D28 2308
doi: 10.1103/PhysRevD.28.2308
inspire_id: 191203
title:
Possible Evidence for Magnetic Monopole Interactions: Anomalous Long Range Alpha Particle Tracks Deep Underground


document_id: BARISH 1987
publication_name: PR D36 2641
doi: 10.1103/PhysRevD.36.2641
inspire_id: 22122
title:
Search for Grand Unification Monopoles and Other Ionizing Heavy Particles Using a Scintillation at the Earth's Surface


document_id: BERMON 1990
publication_name: PRL 64 839
doi: 10.1103/PhysRevLett.64.839
inspire_id: 305239
title:
New Limit Set on Cosmic-Ray Monopole Flux by a Large-Area Superconducting Magnetic-Induction Detector


document_id: HUBER 1990
publication_name: PRL 64 835
doi: 10.1103/PhysRevLett.64.835
inspire_id: 305238
title:
Limit on the Flux of Cosmic-Ray Magnetic Monopoles from Operation of an Eight-Loop Superconducting Detector


document_id: KOLB 1984
publication_name: APJ 286 702
doi: 10.1086/162645
inspire_id: 200685
title:
Limits from the Soft X-ray Background on the Temperature of old Neutron Stars and on the Flux of Superheavy Magnetic Monopoles


document_id: CABRERA 1975
publication_name: Thesis
title:
The use of Superconducting Shields for Generating Ultra-Low Magnetic Field Regions - and Several Related Experiments


document_id: KOVALIK 1986
publication_name: PR A33 1183
doi: 10.1103/PhysRevA.33.1183
inspire_id: 244522
title:
New Superconducting Quantum Interface Device Based Constraints on the Abundance of Magnetic Monopoles Trapped in Matter: An Investigation of Deeply Buried Rocks


document_id: HIDAKA 1991
publication_name: PR D44 927
doi: 10.1103/PhysRevD.44.927
inspire_id: 314970
title:
Absolute Mass Limits of the Gaugino-Higgsino Sector in the Minimal Supersymmetric Model from Data from the CERN Collider LEP and the Fermilab Tevatron


document_id: ALEXANDER 1996J
publication_name: PL B377 181
doi: 10.1016/0370-2693(96)00301-2
inspire_id: 416354
title:
Search for Chargino and Neutralino Production using the OPAL Detector at sqrt(s) = 130-136 GeV at LEP


document_id: ABREU 1996O
publication_name: PL B387 651
doi: 10.1016/0370-2693(96)01197-5
inspire_id: 421994
title:
Search for Neutralinos, Scalar Leptons and Scalar Quarks in e+ e- Interactions at sqrt(s) = 130 and 136 GeV


document_id: ABBOTT 1998C
publication_name: PRL 80 1591
doi: 10.1103/PhysRevLett.80.1591
inspire_id: 443294
title:
Search for the Trilepton Signature from the Associated Production of SUSY Chargino**+- Neutralino Gauginos


document_id: BARATE 1998S
publication_name: EPJ C4 433
doi: 10.1007/s100520050218
inspire_id: 452178
title:
Search for Supersymmetry with a Dominant R-Parity Violating LLEbar Coupling in e+ e- Collisions at Centre-of-Mass Energies of 130 to 172 GeV


document_id: BARATE 1999E
publication_name: EPJ C7 383
doi: 10.1007/s100529901086
inspire_id: 477807
title:
Search for Supersymmetry with a Dominant R Parity Violating LQ Dbar Coupling in e+ e- Collisions at Center-of-Mass Energies of 130 to 172 GeV


document_id: BARATE 1999P
publication_name: EPJ C11 193
doi: 10.1007/s100520050627
inspire_id: 495805
title:
Search for Charginos and Neutralinos in e+ e- Collisions at Ecm near 183 GeV and Constraints on the MSSM Parameter Space


document_id: BARATE 2001
publication_name: PL B499 67
doi: 10.1016/S0370-2693(01)00015-6
inspire_id: 536904
title:
Search for Supersymmetric Particles in e+ e- Collisions at sqrt(s) up to 202 GeV and Mass Limit for the Lightest Neutralino


document_id: ABDALLAH 2003M
publication_name: EPJ C31 421
doi: 10.1140/epjc/s2003-01355-5
inspire_id: 632738
title:
Searches for Supersymmetric Particles in e+ e- Collisions up to 208 GeV and Interpretation of the Results within the MSSM


document_id: HEISTER 2004
publication_name: PL B583 247
doi: 10.1016/j.physletb.2003.12.066
inspire_id: 635850
title:
Absolute Mass Lower Limit for the Lightest Neutralino of the MSSM from e+ e- Data at sqrt(s) up to 209 GeV


document_id: AAD 2014K
publication_name: PR D90 012004
doi: 10.1103/PhysRevD.90.012004
inspire_id: 1288061
title:
Search for Dark Matter in Events with a Z Boson and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2021AX
publication_name: PR D104 112010
doi: 10.1103/PhysRevD.104.112010
inspire_id: 1906174
title:
Search for charginos and neutralinos in final states with two boosted hadronically decaying bosons and missing transverse momentum in $pp$ collisions at $\sqrt {s}$ = 13  TeV with the ATLAS detector


document_id: AAD 2021BF
publication_name: EPJ C81 1023
doi: 10.1140/epjc/s10052-021-09761-x
inspire_id: 1869040
title:
Search for R-parity-violating supersymmetry in a final state containing leptons and many jets with the ATLAS experiment using $\sqrt{s} = 13 { TeV}$ proton–proton collision data


document_id: TUMASYAN 2022S
publication_name: JHEP 2204 147
doi: 10.1007/JHEP04(2022)147
inspire_id: 1872976
title:
Search for electroweak production of charginos and neutralinos in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: TUMASYAN 2022V
publication_name: JHEP 2205 014
doi: 10.1007/JHEP05(2022)014
inspire_id: 2009652
title:
Search for higgsinos decaying to two Higgs bosons and missing transverse momentum in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: AAD 2023CP
publication_name: JHEP 2311 150
doi: 10.1007/JHEP11(2023)150
inspire_id: 2660233
title:
Search for direct production of winos and higgsinos in events with two same-charge leptons or three leptons in $pp$ collision data at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: AAD 2024Z
publication_name: JHEP 2402 107
doi: 10.1007/JHEP02(2024)107
inspire_id: 2673888
title:
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector


document_id: ABDO 2010
publication_name: JCAP 1004 014
doi: 10.1088/1475-7516/2010/04/014
inspire_id: 846536
title:
Constraints on Cosmological Dark Matter Annihilation from the Fermi-LAT Isotopic Diffuse gamma-ray Measurement


document_id: BOLIEV 2013
publication_name: JCAP 1309 019
doi: 10.1088/1475-7516/2013/09/019
inspire_id: 1209500
title:
Search for Muon Signal from Dark Matter Annihilations in the Sun with the Baksan Underground Scintillator Telescope for 24.12 Years


document_id: CHOI 2015
publication_name: PRL 114 141301
doi: 10.1103/PhysRevLett.114.141301
inspire_id: 1353118
title:
Search for Neutrinos from Annihilation of Captured Low-Mass Dark Matter Particles in the Sun by Super-Kamiokande


document_id: BUCKLEY 2015
publication_name: PR D91 102001
doi: 10.1103/PhysRevD.91.102001
inspire_id: 1342903
title:
Search for Gamma-ray Emission from Dark Matter Annihilation in the Large Magellanic Cloud with the Fermi Large Area Telescope


document_id: ACKERMANN 2015
publication_name: PR D91 122002
doi: 10.1103/PhysRevD.91.122002
inspire_id: 1373872
title:
Updated Search for Spectral Lines from Galactic Dark Matter Interactions with Pass 8 Data from the Fermi Large Area Telescope


document_id: ABRAMOWSKI 2015
publication_name: PRL 114 081301
doi: 10.1103/PhysRevLett.114.081301
inspire_id: 1343968
title:
Constraints on an Annihilation Signal from a Core of Constant Dark Matter Density around the Milky Way Center with H.E.S.S.


document_id: ACKERMANN 2015A
publication_name: JCAP 1509 008
doi: 10.1088/1475-7516/2015/09/008
inspire_id: 1340670
title:
Limits on Dark Matter Annihilation Signals from the Fermi LAT 4-year Measurement of the Isotropic Gamma-Ray Background


document_id: ACKERMANN 2015B
publication_name: PRL 115 231301
doi: 10.1103/PhysRevLett.115.231301
inspire_id: 1351193
title:
Searching for Dark Matter Annihilation from Milky Way Dwarf Spheroidal Galaxies with Six Years of Fermi Large Area Telescope Data


document_id: ABDALLAH 2016
publication_name: PRL 117 111301
doi: 10.1103/PhysRevLett.117.111301
inspire_id: 1478165
title:
Search for Dark Matter Annihilations Towards the Inner Galactic Halo from 10 Years of Observations with H.E.S.S


document_id: AVRORIN 2016
publication_name: ASP 81 12
doi: 10.1016/j.astropartphys.2016.04.004
inspire_id: 1407939
title:
A Search for Neutrino Signal from Dark Matter Annihilation in the Center of the Milky Way with Baikal NT200


document_id: AHNEN 2016
publication_name: JCAP 1602 039
doi: 10.1088/1475-7516/2016/02/039
inspire_id: 1416788
title:
Limits to Dark Matter Annihilation Cross-Section from a Combined Analysis of MAGIC and Fermi-LAT Observations of Dwarf Satellite Galaxies


document_id: AARTSEN 2016C
publication_name: JCAP 1604 022
doi: 10.1088/1475-7516/2016/04/022
inspire_id: 1413075
title:
Improved Limits on Dark Matter Annihilation in the Sun with the 79-string IceCube Detector and Implications for Supersymmetry


document_id: ABDALLAH 2016A
publication_name: PRL 117 151302
doi: 10.1103/PhysRevLett.117.151302
inspire_id: 1488060
title:
H.E.S.S. Limits on Linelike Dark Matter Signatures in the 100 GeV to 2 TeV Energy Range Close to the Galactic Center


document_id: AARTSEN 2016D
publication_name: EPJ C76 531
doi: 10.1140/epjc/s10052-016-4375-3
inspire_id: 1466608
title:
All-flavour Search for Neutrinos from Dark Matter Annihilations in the Milky Way with IceCube/DeepCore


document_id: ALBERT 2017A
publication_name: PL B769 249
doi: 10.1016/j.physletb.2017.03.063
inspire_id: 1503367
title:
Results from the Search for Dark Matter in the Milky Way with 9 Years of Data of the ANTARES Neutrino Telescope


document_id: AARTSEN 2017C
publication_name: EPJ C77 627
doi: 10.1140/epjc/s10052-017-5213-y
inspire_id: 1600987
title:
Search for Neutrinos from Dark Matter Self-Annihilations in the Center of the Milky Way with 3 Years of IceCube/DeepCore


document_id: ABDALLAH 2018
publication_name: PRL 120 201101
doi: 10.1103/PhysRevLett.120.201101
inspire_id: 1673261
title:
Search for $\gamma$-Ray Line Signals from Dark Matter Annihilations in the Inner Galactic Halo from 10 Years of Observations with H.E.S.S.


document_id: ALBERT 2018B
publication_name: JCAP 1806 043
doi: 10.1088/1475-7516/2018/06/043
inspire_id: 1665613
title:
Search for Dark Matter Gamma-ray Emission from the Andromeda Galaxy with the High-Altitude Water Cherenkov Observatory


document_id: ALBERT 2018C
publication_name: PR D98 123012
doi: 10.1103/PhysRevD.98.123012
inspire_id: 1688671
title:
Constraints on Spin-Dependent Dark Matter Scattering with Long-Lived Mediators from TeV Observations of the Sun with HAWC


document_id: DI-MAURO 2019
publication_name: PR D99 123027
doi: 10.1103/PhysRevD.99.123027
inspire_id: 1731263
title:
Search for $\gamma$-ray emission from dark matter particle interactions from Andromeda and Triangulum Galaxies with the Fermi Large Area Telescope


document_id: ALBERT 2020
publication_name: PR D101 103001
doi: 10.1103/PhysRevD.101.103001
inspire_id: 1770426
title:
Search for gamma-ray spectral lines from dark matter annihilation in dwarf galaxies with the High-Altitude Water Cherenkov observatory


document_id: HOOF 2020
publication_name: JCAP 2002 012
doi: 10.1088/1475-7516/2020/02/012
inspire_id: 1709795
title:
A Global Analysis of Dark Matter Signals from 27 Dwarf Spheroidal Galaxies using 11 Years of Fermi-LAT Observations


document_id: ABDALLAH 2020
publication_name: PR D102 062001
doi: 10.1103/PhysRevD.102.062001
inspire_id: 1809922
title:
Search for dark matter signals towards a selection of recently detected DES dwarf galaxy satellites of the Milky Way with H.E.S.S.


document_id: ABE 2020G
publication_name: PR D102 072002
doi: 10.1103/PhysRevD.102.072002
inspire_id: 1795075
title:
Indirect search for dark matter from the Galactic Center and halo with the Super-Kamiokande detector


document_id: ALBERT 2020C
publication_name: PR D102 082002
doi: 10.1103/PhysRevD.102.082002
inspire_id: 1785680
title:
Combined search for neutrinos from dark matter self-annihilation in the Galactic Center with ANTARES and IceCube


document_id: ABDALLAH 2021
publication_name: PR D103 102002
doi: 10.1103/PhysRevD.103.102002
inspire_id: 1862747
title:
Search for dark matter annihilation in the Wolf-Lundmark-Melotte dwarf irregular galaxy with H.E.S.S.


document_id: ABE 2023B
publication_name: PRL 130 061002
doi: 10.1103/PhysRevLett.130.061002
inspire_id: 2616525
title:
Search for Gamma-Ray Spectral Lines from Dark Matter Annihilation up to 100 TeV toward the Galactic Center with MAGIC


document_id: GUO 2023A
publication_name: PR D108 043001
doi: 10.1103/PhysRevD.108.043001
inspire_id: 2665922
title:
Searching for dark-matter induced neutrino signals in dwarf spheroidal galaxies using 10 years of IceCube public data


document_id: MCDANIEL 2024
publication_name: PR D109 063024
doi: 10.1103/PhysRevD.109.063024
inspire_id: 2720512
title:
Legacy Analysis of Dark Matter Annihilation from the Milky Way Dwarf Spheroidal Galaxies with 14 Years of Fermi-LAT Data


document_id: BERNABEI 1997
publication_name: ASP 7 73
doi: 10.1016/S0927-6505(97)00003-0
inspire_id: 457927
title:
Improved Limits on WIMP-F19 Elastic Scattering and First Limit on the 2EC2nuCa40 Decay by using a Low Radioactive CaF(2)(Eu) Scintillator


document_id: BELLI 1999C
publication_name: NP B563 97
doi: 10.1016/S0550-3213(99)00618-5
inspire_id: 514228
title:
New Limits on Spin Dependent Coupled WIMPs and on 2beta Processes in Ca40 and Ca46 by using Low Radioactive CaF-2 (Eu) Crystal Scintillators


document_id: SPOONER 2000
publication_name: PL B473 330
doi: 10.1016/S0370-2693(99)01476-8
inspire_id: 526524
title:
NaI Dark Matter Limits and the NAIAD Array - a Detector with Improved Sensitivity to WIMPs using Unencapsulated NaI


document_id: TAKEDA 2003
publication_name: PL B572 145
doi: 10.1016/j.physletb.2003.07.090
inspire_id: 621442
title:
Limits on the WIMP-Nucleon Coupling Coefficients from Dark Matter Search Experiment with NaF Bolometer


document_id: LEE 2007A
publication_name: PRL 99 091301
doi: 10.1103/PhysRevLett.99.091301
inspire_id: 747779
title:
Limits on Interactions between Weakly Interacting Massive Particles and Nucleons Obtained with CsI(Tl) Crystal Detectors


document_id: LEBEDENKO 2009A
publication_name: PRL 103 151302
doi: 10.1103/PhysRevLett.103.151302
inspire_id: 812072
title:
Limits on the Spin-Dependent WIMP-Nucleon Cross Sections from the First Science Run of the ZEPLIN-III Experiment


document_id: KIM 2012
publication_name: PRL 108 181301
doi: 10.1103/PhysRevLett.108.181301
inspire_id: 1110777
title:
New Limits on Interactions between Weakly Interacting Massive Particles and Nucleons Obtained with CsI(Tl) Crystal Detectors


document_id: BEHNKE 2012
publication_name: PR D86 052001
doi: 10.1103/PhysRevD.86.052001
inspire_id: 1110911
title:
First Dark Matter Search Results from a 4-kg CF(3)I Bubble Chamber Operated in a Deep Underground Site


document_id: AKERIB 2016A
publication_name: PRL 116 161302
doi: 10.1103/PhysRevLett.116.161302
inspire_id: 1420704
title:
Results on the Spin-Dependent Scattering of Weakly Interacting Massive Particles on Nucleons from the Run 3 Data of the LUX Experiment


document_id: FU 2017
publication_name: PRL 118 071301
doi: 10.1103/PhysRevLett.118.071301
inspire_id: 1499474
title:
Spin-Dependent Weakly-Interacting-Massive-Particle-Nucleon Cross Section Limits from First Data of PandaX-II Experiment


document_id: HUANG 2022
publication_name: PL B834 137487
doi: 10.1016/j.physletb.2022.137487
inspire_id: 2133222
title:
Constraints on the axial-vector and pseudo-scalar mediated WIMP-nucleus interactions from PandaX-4T experiment


document_id: ARMENGAUD 2011
publication_name: PL B702 329
doi: 10.1016/j.physletb.2011.07.034
inspire_id: 893203
title:
Final Results of the EDELWEISS-II WIMP Search using a 4-kg Array of Cryogenic Germanium Detectors with Interleaved Electrodes


document_id: BERNABEI 2000
publication_name: PL B480 23
doi: 10.1016/S0370-2693(00)00405-6
inspire_id: 524173
title:
Search for WIMP Annual Modulation Signature: Result from DAMA/NAI-3 and DAMA/NAI-4 and the Global Combined Analysis


document_id: KIM 2002B
publication_name: JHEP 0212 034
doi: 10.1088/1126-6708/2002/12/034
inspire_id: 592141
title:
Upper and Lower Limits on Neutralino WIMP Mass and Spin Independent Scattering Cross Section, and Impact of New (g-2)((mu) Measurement


document_id: ANGLOHER 2005
publication_name: ASP 23 325
doi: 10.1016/j.astropartphys.2005.01.006
inspire_id: 655556
title:
Limits on WIMP Dark Matter using Scintillating CaWO(4) Cryogenic Detectors with Active Background Suppression


document_id: AKERIB 2005
publication_name: PR D72 052009
doi: 10.1103/PhysRevD.72.052009
inspire_id: 686953
title:
Exclusion Limits on the WIMP-Nucleon Cross Section from the First Run of the Cryogenic Dark Matter Search in the Soudan Underground Laboratory


document_id: AKERIB 2006A
publication_name: PRL 96 011302
doi: 10.1103/PhysRevLett.96.011302
inspire_id: 691711
title:
Limits on Spin-Independent Interactions of Weakly Interacting Massive Particles with Nucleons from the Two-Tower Run of the Cryogenic Dark Matter Search


document_id: ALNER 2007A
publication_name: ASP 28 287
doi: 10.1016/j.astropartphys.2007.06.002
inspire_id: 743428
title:
First Limits on WIMP Nuclear Recoil Signals in ZEPLIN-II: A Two-Phase Xenon Detector for Dark Matter Detection


document_id: BENETTI 2008
publication_name: ASP 28 495
doi: 10.1016/j.astropartphys.2007.08.002
inspire_id: 742079
title:
First Results from a Dark Matter Search with Liquid Argon at 87 K in the Gran Sasso Underground Laboratory


document_id: AHMED 2009
publication_name: PRL 102 011301
doi: 10.1103/PhysRevLett.102.011301
inspire_id: 780247
title:
Search for Weakly Interacting Massive Particles with the First Five-Tower Data from the Cryogenic Dark Matter Search at the Soudan Underground Laboratory


document_id: BUCHMUELLER 2009
publication_name: EPJ C64 391
doi: 10.1140/epjc/s10052-009-1159-z
inspire_id: 827593
title:
Likelihood Functions for Supersymmetric Observables in Frequentist Analyses of the CMSSM (constrained MSSM) and NUHM1 (non-universal Higgs masses)


document_id: ARMENGAUD 2010
publication_name: PL B687 294
doi: 10.1016/j.physletb.2010.03.057
inspire_id: 838959
title:
First Results of the EDELWEISS-II WIMP Search using Ge Cryogenic Detectors with Interleaved Electrodes


document_id: CAO 2010
publication_name: PR D82 051701
doi: 10.1103/PhysRevD.82.051701
inspire_id: 859335
title:
Dark Matter Direct Detection Constraints on the Minimal Supersymmetric Standard Model and Implications for LHC Higgs Boson Searches


document_id: LI 2013B
publication_name: PRL 110 261301
doi: 10.1103/PhysRevLett.110.261301
inspire_id: 1222499
title:
Limits on Spin-Independent Couplings of WIMP Dark Matter with a p-Type Point-Contact Germanium Detector


document_id: ROSZKOWSKI 2014
publication_name: JHEP 1408 067
doi: 10.1007/JHEP08(2014)067
inspire_id: 1297006
title:
.What Next for the CMSSM and the NUHM: Improved Prospects for Superpartner and Dark Matter Detection


document_id: AKERIB 2016
publication_name: PRL 116 161301
doi: 10.1103/PhysRevLett.116.161301
inspire_id: 1409257
title:
Improved Limits on Scattering of Weakly Interacting Massive Particles from Reanalysis of 2013 LUX Data


document_id: ELLIS 1998
publication_name: PR D58 095002
doi: 10.1103/PhysRevD.58.095002
inspire_id: 466692
title:
Charginos and Neutralinos in the Light of Radiative Corrections: Sealing the Fate of Higgsino Dark Matter


document_id: ELLIS 1998B
publication_name: PL B444 367
doi: 10.1016/S0370-2693(98)01392-6
inspire_id: 477873
title:
Neutralino - Stau Coannihilation and the Cosmological Upper Limit on the Mass of the Lightest Supersymmetric Particle


document_id: DJOUADI 2001
publication_name: JHEP 0108 055
doi: 10.1088/1126-6708/2001/08/055
inspire_id: 560870
title:
Constraints on the Minimal Supergravity Model and Prospects for SUSY Particle Production at Future Linear e+ e- Colliders


document_id: BUCHMUELLER 2008
publication_name: JHEP 0809 117
doi: 10.1088/1126-6708/2008/09/117
inspire_id: 794064
title:
Predictions for Supersymmetric Particle Masses using Indirect Experimental and Cosmological Constraints


document_id: BAER 2005
publication_name: JHEP 0507 065
doi: 10.1088/1126-6708/2005/07/065
inspire_id: 679508
title:
Direct, Indirect and Collider Detection of Neutralino Dark Matter in SUSY Models with non-Universal Higgs Masses


document_id: PROFUMO 2011
publication_name: PR D84 015008
doi: 10.1103/PhysRevD.84.015008
inspire_id: 901431
title:
Quest for Supersymmetry: Early LHC Results Versus Direct and Indirect Neutralino Dark Matter Searches


document_id: BESKIDT 2012
publication_name: EPJ C72 2166
doi: 10.1140/epjc/s10052-012-2166-z
inspire_id: 1122507
title:
Constraints on Supersymmetry from LHC Data on SUSY Searches and Higgs Bosons Combined with Cosmology and Direct Dark Matter Searches


document_id: CHATRCHYAN 2011B
publication_name: JHEP 1106 093
doi: 10.1007/JHEP06(2011)093
inspire_id: 900114
title:
Search for Supersymmetry in Events with a Lepton, a Photon, and Large Missing Transverse Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: ABE 1989J
publication_name: ZPHY C45 175
doi: 10.1007/BF01674449
inspire_id: 280669
title:
Measurement of the Differential Cross Section of e+ e- --> gamma gamma and e+ e- --> gamma gamma gamma at sqrt(s)=55, 56, 56.5 and 57 GeV and Search for Unstable Photino Pair Production


document_id: ABBOTT 1998
publication_name: PRL 80 442
doi: 10.1103/PhysRevLett.80.442
inspire_id: 446733
title:
Experimental Search for Chargino and Neutralino Production via Gauge Mediated Supersymmetry Breaking Models


document_id: ACCIARRI 1997V
publication_name: PL B415 299
doi: 10.1016/S0370-2693(97)01296-3
inspire_id: 446000
title:
Single and Multiphoton Events with Missing Energy in e+ e- Collisions at 161 GeV < sqrt(s) < 172 GeV


document_id: ACKERSTAFF 1998J
publication_name: EPJ C2 607
doi: 10.1007/s100520050165
inspire_id: 450757
title:
Search for Anomalous Production of Photonic Events with Missing Energy in e+ e- Collisions at sqrt(s) = 130-172 GeV


document_id: BARATE 1998H
publication_name: PL B420 127
doi: 10.1016/S0370-2693(97)01555-4
inspire_id: 449077
title:
Searches for Supersymmetry in the Photon(s) Plus Missing Energy Channels at sqrt(s) = 161 and 172 GeV


document_id: ABREU 1999D
publication_name: EPJ C6 371
doi: 10.1007/s100529801044
inspire_id: 477804
title:
Search for Pair Produced Neutralinos in Events with Photons and Missing Energy from e+ e- Collisions at sqrt(s) = 130-183 GeV


document_id: ABBIENDI 1999F
publication_name: EPJ C8 23
doi: 10.1007/s100520050442
inspire_id: 477626
title:
Search for Anomalous Photonic Events with Missing Energy in e+ e- Collisions at sqrt(s) = 130, 136 and 183 GeV


document_id: ACCIARRI 1999I
publication_name: PL B459 354
doi: 10.1016/S0370-2693(99)00680-2
inspire_id: 496400
title:
Search for R Parity Violating Chargino and Neutralino Decays in e+ e- Collisions up to sqrt(s) = 183 GeV


document_id: ACCIARRI 2001
publication_name: EPJ C19 397
doi: 10.1007/s100520100608
inspire_id: 536864
title:
Search for R-Parity Violating Decays of Supersymmetric Particles in e+e- Collisions at sqrt(s) = 189 GeV


document_id: HEISTER 2002R
publication_name: EPJ C25 339
doi: 10.1007/s10052-002-1005-z
inspire_id: 584153
title:
Search for Gauge Mediated SUSY Breaking Topologies in e+ e- Collisions at Centre-of-Mass Energies up to 209 GeV


document_id: ABDALLAH 2004M
publication_name: EPJ C36 1
doi: 10.1140/epjc/s2004-01881-6
inspire_id: 638198
title:
Search for Supersymmetric Particles Assuming R-Parity non-conservation in e+ e- Collisions at sqrt(s) = 192 to 208 GeV


document_id: ACOSTA 2005E
publication_name: PR D71 031104
doi: 10.1103/PhysRevD.71.031104
inspire_id: 662226
title:
Search for Anomalous Production of Diphoton Events with Missing Transverse Energy at CDF and Limits on Gauge-Mediated Supersymmetry-Breaking Models


document_id: ABAZOV 2006D
publication_name: PL B638 441
doi: 10.1016/j.physletb.2006.05.077
inspire_id: 715625
title:
Search for R-Parity Violating Supersymmetry via the LLEbar couplings lambda_{{121}}, lambda_{{122}} or lambda_{{133}} in p pbar collisions at sqrt(s) = 1.96 TeV


document_id: ABBIENDI 2006B
publication_name: EPJ C46 307
doi: 10.1140/epjc/s2006-02524-8
inspire_id: 687101
title:
Searches for Gauge-Mediated Supersymmetry Breaking Topologies in e+ e- Collisions at Centre-of-Mass Energies up to sqrt(s) = 209 GeV


document_id: ABAZOV 2006P
publication_name: PRL 97 161802
doi: 10.1103/PhysRevLett.97.161802
inspire_id: 721819
title:
Search for Neutral, Long-Lived Particles Decaying into Two Muons in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: AALTONEN 2010
publication_name: PRL 104 011801
doi: 10.1103/PhysRevLett.104.011801
inspire_id: 834428
title:
Search for Supersymmetry with Gauge-Mediated Breaking in Diphoton Events with Missing Transverse Energy at CDF II


document_id: ABAZOV 2010P
publication_name: PRL 105 221802
doi: 10.1103/PhysRevLett.105.221802
inspire_id: 865160
title:
Search for Diphoton Events with Large Missing Transverse Energy in 6.3 fb**-1 of ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2012R
publication_name: PL B707 478
doi: 10.1016/j.physletb.2011.12.057
inspire_id: 927046
title:
Search for Displaced Vertices Arising from Decays of New Heavy Particles in 7 TeV pp Collisions at ATLAS


document_id: ABAZOV 2012AD
publication_name: PR D86 071701
doi: 10.1103/PhysRevD.86.071701
inspire_id: 1094720
title:
Search for Zgamma Events with Large Missing Transverse Energy in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2012CP
publication_name: PL B718 411
doi: 10.1016/j.physletb.2012.10.069
inspire_id: 1184351
title:
Search for Diphoton Events with Large Missing Transverse Momentum in 7 TeV Proton-Proton Collision Data with the ATLAS Detector


document_id: CHATRCHYAN 2012BK
publication_name: JHEP 1211 172
doi: 10.1007/JHEP11(2012)172
inspire_id: 1120997
title:
Search for New Physics with Long-Lived Particles Decaying to Photons and Missing Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2012CT
publication_name: JHEP 1212 124
doi: 10.1007/JHEP12(2012)124
inspire_id: 1190891
title:
Search for R-Parity-Violating Supersymmetry in Events with Four or More Leptons in sqrt(s) = 7 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2013Q
publication_name: PL B719 261
doi: 10.1016/j.physletb.2013.01.041
inspire_id: 1198427
title:
Search for Supersymmetry in Events with Photons, Bottom Quarks, and Missing Transverse Momentum in Proton-Proton Collisions at a Centre-of-Mass Energy of 7 TeV with the ATLAS Detector


document_id: AAD 2013R
publication_name: PL B719 280
doi: 10.1016/j.physletb.2013.01.042
inspire_id: 1193933
title:
Search for Long-Lived, Heavy Particles in Final States with a Muon and Multi-Track Displaced Vertex in Proton-Proton Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: CHATRCHYAN 2013AH
publication_name: PL B722 273
doi: 10.1016/j.physletb.2013.04.027
inspire_id: 1206603
title:
Search for Long-Lived Particles Decaying to Photons and Missing Energy in Proton-Proton Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013AP
publication_name: PR D88 012001
doi: 10.1103/PhysRevD.88.012001
inspire_id: 1229502
title:
Search for Nonpointing Photons in the Diphoton and E(T)**miss Final State in sqrt(s) = 7 TeV Proton-Proton Collisions using the ATLAS Detector


document_id: AALTONEN 2013I
publication_name: PR D88 031103
doi: 10.1103/PhysRevD.88.031103
inspire_id: 1240679
title:
A Signature-Based Search for Delayed Photons in Exclusive Photon Plus Missing Transverse Energy Events from ppbar Collisions with sqrt(s) = 1.96 TeV


document_id: KHACHATRYAN 2014L
publication_name: PR D90 092007
doi: 10.1103/PhysRevD.90.092007
inspire_id: 1315820
title:
Searches for Electroweak Neutralino and Chargino Production in Channels with Higgs, Z, and W Bosons in pp Collisions at 8 TeV


document_id: AAD 2014BH
publication_name: PR D90 112005
doi: 10.1103/PhysRevD.90.112005
inspire_id: 1318336
title:
Search for Nonpointing and Delayed Photons in the Diphoton and Missing Transverse Momentum Final State in 8 TeV pp Collisions at the LHC using the ATLAS Detector


document_id: KHACHATRYAN 2016BX
publication_name: PR D94 112009
doi: 10.1103/PhysRevD.94.112009
inspire_id: 1472314
title:
Searches for R-Parity-Violating Supersymmetry in pp Collisions at sqrt(s) = 8 TeV in Final States with 0 -- 4 Leptons


document_id: KHACHATRYAN 2017AR
publication_name: PR D95 012009
doi: 10.1103/PhysRevD.95.012009
inspire_id: 1492321
title:
Search for R-Parity Violating Supersymmetry with Displaced Vertices in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: SIRUNYAN 2018O
publication_name: PR D97 032007
doi: 10.1103/PhysRevD.97.032007
inspire_id: 1623562
title:
Search for Higgsino pair production in $pp$ collisions at $\sqrt{s}$ = 13  TeV in final states with large missing transverse momentum and two Higgs bosons decaying via $H \to b \bar b$


document_id: AABOUD 2018Z
publication_name: PR D98 032009
doi: 10.1103/PhysRevD.98.032009
inspire_id: 1667045
title:
Search for supersymmetry in events with four or more leptons in $\sqrt{s}=13$ TeV $pp$ collisions with ATLAS


document_id: SIRUNYAN 2018X
publication_name: PL B779 166
doi: 10.1016/j.physletb.2017.12.069
inspire_id: 1621281
title:
Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at $\sqrt{s} = $ 13 TeV


document_id: SIRUNYAN 2018AO
publication_name: JHEP 1803 166
doi: 10.1007/JHEP03(2018)166
inspire_id: 1624165
title:
Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: SIRUNYAN 2018AP
publication_name: JHEP 1803 160
doi: 10.1007/JHEP03(2018)160
inspire_id: 1647947
title:
Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2018AR
publication_name: JHEP 1803 076
doi: 10.1007/s13130-018-7845-2
inspire_id: 1625745
title:
Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV


document_id: AABOUD 2018CK
publication_name: PR D98 092002
doi: 10.1103/PhysRevD.98.092002
inspire_id: 1677389
title:
Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector


document_id: SIRUNYAN 2019K
publication_name: JHEP 1901 154
doi: 10.1007/JHEP01(2019)154
inspire_id: 1708516
title:
Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2019CA
publication_name: PR D100 112003
doi: 10.1103/PhysRevD.100.112003
inspire_id: 1754075
title:
Search for long-lived particles using delayed photons in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2020D
publication_name: PL B801 135114
doi: 10.1016/j.physletb.2019.135114
inspire_id: 1745920
title:
Search for displaced vertices of oppositely charged leptons from decays of long-lived particles in $pp$ collisions at $\sqrt {s}$ =13 TeV with the ATLAS detector


document_id: AAD 2020AN
publication_name: JHEP 2010 005
doi: 10.1007/JHEP10(2020)005
inspire_id: 1792399
title:
Search for direct production of electroweakinos in final states with missing transverse momentum and a Higgs boson decaying into photons in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector


document_id: SIRUNYAN 2021M
publication_name: JHEP 2104 123
doi: 10.1007/JHEP04(2021)123
inspire_id: 1836850
title:
Search for supersymmetry in final states with two oppositely charged same-flavor leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: AAD 2021Y
publication_name: JHEP 2107 167
doi: 10.1007/JHEP07(2021)167
inspire_id: 1852821
title:
Search for supersymmetry in events with four or more charged leptons in 139 fb$^{−1}$ of $ \sqrt{s} $ = 13 TeV pp collisions with the ATLAS detector


document_id: SIRUNYAN 2021AF
publication_name: PR D104 052011
doi: 10.1103/PhysRevD.104.052011
inspire_id: 1861146
title:
Search for long-lived particles decaying to jets with displaced vertices in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2023AE
publication_name: EPJ C83 515
doi: 10.1140/epjc/s10052-023-11434-w
inspire_id: 2072870
title:
Searches for new phenomena in events with two leptons, jets, and missing transverse momentum in 139 fb$^{-1}$ of $\varvec{\sqrt{s}}=13$ TeV $\varvec{pp}$ collisions with the ATLAS detector


document_id: AAD 2023AM
publication_name: PR D108 012012
doi: 10.1103/PhysRevD.108.012012
inspire_id: 2654099
title:
Search in diphoton and dielectron final states for displaced production of Higgs or <math display=\"inline\"><mi>Z</mi></math> bosons with the ATLAS detector in <math display=\"inline\"><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math> <math display=\"inline\"><mi>p</mi><mi>p</mi></math> collisions


document_id: TUMASYAN 2023AO
publication_name: JHEP 2307 210
doi: 10.1007/JHEP07(2023)210
inspire_id: 2613855
title:
Search for long-lived particles using out-of-time trackless jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: HAYRAPETYAN 2024N
publication_name: PR D109 112001
doi: 10.1103/PhysRevD.109.112001
inspire_id: 2755433
title:
Combined search for electroweak production of winos, binos, higgsinos, and sleptons in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: AAD 2024U
publication_name: PR D109 112011
doi: 10.1103/PhysRevD.109.112011
inspire_id: 2751932
title:
Search for pair production of higgsinos in events with two Higgs bosons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions at the ATLAS experiment


document_id: AAD 2024AX
publication_name: PL B856 138938
doi: 10.1016/j.physletb.2024.138938
inspire_id: 2773395
title:
Search for pair-produced higgsinos decaying via Higgs or $Z$ bosons to final states containing a pair of photons and a pair of $b$-jets with the ATLAS detector


document_id: HAYRAPETYAN 2024AP
publication_name: PRL 133 201803
doi: 10.1103/PhysRevLett.133.201803
inspire_id: 2774247
title:
Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV


document_id: ABACHI 1996
publication_name: PRL 76 2228
doi: 10.1103/PhysRevLett.76.2228
inspire_id: 403196
title:
Search for Supersymmetric Wtilde_{{1}} Ztilde_{{2}} Production via Trilepton Final States in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: BUSKULIC 1996K
publication_name: PL B373 246
doi: 10.1016/0370-2693(96)00182-7
inspire_id: 416101
title:
Search for Supersymmetric Particles in e+ e- Collisions of Center-of-Mass Energies of 130 and 136 GeV


document_id: ABULENCIA 2007N
publication_name: PRL 98 221803
doi: 10.1103/PhysRevLett.98.221803
inspire_id: 745482
title:
Inclusive Search for New Physics with Like-Sign Dilepton Events in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2012T
publication_name: PL B709 137
doi: 10.1016/j.physletb.2012.01.076
inspire_id: 943401
title:
Searches for Supersymmetry with the ATLAS Detector using Final States with Two Leptons and Missing Transverse Momentum in sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: AAD 2012AS
publication_name: PRL 108 261804
doi: 10.1103/PhysRevLett.108.261804
inspire_id: 1112263
title:
Search for Supersymmetry in Events with Three Leptons and Missing Transverse Momentum in sqrt(s) = 7 TeV pp Collisions with the ATLAS Detector


document_id: CHATRCHYAN 2012BJ
publication_name: JHEP 1211 147
doi: 10.1007/JHEP11(2012)147
inspire_id: 1188683
title:
Search for Electroweak Production of Charginos and Neutralinos using Leptonic Final States in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013
publication_name: PL B718 841
doi: 10.1016/j.physletb.2012.11.039
inspire_id: 1127601
title:
Search for Direct Production of Charginos and Neutralinos in Events with Three Leptons and Missing Transverse Momentum in sqrt(s) = 7 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2014G
publication_name: JHEP 1405 071
doi: 10.1007/JHEP05(2014)071
inspire_id: 1286761
title:
Search for Direct Production of charginos, neutralinos and sleptons in Final States with Two Leptons and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2014H
publication_name: JHEP 1404 169
doi: 10.1007/JHEP04(2014)169
inspire_id: 1282905
title:
Search for Direct Production of Charginos and Neutralinos in Events with Three Leptons and Missing Transverse Momentum in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2014X
publication_name: PR D90 052001
doi: 10.1103/PhysRevD.90.052001
inspire_id: 1297226
title:
Search for Supersymmetry in Events with Four or More Leptons in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: KHACHATRYAN 2014I
publication_name: EPJ C74 3036
doi: 10.1140/epjc/s10052-014-3036-7
inspire_id: 1298508
title:
Searches for Electroweak Production of charginos, neutralinos, and sleptons Decaying to Leptons and W, Z, and Higgs Bosons in pp Collisions at 8 TeV


document_id: AAD 2015BA
publication_name: EPJ C75 208
doi: 10.1140/epjc/s10052-015-3408-7
inspire_id: 1341609
title:
Search for Direct Pair Production of a Chargino and a Neutralino Decaying to the 125 GeV Higgs Boson in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2016AA
publication_name: PR D93 052002
doi: 10.1103/PhysRevD.93.052002
inspire_id: 1394670
title:
Search for the Electroweak Production of Supersymmetric Particles in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: SIRUNYAN 2017AW
publication_name: JHEP 1711 029
doi: 10.1007/JHEP11(2017)029
inspire_id: 1608161
title:
Search for Electroweak Production of Charginos and Neutralinos in WH Events in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2018R
publication_name: PR D97 052010
doi: 10.1103/PhysRevD.97.052010
inspire_id: 1644618
title:
Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: AABOUD 2018U
publication_name: PR D97 092006
doi: 10.1103/PhysRevD.97.092006
inspire_id: 1654357
title:
Search for photonic signatures of gauge-mediated supersymmetry in 13 TeV $pp$ collisions with the ATLAS detector


document_id: SIRUNYAN 2018AJ
publication_name: PL B782 440
doi: 10.1016/j.physletb.2018.05.062
inspire_id: 1646260
title:
Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AABOUD 2018AY
publication_name: EPJ C78 154
doi: 10.1140/epjc/s10052-018-5583-9
inspire_id: 1620202
title:
Search for the direct production of charginos and neutralinos  in final states with tau leptons in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector


document_id: AABOUD 2018BT
publication_name: EPJ C78 995
doi: 10.1140/epjc/s10052-018-6423-7
inspire_id: 1658902
title:
Search for electroweak production of supersymmetric particles in final states with two or three leptons at $\sqrt{s}=13\,$TeV with the ATLAS detector


document_id: SIRUNYAN 2018DP
publication_name: JHEP 1811 151
doi: 10.1007/JHEP11(2018)151
inspire_id: 1681016
title:
Search for supersymmetry in events with a $\tau$ lepton pair and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: AABOUD 2018CO
publication_name: PR D98 092012
doi: 10.1103/PhysRevD.98.092012
inspire_id: 1676551
title:
Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: AABOUD 2019AU
publication_name: PR D100 012006
doi: 10.1103/PhysRevD.100.012006
inspire_id: 1711261
title:
Search for chargino and neutralino production in final states with a Higgs boson and missing transverse momentum at $\sqrt{s} = 13$ TeV with the ATLAS detector


document_id: SIRUNYAN 2019BU
publication_name: JHEP 1908 150
doi: 10.1007/JHEP08(2019)150
inspire_id: 1737508
title:
Search for supersymmetry with a compressed mass spectrum in the vector boson fusion topology with 1-lepton and 0-lepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2020I
publication_name: PR D101 052005
doi: 10.1103/PhysRevD.101.052005
inspire_id: 1767649
title:
Searches for electroweak production of supersymmetric particles with compressed mass spectra in $\sqrt{s}=$ 13 TeV $pp$ collisions with the ATLAS detector


document_id: AAD 2020K
publication_name: PR D101 072001
doi: 10.1103/PhysRevD.101.072001
inspire_id: 1771533
title:
Search for chargino-neutralino production with mass splittings near the electroweak scale in three-lepton final states in $\sqrt {s}$=13  TeV $pp$ collisions with the ATLAS detector


document_id: AAD 2020R
publication_name: EPJ C80 691
doi: 10.1140/epjc/s10052-020-8050-3
inspire_id: 1755298
title:
Search for direct production of electroweakinos in final states with one lepton, missing transverse momentum and a Higgs boson decaying into two $b$-jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: SIRUNYAN 2020AU
publication_name: PRL 124 041803
doi: 10.1103/PhysRevLett.124.041803
inspire_id: 1757579
title:
Search for Supersymmetry with a Compressed Mass Spectrum in Events with a Soft $\tau$ Lepton, a Highly Energetic Jet, and Large Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt{s}=$  TeV


document_id: TUMASYAN 2021C
publication_name: JHEP 2110 045
doi: 10.1007/JHEP10(2021)045
inspire_id: 1895525
title:
Search for chargino-neutralino production in events with Higgs and W bosons using 137 fb$^{−1}$ of proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: AAD 2021BG
publication_name: EPJ C81 1118
doi: 10.1140/epjc/s10052-021-09749-7
inspire_id: 1866951
title:
Search for chargino–neutralino pair production in final states with three leptons and missing transverse momentum in $\sqrt{s} = 13$ TeV pp collisions with the ATLAS detector


document_id: TUMASYAN 2022Q
publication_name: JHEP 2204 091
doi: 10.1007/JHEP04(2022)091
inspire_id: 1966342
title:
Search for supersymmetry in final states with two or three soft leptons and missing transverse momentum in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: TUMASYAN 2023B
publication_name: PL B842 137460
doi: 10.1016/j.physletb.2022.137460
inspire_id: 2085373
title:
Search for electroweak production of charginos and neutralinos at <math altimg=\"si1.svg\"><msqrt><mrow><mi>s</mi></mrow></msqrt><mo linebreak=\"goodbreak\" linebreakstyle=\"after\">=</mo><mn>13</mn><mspace width=\"0.25em\"/><mtext>TeV</mtext></math> in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum


document_id: HAYRAPETYAN 2023E
publication_name: JHEP 2310 046
doi: 10.1007/JHEP10(2023)046
inspire_id: 2683599
title:
Search for new physics in multijet events with at least one photon and large missing transverse momentum in proton-proton collisions at 13 TeV


document_id: AAD 2023CI
publication_name: JHEP 2312 167
doi: 10.1007/JHEP12(2023)167
inspire_id: 2710022
title:
Search for direct production of electroweakinos in final states with one lepton, jets and missing transverse momentum in pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: AAD 2024G
publication_name: PRL 132 221801
doi: 10.1103/PhysRevLett.132.221801
inspire_id: 2751400
title:
Search for nearly mass-degenerate higgsinos using low-momentum mildly-displaced tracks in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector


document_id: AAD 2024AJ
publication_name: JHEP 2405 150
doi: 10.1007/JHEP05(2024)150
inspire_id: 2754043
title:
Search for electroweak production of supersymmetric particles in final states with two $\tau$-leptons in $\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector


document_id: ADEVA 1989B
publication_name: PL B233 530
doi: 10.1016/0370-2693(89)91353-1
inspire_id: 282645
title:
Mass Limits for Scalar Muons, Scalar Electrons, and Winos from e+ e- Collisions near sqrt(s) = 91 GeV


document_id: AKRAWY 1990D
publication_name: PL B240 261
doi: 10.1016/0370-2693(90)90444-B
inspire_id: 285183
title:
A Search for Acoplanar Pairs of Leptons or Jets in Z0 Decays: Mass Limits on Supersymmetric Particles


document_id: ACKERSTAFF 1998K
publication_name: EPJ C4 47
doi: 10.1007/PL00021655
inspire_id: 449533
title:
Search for Anomalous Production of Dilepton Events with Missing Transverse Momentum in e+ e- Collisions at sqrt(s) = 161 an


document_id: ABREU 1999V
publication_name: PL B466 61
doi: 10.1016/S0370-2693(99)01105-3
inspire_id: 507867
title:
Search for Chargino Pair Production in Scenarios with Gravitino LSP and Stau NLSP at sqrt(s) ~~ 183 GeV at LEP


document_id: BARATE 2000H
publication_name: EPJ C13 29
doi: 10.1007/s100520000284
inspire_id: 504716
title:
Search for R Parity Violating Decays of Supersymmetric Particles in e+ e- Collisions at Ecm near 183 GeV


document_id: ACCIARRI 2000K
publication_name: PL B482 31
doi: 10.1016/S0370-2693(00)00488-3
inspire_id: 523976
title:
Search for Charginos with a Small Mass Difference with the Lightest Supersymmetric Particle at sqrt(s) = 189 GeV


document_id: BARATE 2001B
publication_name: EPJ C19 415
doi: 10.1007/s100520100633
inspire_id: 536138
title:
Search for R-Parity Violating Decays of Supersymmetric Particles in e+e- Collisions at Ecm from 189 to 202 GeV


document_id: HEISTER 2002J
publication_name: PL B533 223
doi: 10.1016/S0370-2693(02)01584-8
inspire_id: 584019
title:
Search for Charginos Nearly Mass Degenerate with the Lightest Neutralino in e+ e- Collisions at Center-of-Mass Energies up to 209-GeV


document_id: HEISTER 2003G
publication_name: EPJ C31 1
doi: 10.1140/epjc/s2003-01311-5
inspire_id: 598949
title:
Search for Supersymmetric Particles with R-Paryty Violating Decays in e+ e- Collisions at sqrt(s) up to 209 GeV


document_id: ABAZOV 2005U
publication_name: PRL 95 151805
doi: 10.1103/PhysRevLett.95.151805
inspire_id: 680705
title:
Search for Supersymmetry via Associated Production of Charginos and Neutralinos in Final States with Three Leptons


document_id: AALTONEN 2008L
publication_name: PR D77 052002
doi: 10.1103/PhysRevD.77.052002
inspire_id: 768187
title:
Search for Chargino-Neutralino Production in p pbar Collisions at sqrt(s) = 1.96 TeV with high-pT Leptons


document_id: AALTONEN 2008AE
publication_name: PRL 101 251801
doi: 10.1103/PhysRevLett.101.251801
inspire_id: 793317
title:
Search for Supersymmetry in p pbar Collisions at sqrt(s) = 1.96 TeV using the Trilepton Signature for Chargino-Neutralino Production


document_id: AALTONEN 2009G
publication_name: PR D79 052004
doi: 10.1103/PhysRevD.79.052004
inspire_id: 800000
title:
Search for New Physics in the mumu + e/mu + notET Channel with a Low-pT Lepton Threshold at the Collider Detector at Fermilab


document_id: ABAZOV 2009T
publication_name: PL B680 34
doi: 10.1016/j.physletb.2009.08.011
inspire_id: 810372
title:
Search for Associated Production of Charginos and Neutralinos in the Trilepton Final State using 2.3 fb^{-1} of data


document_id: CHATRCHYAN 2011V
publication_name: PL B704 411
doi: 10.1016/j.physletb.2011.09.047
inspire_id: 912697
title:
Search for Physics beyond the Standard Model using Multilepton Signatures in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013B
publication_name: PL B718 879
doi: 10.1016/j.physletb.2012.11.058
inspire_id: 1127505
title:
Search for Direct Slepton and Gaugino Production in Final States with Two Leptons and Missing Transverse Momentum with the ATLAS Detector in pp Collisions at sqrt(s) = 7 TeV


document_id: AALTONEN 2014
publication_name: PR D90 012011
doi: 10.1103/PhysRevD.90.012011
inspire_id: 1256081
title:
Search for New Physics in Trilepton Events and Limits on the Associated Chargino-Neutralino Production at CDF


document_id: AAD 2014AV
publication_name: JHEP 1410 096
doi: 10.1007/JHEP10(2014)096
inspire_id: 1304288
title:
Search for the Direct Production of charginos, neutralinos and staus in Final States with at least Two Hadronically Decaying taus and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2015CA
publication_name: PR D92 072001
doi: 10.1103/PhysRevD.92.072001
inspire_id: 1383883
title:
Search for Photonic Signatures of Gauge-Mediated Supersymmetry in 8 TeV pp Collisions with the ATLAS Detector


document_id: KHACHATRYAN 2016R
publication_name: PL B757 6
doi: 10.1016/j.physletb.2016.03.039
inspire_id: 1386851
title:
Search for Supersymmetry in Events with a Photon, a Lepton, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV


document_id: KHACHATRYAN 2016Y
publication_name: PL B759 9
doi: 10.1016/j.physletb.2016.05.033
inspire_id: 1411443
title:
Search for Supersymmetry in Events with Soft Leptons, Low Jet Multiplicity, and Missing Transverse Energy in Proton-Proton Collisions at sqrt(s) =8 TeV


document_id: KHACHATRYAN 2016AA
publication_name: PL B759 479
doi: 10.1016/j.physletb.2016.05.088
inspire_id: 1424834
title:
Search for Supersymmetry in Electroweak Production with Photons and Large Missing Transverse Energy in pp Collisions at sqrt(s) = 8 TeV


document_id: KHACHATRYAN 2017L
publication_name: JHEP 1704 018
doi: 10.1007/JHEP04(2017)018
inspire_id: 1492317
title:
Search for Electroweak Production of Charginos in Final States with Two tau Leptons in pp Collisions at sqrt(s) = 8 TeV


document_id: SIRUNYAN 2018AA
publication_name: PL B780 118
doi: 10.1016/j.physletb.2018.02.045
inspire_id: 1637580
title:
Search for gauge-mediated supersymmetry in events with at least one photon and missing transverse momentum in pp collisions at $\sqrt{s} = $ 13 TeV


document_id: SIRUNYAN 2018DN
publication_name: JHEP 1811 079
doi: 10.1007/JHEP11(2018)079
inspire_id: 1683312
title:
Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2020O
publication_name: EPJ C80 123
doi: 10.1140/epjc/s10052-019-7594-6
inspire_id: 1750597
title:
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector


document_id: AAD 2021E
publication_name: PR D103 112003
doi: 10.1103/PhysRevD.103.112003
inspire_id: 1831992
title:
Search for trilepton resonances from chargino and neutralino pair production in $\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector


document_id: AAD 2023M
publication_name: JHEP 2306 031
doi: 10.1007/JHEP06(2023)031
inspire_id: 2157951
title:
Search for direct pair production of sleptons and charginos decaying to two leptons and neutralinos with mass splittings near the W-boson mass in $ \sqrt{s} $ = 13 TeV pp collisions with the ATLAS detector


document_id: HAYRAPETYAN 2024M
publication_name: PR D109 072007
doi: 10.1103/PhysRevD.109.072007
inspire_id: 2705044
title:
Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: AAD 2024CE
publication_name: JHEP 2412 116
doi: 10.1007/JHEP12(2024)116
inspire_id: 2835159
title:
Search for supersymmetry using vector boson fusion signatures and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: ACKERSTAFF 1998P
publication_name: PL B433 195
doi: 10.1016/S0370-2693(98)00518-8
inspire_id: 468524
title:
Search for Stable and Longlived Massive Charged Particles with the OPAL Detector at LEP in e+e- Collisions at sqrt(s) = 13


document_id: ABREU 1998P
publication_name: PL B444 491
doi: 10.1016/S0370-2693(98)01443-9
inspire_id: 478905
title:
A Search for Heavy Stable and Longlived Squarks and Sleptons in e+ e- Collisions at Energies from 130 to 183 GeV


document_id: AAD 2012BJ
publication_name: EPJ C72 1993
doi: 10.1140/epjc/s10052-012-1993-2
inspire_id: 1090055
title:
Search for Anomaly-Mediated Supersymmetry Breaking with the ATLAS Detector Based on a Disappearing-Track Signature in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013H
publication_name: JHEP 1301 131
doi: 10.1007/JHEP01(2013)131
inspire_id: 1190185
title:
Search for Direct Chargino Production in Anomaly-Mediated Supersymmetry Breaking Models Based on a Disappearing-Track Signature in pp Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2013BD
publication_name: PR D88 112006
doi: 10.1103/PhysRevD.88.112006
inspire_id: 1258398
title:
Search for Charginos Nearly Mass Degenerate with the Lightest Neutralino Based on a Disappearing-Track Signature in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2015W
publication_name: PR D91 052012
doi: 10.1103/PhysRevD.91.052012
inspire_id: 1329959
title:
Search for Long-Lived Particles that Decay into Final States Containing Two Electrons or Two Muons in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2015AE
publication_name: JHEP 1501 068
doi: 10.1007/JHEP01(2015)068
inspire_id: 1329957
title:
Searches for Heavy Long-Lived Charged Particles with the ATLAS Detector in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: KHACHATRYAN 2015AO
publication_name: EPJ C75 325
doi: 10.1140/epjc/s10052-015-3533-3
inspire_id: 1343509
title:
Constraints on the pMSSM, AMSB Model and on Other Models from the Search for Long-Lived Charged Particles in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2015BM
publication_name: EPJ C75 407
doi: 10.1140/epjc/s10052-015-3609-0
inspire_id: 1376482
title:
Search for Metastable Heavy Charged Particles with Large Ionisation Energy Loss in pp Collisions at sqrt(s) = 8 TeV using the ATLAS Experiment


document_id: AABOUD 2018AS
publication_name: JHEP 1806 022
doi: 10.1007/JHEP06(2018)022
inspire_id: 1641262
title:
Search for long-lived charginos based on a disappearing-track signature in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector


document_id: SIRUNYAN 2018BR
publication_name: JHEP 1808 016
doi: 10.1007/JHEP08(2018)016
inspire_id: 1669245
title:
Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: AABOUD 2019AT
publication_name: PR D99 092007
doi: 10.1103/PhysRevD.99.092007
inspire_id: 1718558
title:
Search for heavy charged long-lived particles in the ATLAS detector in 36.1 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV


document_id: AAD 2022U
publication_name: EPJ C82 606
doi: 10.1140/epjc/s10052-022-10489-5
inspire_id: 2005658
title:
Search for long-lived charginos based on a disappearing-track signature using 136 fb$^{-1}$ of pp collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector


document_id: AAD 2023G
publication_name: JHEP 2306 158
doi: 10.1007/JHEP06(2023)158
inspire_id: 2080541
title:
Search for heavy, long-lived, charged particles with large ionisation energy loss in $pp$ collisions at $\sqrt{s} = 13~\text{TeV}$ using the ATLAS experiment and the full Run 2 dataset


document_id: BECK 1994
publication_name: PL B336 141
doi: 10.1016/0370-2693(94)01000-5
inspire_id: 361098
title:
Searching for Dark Matter with the Enriched Ge Detectors of the Heidelberg-Moscow Double beta Decay Experiment


document_id: ABBIENDI 2000R
publication_name: EPJ C13 553
doi: 10.1007/s100520000315
inspire_id: 504989
title:
Tests of the Standard Model and Constraints on New Physics from Measurements of Fermion Pair Production at 189 GeV at LEP


document_id: HEISTER 2002F
publication_name: EPJ C25 1
doi: 10.1007/s10052-002-1010-2
inspire_id: 581519
title:
Search for R-Parity Violating Production of Single Sneutrinos in e+ e- Collisions at sqrt(s) = 189 to 209 GeV


document_id: ABAZOV 2002H
publication_name: PRL 89 261801
doi: 10.1103/PhysRevLett.89.261801
inspire_id: 591658
title:
Search for the Production of Single Sleptons Trhough R-Parity Violation in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABAZOV 2008Q
publication_name: PRL 100 241803
doi: 10.1103/PhysRevLett.100.241803
inspire_id: 768210
title:
Search for Scalar Neutrino Superpartners in e + mu Final States in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: AALTONEN 2010Z
publication_name: PRL 105 191801
doi: 10.1103/PhysRevLett.105.191801
inspire_id: 852448
title:
Search for R-Parity Violating Decays of Sneutrinos to emu, mutau, and etau Pairs in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2010M
publication_name: PRL 105 191802
doi: 10.1103/PhysRevLett.105.191802
inspire_id: 863389
title:
Search for Sneutrino Production in emu Final States in 5.3 fb**-1 of ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: SIRUNYAN 2019AO
publication_name: EPJ C79 305
doi: 10.1140/epjc/s10052-019-6800-x
inspire_id: 1704953
title:
Search for resonant production of second-generation sleptons with same-sign dimuon events in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: BRANDELIK 1982B
publication_name: PL 117B 365
doi: 10.1016/0370-2693(82)90737-7
inspire_id: 178495
title:
Electroweak Coupling Constants in the Leptonic Reactions e+ e- --> e+ e- and e+ e- --> mu+ mu- and Search for Scalar Leptons


document_id: ZHUKOVSKII 1990
publication_name: SJNP 52 931
inspire_id: 307801
title:
Production of Photinos in Intensive Electromagnetic Field and Constraint on Scalar Electron Mass in Supersymmetric Theories


document_id: ABE 1995A
publication_name: PL B361 199
doi: 10.1016/0370-2693(95)01177-R
inspire_id: 406593
title:
A Study of Single Photon Production in e+ e- Collisions at sqrt(s) = 58 GeV with the TOPAZ Detector at TRISTAN


document_id: ABREU 1999C
publication_name: EPJ C6 385
doi: 10.1007/s100529801043
inspire_id: 477802
title:
Search for Scalar Fermions and Long Lived Scalar Leptons at Centre-of-Mass Energies of 130 to 172 GeV


document_id: ABBIENDI 2000G
publication_name: EPJ C14 51
doi: 10.1007/s100520000335
inspire_id: 507875
title:
Search for Anomalous Production of Acoplanar Dilepton Events in e+ e- Collisions at sqrt(s) = 183 and 189 GeV


document_id: SIRUNYAN 2019AW
publication_name: PL B790 140
doi: 10.1016/j.physletb.2019.01.005
inspire_id: 1677905
title:
Search for supersymmetric partners of electrons and muons in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: FAYET 1979
publication_name: PL 84B 416
doi: 10.1016/0370-2693(79)91229-2
inspire_id: 7725
title:
Relations between the Masses of the Superpartners of Leptons and Quarks, the Goldstino Couplings and the Neutral Currents


document_id: AAD 2012AF
publication_name: PL B714 180
doi: 10.1016/j.physletb.2012.06.055
inspire_id: 1095404
title:
Search for Events with Large Missing Transverse Momentum, Jets, and at least Two tau Leptons in 7 TeV Proton-Proton Collision Data with the ATLAS Detector


document_id: AAD 2012AG
publication_name: PL B714 197
doi: 10.1016/j.physletb.2012.06.061
inspire_id: 1111144
title:
Search for Supersymmetry with Jets, Missing Transverse Momentum and at least One Hadronically Decaying tau Lepton in Proton-Proton Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2012CM
publication_name: EPJ C72 2215
doi: 10.1140/epjc/s10052-012-2215-7
inspire_id: 1189432
title:
Search for Supersymmetry in Events with Large Missing Transverse Momentum, Jets, and at Least One tau Lepton in 7 TeV Proton-Proton Collision Data with the ATLAS Detector


document_id: AAD 2020H
publication_name: PR D101 032009
doi: 10.1103/PhysRevD.101.032009
inspire_id: 1765529
title:
Search for direct stau production in events with two hadronic $\tau$-leptons in $\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector


document_id: SIRUNYAN 2020P
publication_name: EPJ C80 189
doi: 10.1140/epjc/s10052-020-7739-7
inspire_id: 1747233
title:
Search for direct pair production of supersymmetric partners to the $\tau$ lepton in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: TUMASYAN 2023AG
publication_name: PR D108 012011
doi: 10.1103/PhysRevD.108.012011
inspire_id: 2678649
title:
Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: AAD 2011P
publication_name: PL B703 428
doi: 10.1016/j.physletb.2011.08.042
inspire_id: 914491
title:
Search for Heavy Long-Lived Charged Particles with the ATLAS Detector in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013AA
publication_name: PL B720 277
doi: 10.1016/j.physletb.2013.02.015
inspire_id: 1199005
title:
Searches for Heavy Long-Lived Sleptons and R-Hadrons with the ATLAS Detector in pp Collisions at sqrt(s) = 7 TeV


document_id: TUMASYAN 2022AF
publication_name: EPJ C82 153
doi: 10.1140/epjc/s10052-022-10027-3
inspire_id: 1940976
title:
Search for long-lived particles decaying to leptons with large impact parameter in proton–proton collisions at $\sqrt{s} = 13\,\text {Te}\text {V} $


document_id: AAD 2023BQ
publication_name: PL B846 138172
doi: 10.1016/j.physletb.2023.138172
inspire_id: 2656211
title:
Search for pairs of muons with small displacements in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector


document_id: CHATRCHYAN 2011C
publication_name: JHEP 1106 026
doi: 10.1007/JHEP06(2011)026
inspire_id: 891814
title:
Search for Physics beyond the Standard Model in Opposite-Sign Dilepton Events in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2011B
publication_name: EPJ C71 1682
doi: 10.1140/epjc/s10052-011-1682-6
inspire_id: 894578
title:
Search for Supersymmetric Particles in Events with Lepton Pairs and Large Missing Transverse Momentum in sqrt(s) = 7 TeV Proton-Proton Collisions with the ATLAS Experiment


document_id: AAD 2011C
publication_name: EPJ C71 1647
doi: 10.1140/epjc/s10052-011-1647-9
inspire_id: 894579
title:
Search for an Excess of Events with an Identical Flavour Lepton Pair and Significant Missing Transverse Momentum in sqrt(s) = 7 TeV proton-proton Collisions with the ATLAS Detector


document_id: AAD 2011G
publication_name: PRL 106 131802
doi: 10.1103/PhysRevLett.106.131802
inspire_id: 889431
title:
Search for supersymmetry using final states with one lepton, jets, and missing transverse momentum with the ATLAS detector in sqrt{s} = 7 TeV pp


document_id: AAD 2011N
publication_name: PL B701 186
doi: 10.1016/j.physletb.2011.05.061
inspire_id: 890749
title:
Search for squarks and gluinos using Final States with Jets and Missing Transverse Momentum with the ATLAS Detector in sqrt(s) = 7 TeV proton-proton Collisions


document_id: KHACHATRYAN 2011I
publication_name: PL B698 196
doi: 10.1016/j.physletb.2011.03.021
inspire_id: 883771
title:
Search for Supersymmetry in pp Collisions at 7 TeV in Events with Jets and Missing Transverse Energy


document_id: CHATRCHYAN 2011G
publication_name: PRL 106 211802
doi: 10.1103/PhysRevLett.106.211802
inspire_id: 891482
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 7 TeV in Events with Two Photons and Missing Transverse Energy


document_id: ALBAJAR 1987D
publication_name: PL B198 261
doi: 10.1016/0370-2693(87)91509-7
inspire_id: 249740
title:
Events with Large Missing Transverse Energy at the CERN Collider: III. Mass Limits on Supersymmetric Particles


document_id: ABBOTT 1999
publication_name: PRL 82 29
doi: 10.1103/PhysRevLett.82.29
inspire_id: 474782
title:
Search for Squarks and Gluinos in Single-Photon Events with Jets and Large Missing Transverse Energy in ppbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABE 1999M
publication_name: PRL 83 2133
doi: 10.1103/PhysRevLett.83.2133
inspire_id: 480447
title:
Search for R-Parity Violating Supersymmetry using Like Sign Dielectrons in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABBOTT 2001D
publication_name: PR D63 091102
doi: 10.1103/PhysRevD.63.091102
inspire_id: 524477
title:
Search for Dilepton Signatures from Minimal Low Energy Supergravity in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABBIENDI 2002
publication_name: EPJ C23 1
doi: 10.1007/s100520100859
inspire_id: 557820
title:
Search for Single Leptoquark and Squark Production in Electron Photon Scattering at sqrt(s(ee)) = 189 GeV at LEP


document_id: ABAZOV 2002G
publication_name: PR D66 112001
doi: 10.1103/PhysRevD.66.112001
inspire_id: 586179
title:
Search for MSUGRA in Single Electron Events with Jets and Large Missing Transverse Energy in p pbar Collisions at sqrt(s) = 1.8-TeV


document_id: ABAZOV 2006C
publication_name: PL B638 119
doi: 10.1016/j.physletb.2006.05.030
inspire_id: 714446
title:
Search for Squarks and Gluinos in Events with Jets and Missing Transverse Energy in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2008G
publication_name: PL B660 449
doi: 10.1016/j.physletb.2008.01.042
inspire_id: 771372
title:
Search for Squarks and Gluinos in Events with Jets and Missing Transverse Energy using 2.1 fb**-1 of p pbar Collision Data at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2009S
publication_name: PL B680 24
doi: 10.1016/j.physletb.2009.08.002
inspire_id: 821287
title:
Search for squark Production in Events with Jets, Hadronically Decaying tau Leptons and Missing Transverse Energy at sqrt(s) = 1.96TeV


document_id: CHATRCHYAN 2011Q
publication_name: JHEP 1108 156
doi: 10.1007/JHEP08(2011)156
inspire_id: 917588
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 7  TeV in Events with a Single Lepton, Jets, and Missing Transverse Momentum


document_id: CHATRCHYAN 2011AC
publication_name: JHEP 1108 155
doi: 10.1007/JHEP08(2011)155
inspire_id: 914487
title:
Search for New Physics with Jets and Missing Transverse Momentum in pp Collisions at sqrt(s) =  7 TeV


document_id: AAD 2011AE
publication_name: JHEP 1110 107
doi: 10.1007/JHEP10(2011)107
inspire_id: 921596
title:
Inclusive Search for Same-Sign Dilepton Signatures in pp Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2011AF
publication_name: JHEP 1111 099
doi: 10.1007/JHEP11(2011)099
inspire_id: 939504
title:
Search for New Phenomena in Final States with Large Jet Multiplicities and Missing Transverse Momentum using sqrt(s) = 7 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2012W
publication_name: PL B710 67
doi: 10.1016/j.physletb.2012.02.051
inspire_id: 930002
title:
Search for squarks and gluinos using Final States with Jets and Missing Transverse Momentum with the ATLAS Detector in sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: AAD 2012AX
publication_name: PR D85 012006
doi: 10.1103/PhysRevD.85.012006
inspire_id: 930005
title:
Search for Supersymmetry in Final States with Jets, Missing Transverse Momentum and One Isolated Lepton in sqrt(s) = 7 TeV pp Collisions using 1 fb^{-1} of ATLAS data


document_id: CHATRCHYAN 2012AE
publication_name: PRL 109 171803
doi: 10.1103/PhysRevLett.109.171803
inspire_id: 1121703
title:
Search for New Physics in the Multijet and Missing Transverse Momentum Final State in Proton-Proton Collisions at sqrt(s) = 7 TeV


document_id: AAD 2012CJ
publication_name: PR D86 092002
doi: 10.1103/PhysRevD.86.092002
inspire_id: 1180197
title:
Further Search for Supersymmetry at sqrt(s) = 7 TeV in Final States with Jets, Missing Transverse Momentum, and Isolated Leptons with the ATLAS Detector


document_id: CHATRCHYAN 2013
publication_name: PL B718 815
doi: 10.1016/j.physletb.2012.11.036
inspire_id: 1118578
title:
Search for New Physics in Events with Opposite-Sign Leptons, Jets, and Missing Transverse Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2013G
publication_name: JHEP 1301 077
doi: 10.1007/JHEP01(2013)077
inspire_id: 1194120
title:
Search for Supersymmetry in Final States with Missing Transverse Energy and 0, 1, 2, or >=3 b-Quark Jets in 7 TeV pp Collisions using the Variable alpha_{{T}}


document_id: AAD 2013L
publication_name: PR D87 012008
doi: 10.1103/PhysRevD.87.012008
inspire_id: 1125961
title:
Search for Squarks and Gluinos with the ATLAS Detector in Final States with Jets and Missing Transverse Momentum using 4.7 fb^{-1} of sqrt(s) = 7 TeV Proton-Proton Collision Data


document_id: CHATRCHYAN 2013H
publication_name: PL B719 42
doi: 10.1016/j.physletb.2012.12.055
inspire_id: 1189815
title:
Search for Supersymmetry in Events with Photons and Low Missing Transverse Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2013T
publication_name: EPJ C73 2568
doi: 10.1140/epjc/s10052-013-2568-6
inspire_id: 1223519
title:
Search for Supersymmetry in Hadronic Final States with Missing Transverse Energy using the Variables alpha(T) and b-Quark Multiplicity in pp Collisions at 8 TeV


document_id: CHATRCHYAN 2013W
publication_name: JHEP 1303 111
doi: 10.1007/JHEP03(2013)111
inspire_id: 1203307
title:
Search for New Physics in Events with Photons, Jets, and Missing Transverse Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2013AO
publication_name: PR D87 072001
doi: 10.1103/PhysRevD.87.072001
inspire_id: 1209556
title:
Search for Supersymmetry in Events with Opposite-Sign Dileptons and Missing Transverse Energy using an Artificial Neural Network


document_id: AAD 2014E
publication_name: JHEP 1406 035
doi: 10.1007/JHEP06(2014)035
inspire_id: 1289225
title:
Search for Supersymmetry at sqrt(s) = 8 TeV in Final States with Jets and Two Same-Sign Leptons or Three Leptons with the ATLAS Detector


document_id: CHATRCHYAN 2014I
publication_name: JHEP 1406 055
doi: 10.1007/JHEP06(2014)055
inspire_id: 1281837
title:
Search for New Physics in the Multijet and Missing Transverse Momentum Final State in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2014AE
publication_name: JHEP 1409 176
doi: 10.1007/JHEP09(2014)176
inspire_id: 1298722
title:
Search for squarks and gluinos with the ATLAS Detector in Final States with Jets and Missing Transverse Momentum using sqrt(s) = 8 TeV Proton-Proton Collision Data


document_id: AAD 2015K
publication_name: PRL 114 161801
doi: 10.1103/PhysRevLett.114.161801
inspire_id: 1337472
title:
Search for Scalar Charm Quark Pair Production in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2015AI
publication_name: JHEP 1504 116
doi: 10.1007/JHEP04(2015)116
inspire_id: 1339376
title:
Search for Squarks and Gluinos in Events with Isolated Leptons, Jets and Missing Transverse Momentum at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2015AF
publication_name: JHEP 1505 078
doi: 10.1007/JHEP05(2015)078
inspire_id: 1345027
title:
Searches for Supersymmetry using the M(T2) Variable in Hadronic Events Produced in pp Collisions at 8 TeV


document_id: KHACHATRYAN 2015AR
publication_name: PL B743 503
doi: 10.1016/j.physletb.2015.03.017
inspire_id: 1330294
title:
Collins and Sivers Asymmetries in Muonproduction of Pions and Kaons off Transversely Polarised Protons


document_id: AAD 2015BV
publication_name: JHEP 1510 054
doi: 10.1007/JHEP10(2015)054
inspire_id: 1383884
title:
Summary of the Searches for Squarks and Gluinos using sqrt(s) = 8 TeV pp Collisions with the ATLAS Experiment at the LHC


document_id: AAD 2015CB
publication_name: PR D92 072004
doi: 10.1103/PhysRevD.92.072004
inspire_id: 1362183
title:
Search for Massive, Long-Lived Particles using Multitrack Displaced Vertices or Displaced Lepton Pairs in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2015CS
publication_name: PR D91 012008
doi: 10.1103/PhysRevD.91.012008
inspire_id: 1326409
title:
Search for New Phenomena in Events with a Photon and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AABOUD 2016D
publication_name: PR D94 032005
doi: 10.1103/PhysRevD.94.032005
inspire_id: 1452559
title:
Search for New Phenomena in Final States with an Energetic Jet and Large Missing Transverse Momentum in pp Collisions at sqrt(s) = 13 TeV using the ATLAS Detector


document_id: AABOUD 2016N
publication_name: EPJ C76 392
doi: 10.1140/epjc/s10052-016-4184-8
inspire_id: 1458270
title:
Search for Squarks and Gluinos in Final States with Jets and Missing Transverse Momentum at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2016BS
publication_name: JHEP 1610 006
doi: 10.1007/JHEP10(2016)006
inspire_id: 1427411
title:
Search for New Physics with the MT2 Variable in all-Jets Final States Produced in pp Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2017N
publication_name: EPJ C77 144
doi: 10.1140/epjc/s10052-017-4700-5
inspire_id: 1498566
title:
Search for New Phenomena in Events Containing a Same-Flavour Opposite-Sign Dilepton Pair, Jets, and Large Missing Transverse Momentum in sqrt(s) = 13 pp Collisions with the ATLAS Detector


document_id: KHACHATRYAN 2017P
publication_name: EPJ C77 294
doi: 10.1140/epjc/s10052-017-4787-8
inspire_id: 1495423
title:
A Search for New Phenomena in pp Collisions at sqrt(s) = 13TeV in Final States with Missing Transverse Momentum and at Least One Jet using the alpha(T) Variable


document_id: KHACHATRYAN 2017V
publication_name: PL B769 391
doi: 10.1016/j.physletb.2017.04.005
inspire_id: 1499477
title:
Search for Supersymmetry in Events with Photons and Missing Transverse Energy in pp Collisions at 13 TeV


document_id: SIRUNYAN 2017P
publication_name: PR D96 032003
doi: 10.1103/PhysRevD.96.032003
inspire_id: 1594909
title:
Search for Supersymmetry in Multijet Events with Missing Transverse Momentum in Proton-Proton Collisions at 13 TeV


document_id: AABOUD 2017AR
publication_name: PR D96 112010
doi: 10.1103/PhysRevD.96.112010
inspire_id: 1620206
title:
Search for squarks and gluinos in Events with an Isolated Lepton, Jets, and Missing Transverse Momentum at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: SIRUNYAN 2017AY
publication_name: JHEP 1712 142
doi: 10.1007/JHEP12(2017)142
inspire_id: 1610629
title:
Search for Supersymmetry in Events with at Least One Photon, Missing Transverse Momentum, and Large Transverse Event Activity in Proton-Proton Collisions at sqrt(s) =13 TeV


document_id: SIRUNYAN 2017AZ
publication_name: EPJ C77 710
doi: 10.1140/epjc/s10052-017-5267-x
inspire_id: 1599400
title:
Search for New Phenomena with the M(T2) Variable in the All-Hadronic Final State Produced in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2018I
publication_name: JHEP 1801 126
doi: 10.1007/JHEP01(2018)126
inspire_id: 1635274
title:
Search for Dark Matter and other New Phenomena in Events with an Energetic Jet and Large Missing Transverse Momentum using the ATLAS Detector


document_id: AABOUD 2018V
publication_name: PR D97 112001
doi: 10.1103/PhysRevD.97.112001
inspire_id: 1641270
title:
Search for squarks and gluinos in final states with jets and missing transverse momentum using 36  fb$^{-1}$ of $\sqrt{s}=13$  TeV pp collision data with the ATLAS detector


document_id: SIRUNYAN 2018AY
publication_name: JHEP 1805 025
doi: 10.1007/JHEP05(2018)025
inspire_id: 1653451
title:
Search for natural and split supersymmetry in proton-proton collisions at $ \sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum


document_id: AABOUD 2018BJ
publication_name: EPJ C78 625
doi: 10.1140/epjc/s10052-018-6081-9
inspire_id: 1675352
title:
Search for new phenomena using the invariant mass distribution of same-flavour opposite-sign dilepton pairs in events with missing transverse momentum in $\sqrt{s}=13$   $\text {Te}\text {V}$ pp collisions with the ATLAS detector


document_id: AABOUD 2018BV
publication_name: JHEP 1809 050
doi: 10.1007/JHEP09(2018)050
inspire_id: 1672099
title:
Search for supersymmetry in final states with charm jets and missing transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector


document_id: SIRUNYAN 2019AG
publication_name: JHEP 1906 143
doi: 10.1007/JHEP06(2019)143
inspire_id: 1725476
title:
Search for supersymmetry in final states with photons and missing transverse momentum in proton-proton collisions at 13 TeV


document_id: SIRUNYAN 2019CH
publication_name: JHEP 1910 244
doi: 10.1007/JHEP10(2019)244
inspire_id: 1749379
title:
Search for supersymmetry in proton-proton collisions at 13 TeV in final states with jets and missing transverse momentum


document_id: AAD 2021L
publication_name: JHEP 2102 143
doi: 10.1007/JHEP02(2021)143
inspire_id: 1827025
title:
Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector


document_id: AAD 2021AK
publication_name: EPJ C81 600
doi: 10.1140/epjc/s10052-021-09344-w
inspire_id: 1839446
title:
Search for squarks and gluinos in final states with one isolated lepton, jets, and missing transverse momentum at $\sqrt{s}=13$  with the ATLAS detector


document_id: HAYRAPETYAN 2024Q
publication_name: PR D109 112009
doi: 10.1103/PhysRevD.109.112009
inspire_id: 2706677
title:
Search for stealth supersymmetry in final states with two photons, jets, and low missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: SIRUNYAN 2018EA
publication_name: PRL 121 141802
doi: 10.1103/PhysRevLett.121.141802
inspire_id: 1676219
title:
Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: HAYRAPETYAN 2024Y
publication_name: JHEP 2405 047
doi: 10.1007/JHEP05(2024)047
inspire_id: 2760892
title:
Search for long-lived particles decaying to final states with a pair of muons in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV


document_id: AAD 2013BC
publication_name: PR D88 112003
doi: 10.1103/PhysRevD.88.112003
inspire_id: 1261968
title:
Search for Long-Lived Stopped R-Hadrons Decaying out of Time with pp Collisions using the ATLAS Detector


document_id: KHACHATRYAN 2015AK
publication_name: EPJ C75 151
doi: 10.1140/epjc/s10052-015-3367-z
inspire_id: 1340699
title:
Search for Decays of Stopped Long-Lived Particles Produced in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AABOUD 2016B
publication_name: PL B760 647
doi: 10.1016/j.physletb.2016.07.042
inspire_id: 1470936
title:
Search for Heavy Long-Lived Charged R-Hadrons with the ATLAS Detector in 3.2 fb^{-1} of Proton-Proton Collision Data at sqrt(s) =13 TeV


document_id: SIRUNYAN 2019BH
publication_name: PR D99 032011
doi: 10.1103/PhysRevD.99.032011
inspire_id: 1704319
title:
Search for long-lived particles decaying into displaced jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2011O
publication_name: PL B701 398
doi: 10.1016/j.physletb.2011.06.015
inspire_id: 893493
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 7 TeV in Final States with Missing Transverse Momentum and b-Jets


document_id: ACCIARRI 1999C
publication_name: PL B445 428
doi: 10.1016/S0370-2693(98)01505-6
inspire_id: 476785
title:
Searches for Scalar Top and Scalar Bottom Quarks in e+ e- Interactions at 161 GeV <= sqrt(s) <= 183 GeV


document_id: AALTONEN 2007E
publication_name: PR D76 072010
doi: 10.1103/PhysRevD.76.072010
inspire_id: 756023
title:
Searches for Direct Pair Production of Supersymmetric Top and Supersymmetric Bottom Quarks in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2012AN
publication_name: PRL 108 181802
doi: 10.1103/PhysRevLett.108.181802
inspire_id: 1081778
title:
Search for Scalar Bottom Quark Pair Production with the ATLAS Detector in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2013V
publication_name: JHEP 1303 037
doi: 10.1007/JHEP03(2013)037
inspire_id: 1208703
title:
Search for New Physics in Events with Same-Sign Dileptons and b Jets in pp Collisions at sqrt(s) = 8 TeV


document_id: AAD 2013AU
publication_name: JHEP 1310 189
doi: 10.1007/JHEP10(2013)189
inspire_id: 1247462
title:
Search for Direct Third-Generation Squark Pair Production in Final States with Missing Transverse Momentum and Two b-Jets in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: CHATRCHYAN 2014H
publication_name: JHEP 1401 163
doi: 10.1007/JHEP01(2014)163
inspire_id: 1266257
title:
Search for New Physics in Events with Same-Sign Dileptons and Jets in pp Collisions at sqrt(s) = 8 TeV


document_id: AAD 2014T
publication_name: PR D90 052008
doi: 10.1103/PhysRevD.90.052008
inspire_id: 1304459
title:
Search for Pair-Produced Third-Generation squarks Decaying via Charm Quarks or in Compressed Supersymmetric Scenarios in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2014AX
publication_name: JHEP 1410 024
doi: 10.1007/JHEP10(2014)024
inspire_id: 1304457
title:
Search for Strong Production of Supersymmetric Particles in Final States with Missing Transverse Momentum and at Least Three b-Jets at sqrt(s) = 8 TeV Proton-Proton Collisions with the ATLAS Detector


document_id: KHACHATRYAN 2015AD
publication_name: JHEP 1504 124
doi: 10.1007/JHEP04(2015)124
inspire_id: 1345823
title:
Search for Physics Beyond the Standard Model in Events with Two Leptons, Jets, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV


document_id: KHACHATRYAN 2015AH
publication_name: JHEP 1506 116
doi: 10.1007/JHEP06(2015)116
inspire_id: 1356728
title:
Searches for Third-Generation Squark Production in Fully Hadronic Final States in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2015CJ
publication_name: EPJ C75 510
doi: 10.1140/epjc/s10052-015-3726-9
inspire_id: 1380183
title:
ATLAS Run 1 Searches for Direct Pair Production of Third-Generation Squarks at the Large Hadron Collider


document_id: AAD 2016BB
publication_name: EPJ C76 259
doi: 10.1140/epjc/s10052-016-4095-8
inspire_id: 1424844
title:
Search for Supersymmetry at sqrt(s) = 13 TeV in Final States with Jets and Two Same-Sign Leptons or Three Leptons with the ATLAS Detector


document_id: AABOUD 2016Q
publication_name: EPJ C76 547
doi: 10.1140/epjc/s10052-016-4382-4
inspire_id: 1472822
title:
Search for Bottom Squark Pair Production in Proton-Proton Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2017A
publication_name: PRL 118 021802
doi: 10.1103/PhysRevLett.118.021802
inspire_id: 1466301
title:
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: KHACHATRYAN 2016BY
publication_name: JHEP 1612 013
doi: 10.1007/JHEP12(2016)013
inspire_id: 1473675
title:
Search for New Physics in Final States with Two Opposite-Sign, Same-Flavor leptons, jets, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 13 TeV


document_id: KHACHATRYAN 2017AW
publication_name: EPJ C77 635
doi: 10.1140/epjc/s10052-017-5182-1
inspire_id: 1510442
title:
Search for New Phenomena with Multiple Charged Leptons in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2017AJ
publication_name: JHEP 1709 084
doi: 10.1007/JHEP09(2017)084
inspire_id: 1604276
title:
Search for Supersymmetry in Final States with Two Same-Sign or Three Leptons and Jets using 36 fb^{-1} of sqrt(s) = 13 TeV pp Collision Data with the ATLAS Detector


document_id: AABOUD 2017AX
publication_name: JHEP 1711 195
doi: 10.1007/JHEP11(2017)195
inspire_id: 1620694
title:
Search for Supersymmetry in Events with b-Tagged Jets and Missing Transverse Momentum in pp Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: SIRUNYAN 2018B
publication_name: PL B778 263
doi: 10.1016/j.physletb.2018.01.012
inspire_id: 1611299
title:
Search for the Pair Production of Third-Generation squarks with Two-Body Decays to a Bottom or Charm Quark and a Neutralino in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: SIRUNYAN 2018AL
publication_name: JHEP 1802 067
doi: 10.1007/JHEP02(2018)067
inspire_id: 1632447
title:
Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV


document_id: AAD 2019H
publication_name: JHEP 1912 060
doi: 10.1007/JHEP12(2019)060
inspire_id: 1748602
title:
Search for bottom-squark pair production with the ATLAS detector in final states containing Higgs bosons, $b$-jets and missing transverse momentum


document_id: SIRUNYAN 2020T
publication_name: EPJ C80 752
doi: 10.1140/epjc/s10052-020-8168-3
inspire_id: 1777617
title:
Search for physics beyond the standard model in events with jets and two same-sign or at least three charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2020V
publication_name: JHEP 2006 046
doi: 10.1007/JHEP06(2020)046
inspire_id: 1754675
title:
Search for squarks and gluinos in final states with same-sign leptons and jets using 139 fb$^{-1}$ of data collected with the ATLAS detector


document_id: AAD 2021AM
publication_name: PR D104 032014
doi: 10.1103/PhysRevD.104.032014
inspire_id: 1851675
title:
Search for bottom-squark pair production in $pp$ collision events at $\sqrt{s} = 13$ TeV with hadronically decaying $\tau$-leptons, $b$-jets and missing transverse momentum using the ATLAS detector


document_id: BARATE 2000P
publication_name: PL B488 234
doi: 10.1016/S0370-2693(00)00893-5
inspire_id: 530949
title:
Search for a Scalar Top Almost Degenerate with the Lightest Neutralino in e+ e- Collisions at sqrt(s) up to 202 GeV


document_id: ACOSTA 2003C
publication_name: PRL 90 251801
doi: 10.1103/PhysRevLett.90.251801
inspire_id: 613065
title:
Search for the Supersymmtric Partner of the Top Quark in Dilepton Events from p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ACOSTA 2004B
publication_name: PRL 92 051803
doi: 10.1103/PhysRevLett.92.051803
inspire_id: 618376
title:
Search for Pair Production of Scalar Top Quarks in R Parity Violating Decay Modes in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABAZOV 2007B
publication_name: PL B645 119
doi: 10.1016/j.physletb.2006.12.024
inspire_id: 730710
title:
Search for the Pair Production of Scalar Top Quarks in the Acoplanar Charm Jet Final State in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2008
publication_name: PL B659 500
doi: 10.1016/j.physletb.2007.11.086
inspire_id: 756262
title:
Search for the Lightest Scalar Top Quark in Events with Two Leptons in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2008Z
publication_name: PL B665 1
doi: 10.1016/j.physletb.2008.05.037
inspire_id: 781447
title:
Search for Scalar Top Quarks in the Acoplanar Charm Jets and Missing Transverse Energy Final State in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2009N
publication_name: PL B674 4
doi: 10.1016/j.physletb.2009.02.027
inspire_id: 810576
title:
Search for Admixture of Scalar Top Quarks in the ttbar Lepton + Jets Final State at sqrt(s) = 1.96TeV


document_id: ABAZOV 2009O
publication_name: PL B675 289
doi: 10.1016/j.physletb.2009.04.039
inspire_id: 801554
title:
Search for the Lightest Scalar Top Quark in Events with Two Leptons in ppbar Collisions at sqrt(s) = 1.96TeV


document_id: AALTONEN 2010O
publication_name: PRL 104 251801
doi: 10.1103/PhysRevLett.104.251801
inspire_id: 839163
title:
Search for Pair Production of Supersymmetric Top Quarks in Dilepton Events from p p Collisions ar sqrt(s) = 1.96 TeV


document_id: AAD 2012J
publication_name: EPJ C72 2040
doi: 10.1140/epjc/s10052-012-2040-z
inspire_id: 1113445
title:
Search for Lepton Flavour Violation in the emu Continuum with the ATLAS Detector in sqrt(s) = 7 TeV pp Collisions at the LHC


document_id: AAD 2012AH
publication_name: PL B715 44
doi: 10.1016/j.physletb.2012.07.010
inspire_id: 1112907
title:
Search for Scalar Top Quark Pair Production in Natural Gauge Mediated Supersymmetry Models with the ATLAS Detector in pp Collisions at  sqrt(s) = 7 TeV


document_id: AAD 2012CB
publication_name: JHEP 1211 094
doi: 10.1007/JHEP11(2012)094
inspire_id: 1186556
title:
Search for a Heavy Top-Quark Partner in Final States with Two Leptons with the ATLAS Detector at the LHC


document_id: AAD 2012CE
publication_name: PRL 109 211802
doi: 10.1103/PhysRevLett.109.211802
inspire_id: 1126136
title:
Search for a Supersymmetric Partner to the Top Quark in Final States with Jets and Missing Transverse Momentum at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2012CF
publication_name: PRL 109 211803
doi: 10.1103/PhysRevLett.109.211803
inspire_id: 1127331
title:
Search for Direct Top Squark Pair Production in Final States with One Isolated Lepton, Jets, and Missing Transverse Momentum in sqrt(s) = 7 TeV pp Collisions Using 4.7 fb^{-1} of ATLAS Data


document_id: AAD 2012CL
publication_name: EPJ C72 2237
doi: 10.1140/epjc/s10052-012-2237-1
inspire_id: 1128464
title:
Search for Light Scalar Top-Quark Pair Production in Final States with Two Leptons with the ATLAS Detector in sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: AAD 2013T
publication_name: PL B720 13
doi: 10.1016/j.physletb.2013.01.049
inspire_id: 1184952
title:
Search for Light Top squark Pair Production in Final States with Leptons and b-Jets with the ATLAS Detector in sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: CHATRCHYAN 2013BN
publication_name: PRL 111 221801
doi: 10.1103/PhysRevLett.111.221801
inspire_id: 1240497
title:
Search for Top Squarks in R-Parity-Violating Supersymmetry using Three or More Leptons and b-Tagged Jets


document_id: CHATRCHYAN 2013BS
publication_name: EPJ C73 2677
doi: 10.1140/epjc/s10052-013-2677-2
inspire_id: 1246905
title:
Search for Top-Squark Pair Production in the Single-Lepton Final State in pp Collisions at sqrt(s) = 8 TeV


document_id: AAD 2014B
publication_name: EPJ C74 2883
doi: 10.1140/epjc/s10052-014-2883-6
inspire_id: 1286622
title:
Search for Direct top squark Pair Production in Events with a Z Boson, b-jets and Missing Transverse Momentum in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2014F
publication_name: JHEP 1406 124
doi: 10.1007/JHEP06(2014)124
inspire_id: 1286444
title:
Search for Direct top-Squark Pair Production in Final States with Two Leptons in pp Collisions at sqrt(s) = 8 TeV with the ATLAS detector


document_id: AAD 2014AJ
publication_name: JHEP 1409 015
doi: 10.1007/JHEP09(2014)015
inspire_id: 1299143
title:
Search for Direct Pair Production of the top squark in all-Hadronic Final States in Proton-Proton Collisions at sqrt(s) = 8 TeV with the ATLAS detector


document_id: AAD 2014BD
publication_name: JHEP 1411 118
doi: 10.1007/JHEP11(2014)118
inspire_id: 1304456
title:
Search for Top squark Pair Production in Final States with One Isolated Lepton, Jets, and Missing Transverse Momentum in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: KHACHATRYAN 2015E
publication_name: PRL 114 061801
doi: 10.1103/PhysRevLett.114.061801
inspire_id: 1317640
title:
Search for Displaced Supersymmetry in Events with an Electron and a Muon with Large Impact Parameters


document_id: KHACHATRYAN 2015L
publication_name: PL B747 98
doi: 10.1016/j.physletb.2015.04.045
inspire_id: 1335501
title:
Search for Pair-Produced Resonances Decaying to Jet Pairs in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: KHACHATRYAN 2015X
publication_name: PR D91 052018
doi: 10.1103/PhysRevD.91.052018
inspire_id: 1342447
title:
Search for Supersymmetry Using Razor Variables in Events with b-Tagged Jets in pp Collisions at sqrt(s) = 8 TeV


document_id: AAD 2016AM
publication_name: JHEP 1606 067
doi: 10.1007/JHEP06(2016)067
inspire_id: 1417099
title:
A Search for Top squarks with R-parity-violating Decays to All-hadronic Final States with the ATLAS Detector in sqrt(s) = 8 TeV Proton-Proton Collisions


document_id: KHACHATRYAN 2016AV
publication_name: JHEP 1607 027
doi: 10.1007/JHEP07(2016)027
inspire_id: 1420556
title:
Search for Direct Pair Production of Scalar Top Quarks in the Single- and Dilepton Channels in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2016AY
publication_name: EPJ C76 81
doi: 10.1140/epjc/s10052-016-3897-z
inspire_id: 1393662
title:
Search for Direct Top Squark Pair Production in Final States with Two Tau Leptons in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2016BK
publication_name: EPJ C76 460
doi: 10.1140/epjc/s10052-016-4292-5
inspire_id: 1425690
title:
Search for Direct Pair Production of Supersymmetric Top Quarks Decaying to All-Hadronic Final States in pp Collisions at sqrt(s) = 8 TeV


document_id: AABOUD 2016J
publication_name: PR D94 052009
doi: 10.1103/PhysRevD.94.052009
inspire_id: 1469069
title:
Search for Top Squarks in Final States with One Isolated Lepton, Jets, and Missing Transverse Momentum in sqrt(s) = 13 TeV pp Collisions with the ATLAS Detector


document_id: KHACHATRYAN 2017S
publication_name: PL B767 403
doi: 10.1016/j.physletb.2017.02.007
inspire_id: 1466293
title:
Search for top squark Pair Production in Compressed-Mass-Spectrum Scenarios in Proton-Proton Collisions at sqrt(s) = 8 TeV using the alpha(T) Variable


document_id: KHACHATRYAN 2017AD
publication_name: PR D96 012004
doi: 10.1103/PhysRevD.96.012004
inspire_id: 1508171
title:
Search for Supersymmetry in the All-Hadronic Final State using Top Quark Tagging in pp Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2017AF
publication_name: JHEP 1708 006
doi: 10.1007/JHEP08(2017)006
inspire_id: 1604889
title:
Search for Direct Top Squark Pair Production in Events with a Higgs or Z Boson, and Missing Transverse Momentum in sqrt(s) = 13 TeV pp Collisions with the ATLAS Detector


document_id: SIRUNYAN 2017AS
publication_name: JHEP 1710 019
doi: 10.1007/JHEP10(2017)019
inspire_id: 1605128
title:
Search for top squark Pair Production in pp Collisions at sqrt(s) = 13 TeV using Single Lepton Events


document_id: SIRUNYAN 2017AT
publication_name: JHEP 1710 005
doi: 10.1007/JHEP10(2017)005
inspire_id: 1609449
title:
Search for Direct Production of Supersymmetric Partners of the Top Quark in the All-Jets Final State in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2017AY
publication_name: JHEP 1712 085
doi: 10.1007/JHEP12(2017)085
inspire_id: 1623207
title:
Search for a Scalar Partner of the Top Quark in the Jets Plus Missing Transverse Momentum Final State at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: AABOUD 2017BE
publication_name: EPJ C77 898
doi: 10.1140/epjc/s10052-017-5445-x
inspire_id: 1615470
title:
Search for Direct Top Squark Pair Production in Final States with Two Leptons in sqrt(s) = 13 TeV pp Collisions with the ATLAS Detector


document_id: SIRUNYAN 2018C
publication_name: PR D97 032009
doi: 10.1103/PhysRevD.97.032009
inspire_id: 1634253
title:
Search for Top Squarks and Dark Matter Particles in Opposite-Charge Dilepton Final States at sqrt(s) = 13 TeV


document_id: AABOUD 2018Y
publication_name: PR D98 032008
doi: 10.1103/PhysRevD.98.032008
inspire_id: 1664486
title:
Search for top squarks decaying to tau sleptons in $pp$ collisions at  $\sqrt{s}= 13$ TeV with the ATLAS detector


document_id: SIRUNYAN 2018AN
publication_name: JHEP 1803 167
doi: 10.1007/JHEP03(2018)167
inspire_id: 1609450
title:
Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV


document_id: AABOUD 2018AQ
publication_name: JHEP 1806 108
doi: 10.1007/JHEP06(2018)108
inspire_id: 1639856
title:
Search for top-squark pair production in final states with one lepton, jets, and missing transverse momentum using 36 fb$^{−1}$ of $ \sqrt{s}=13 $ TeV pp collision data with the ATLAS detector


document_id: SIRUNYAN 2018DI
publication_name: JHEP 1809 065
doi: 10.1007/JHEP09(2018)065
inspire_id: 1673197
title:
Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2019S
publication_name: JHEP 1903 031
doi: 10.1007/JHEP03(2019)031
inspire_id: 1709318
title:
Inclusive search for supersymmetry in pp collisions at $ \sqrt{s}=13 $ TeV using razor variables and boosted object identification in zero and one lepton final states


document_id: SIRUNYAN 2019U
publication_name: JHEP 1903 101
doi: 10.1007/JHEP03(2019)101
inspire_id: 1712372
title:
Search for the pair production of light top squarks in the e$^{\pm}\mu^{\mp}$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: SIRUNYAN 2019AU
publication_name: EPJ C79 444
doi: 10.1140/epjc/s10052-019-6926-x
inspire_id: 1716137
title:
Search for supersymmetry in events with a photon, jets, $\mathrm {b}$ -jets, and missing transverse momentum in proton–proton collisions at 13 $\,\text {Te}\text {V}$


document_id: AABOUD 2020
publication_name: EPJ C80 754
doi: 10.1140/epjc/s10052-020-8181-6
inspire_id: 1725498
title:
Measurements of top-quark pair spin correlations in the $e\mu$ channel at $\sqrt{s} = 13$ TeV using $pp$ collisions in the ATLAS detector


document_id: SIRUNYAN 2020U
publication_name: JHEP 2002 015
doi: 10.1007/JHEP02(2020)015
inspire_id: 1762677
title:
Search for top squark pair production in a final state with two tau leptons in proton-proton collisions at $ \sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2020AH
publication_name: JHEP 2005 032
doi: 10.1007/JHEP05(2020)032
inspire_id: 1771845
title:
Search for direct top squark pair production in events with one lepton, jets, and missing transverse momentum at 13 TeV with the CMS experiment


document_id: AAD 2020AS
publication_name: EPJ C80 1080
doi: 10.1140/epjc/s10052-020-08469-8
inspire_id: 1800411
title:
Search for top squarks in events with a Higgs or $Z$ boson using 139 fb$^{-1}$ of $pp$ collision data at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: SIRUNYAN 2021B
publication_name: EPJ C81 3
doi: 10.1140/epjc/s10052-020-08701-5
inspire_id: 1811597
title:
Search for top squark pair production using dilepton final states in pp collision data collected at $\sqrt{s} =$ 13 TeV


document_id: AAD 2021O
publication_name: JHEP 2104 174
doi: 10.1007/JHEP04(2021)174
inspire_id: 1835604
title:
Search for new phenomena with top quark pairs in final states with one lepton, jets, and missing transverse momentum in $pp$ collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector


document_id: AAD 2021P
publication_name: JHEP 2104 165
doi: 10.1007/JHEP04(2021)165
inspire_id: 1844425
title:
Search for new phenomena in events with two opposite-charge leptons, jets and missing transverse momentum in pp collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV with the ATLAS detector


document_id: SIRUNYAN 2021AD
publication_name: PR D104 052001
doi: 10.1103/PhysRevD.104.052001
inspire_id: 1849522
title:
Search for top squark production in fully-hadronic final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: TUMASYAN 2021I
publication_name: EPJ C81 970
doi: 10.1140/epjc/s10052-021-09721-5
inspire_id: 1893826
title:
Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at $\sqrt{s} = 13\,\text {Te}\text {V} $


document_id: TUMASYAN 2023K
publication_name: JHEP 2306 060
doi: 10.1007/JHEP06(2023)060
inspire_id: 2624652
title:
Search for top squarks in the four-body decay mode with single lepton final states in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: TUMASYAN 2023AB
publication_name: JHEP 2307 110
doi: 10.1007/JHEP07(2023)110
inspire_id: 2651438
title:
Search for top squark pair production in a final state with at least one hadronically decaying tau lepton in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: AAD 2024AC
publication_name: JHEP 2403 139
doi: 10.1007/JHEP03(2024)139
inspire_id: 2751107
title:
Search for new phenomena with top-quark pairs and large missing transverse momentum using 140 $\mathrm{fb}^{-1}$ of $pp$ collision data at $\sqrt{s}=13$ TeV with the ATLAS detector


document_id: AAD 2024AO
publication_name: JHEP 2407 250
doi: 10.1007/JHEP07(2024)250
inspire_id: 2759516
title:
A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector


document_id: AABOUD 2017AI
publication_name: JHEP 1709 088
doi: 10.1007/JHEP09(2017)088
inspire_id: 1597123
title:
Search for New Phenomena in a Lepton Plus High Jet Multiplicity Final State with the ATLAS Experiment using sqrt(s) = 13 TeV Proton-Proton Collision Data


document_id: AABOUD 2018P
publication_name: PR D97 032003
doi: 10.1103/PhysRevD.97.032003
inspire_id: 1630899
title:
Search for B-L R -parity-violating top squarks in $\sqrt s$ =13  TeV pp collisions with the ATLAS experiment


document_id: AABOUD 2018BB
publication_name: EPJ C78 250
doi: 10.1140/epjc/s10052-018-5693-4
inspire_id: 1631641
title:
A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector


document_id: SIRUNYAN 2018DV
publication_name: PR D98 092011
doi: 10.1103/PhysRevD.98.092011
inspire_id: 1685992
title:
Search for long-lived particles with displaced vertices in multijet events in proton-proton collisions at $\sqrt{s}= $13 TeV


document_id: SIRUNYAN 2018DY
publication_name: PR D98 112014
doi: 10.1103/PhysRevD.98.112014
inspire_id: 1685989
title:
Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AAD 2020M
publication_name: PR D102 032006
doi: 10.1103/PhysRevD.102.032006
inspire_id: 1788448
title:
Search for long-lived, massive particles in events with a displaced vertex and a muon with large impact parameter in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector


document_id: AAD 2021B
publication_name: EPJ C81 11
doi: 10.1140/epjc/s10052-021-08970-8
inspire_id: 1821239
title:
Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC


document_id: SIRUNYAN 2021U
publication_name: PR D104 012015
doi: 10.1103/PhysRevD.104.012015
inspire_id: 1834733
title:
Search for long-lived particles using displaced jets in proton-proton collisions at $\sqrt{s} = $ 13 TeV


document_id: SIRUNYAN 2021V
publication_name: PR D104 032006
doi: 10.1103/PhysRevD.104.032006
inspire_id: 1846679
title:
Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at $\sqrt {s}$ = 13  TeV


document_id: TUMASYAN 2023L
publication_name: JHEP 2307 161
doi: 10.1007/JHEP07(2023)161
inspire_id: 2098256
title:
Search for resonant and nonresonant production of pairs of dijet resonances in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: AAD 2024BT
publication_name: PR D110 092004
doi: 10.1103/PhysRevD.110.092004
inspire_id: 2802475
title:
A search for $R$-parity violating supersymmetric decays of the top squark to a $b$-jet and a lepton in $\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector


document_id: AFFOLDER 2002
publication_name: PRL 88 041801
doi: 10.1103/PhysRevLett.88.041801
inspire_id: 557644
title:
Search for Gluinos and Scalar Quarks in p pbar Collisions at sqrt(s) = 1.8 TeV using the Missing Energy Plus Multijets Signature


document_id: AAD 2011X
publication_name: EPJ C71 1744
doi: 10.1140/epjc/s10052-011-1744-9
inspire_id: 916840
title:
Search for Diphoton Events with Large Missing Transverse Energy with 36 pb**-1 of 7 TeV Proton-Proton Collision Data with the ATLAS Detector


document_id: CHATRCHYAN 2011AB
publication_name: JHEP 1106 077
doi: 10.1007/JHEP06(2011)077
inspire_id: 896527
title:
Search for New Physics with Same-Sign Isolated Dilepton Events with Jets and Missing Transverse Energy at the LHC


document_id: AAD 2012X
publication_name: PL B710 519
doi: 10.1016/j.physletb.2012.02.054
inspire_id: 946427
title:
Search for Diphoton Events with Large Missing Transverse Momentum in 1 fb^{-1} of 7 TeV Proton-Proton Collision Data with the ATLAS Detector


document_id: CHATRCHYAN 2012Q
publication_name: PL B716 260
doi: 10.1016/j.physletb.2012.08.026
inspire_id: 1111141
title:
Search for Physics beyond the Standard Model in Events with a Z Boson, Jets, and Missing Transverse Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2012AP
publication_name: PRL 108 241802
doi: 10.1103/PhysRevLett.108.241802
inspire_id: 1094860
title:
Search for Gluinos in Events with Two Same-Sign Leptons, Jets, and Missing Transverse Momentum with the ATLAS Detector in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2012U
publication_name: PRL 109 071803
doi: 10.1103/PhysRevLett.109.071803
inspire_id: 1116526
title:
Search for New Physics with Same-Sign Isolated Dilepton Events with Jets and Missing Transverse Energy


document_id: AAD 2012BA
publication_name: PR D85 112006
doi: 10.1103/PhysRevD.85.112006
inspire_id: 1095236
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 7 TeV in Final States with Missing Transverse Momentum and b-Jets with the ATLAS Detector


document_id: AAD 2012BI
publication_name: JHEP 1207 167
doi: 10.1007/JHEP07(2012)167
inspire_id: 1117704
title:
Hunt for New Phenomena using Large Jet Multiplicities and Missing Transverse Momentum with ATLAS in 4.7 fb^{-1} of sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: AAD 2012BY
publication_name: EPJ C72 2174
doi: 10.1140/epjc/s10052-012-2174-z
inspire_id: 1123116
title:
Search for Top and Bottom squarks from gluino Pair Production in Final States with Missing Transverse Energy and at Least Three b-Jets with the ATLAS Detector


document_id: CHATRCHYAN 2012AH
publication_name: PR D86 072010
doi: 10.1103/PhysRevD.86.072010
inspire_id: 1181767
title:
Search for Supersymmetry in Events with b-Quark Jets and Missing Transverse Energy in pp Collisions at 7 TeV


document_id: AAD 2012CU
publication_name: JHEP 1212 086
doi: 10.1007/JHEP12(2012)086
inspire_id: 1191022
title:
Search for Pair Production of Massive Particles Decaying into Three Quarks with the ATLAS Detector in sqrt(s) = 7 TeV pp Collisions at the LHC


document_id: AAD 2013AB
publication_name: EPJ C73 2362
doi: 10.1140/epjc/s10052-013-2362-5
inspire_id: 1208701
title:
Multi-Channel Search for Squarks and Gluinos in sqrt(s) = 7 TeV pp Collisions with the ATLAS Detector


document_id: CHATRCHYAN 2013P
publication_name: EPJ C73 2404
doi: 10.1140/epjc/s10052-013-2404-z
inspire_id: 1208988
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 7 TeV in Events with a Single Lepton, Jets, and Missing Transverse Momentum


document_id: CHATRCHYAN 2013R
publication_name: EPJ C73 2493
doi: 10.1140/epjc/s10052-013-2493-8
inspire_id: 1211187
title:
Search for Physics beyond the Standard Model in Events with tau Leptons, Jets, and Large Transverse Momentum Imbalance in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2013AK
publication_name: PL B725 243
doi: 10.1016/j.physletb.2013.06.058
inspire_id: 1232968
title:
Search for Gluino Mediated Bottom- and Top-Squark Production in Multijet Final States in pp Collisions at 8 TeV


document_id: CHATRCHYAN 2013AM
publication_name: PR D87 052006
doi: 10.1103/PhysRevD.87.052006
inspire_id: 1202674
title:
Search for Supersymmetry in Final States with a Single Lepton, b-Quark Jets, and Missing Transverse Energy in Proton-Proton Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013AV
publication_name: JHEP 1310 130
doi: 10.1007/JHEP10(2013)130
inspire_id: 1247060
title:
Search for New Phenomena in Final States with Large Jet Multiplicities and Missing Transverse Momentum at sqrt(s) = 8 TeV Proton-Proton Collisions Using the ATLAS Experiment


document_id: CHATRCHYAN 2014N
publication_name: PL B733 328
doi: 10.1016/j.physletb.2014.04.023
inspire_id: 1265220
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 8 TeV in Events with a Single Lepton, Large Jet Multiplicity, and Multiple b Jets


document_id: AAD 2014AG
publication_name: JHEP 1409 103
doi: 10.1007/JHEP09(2014)103
inspire_id: 1304458
title:
Search for Supersymmetry in Events with Large Missing Transverse Momentum,  Jets, and at least one tau Lepton in 20 fb**-1 of sqrt(s) = 8 TeV Proton-Proton Collision Data with the ATLAS Detector


document_id: AAD 2015X
publication_name: PR D91 112016
doi: 10.1103/PhysRevD.91.112016
inspire_id: 1345355
title:
Search for Massive Supersymmetric Particles Decaying to Many Jets using the ATLAS Detector in pp Collisions at sqrt(s) = 8 TeV


document_id: AAD 2015AB
publication_name: PR D92 012010
doi: 10.1103/PhysRevD.92.012010
inspire_id: 1359456
title:
Search for Long-Lived, Weakly Interacting Particles that Decay to Displaced Hadronic Jets in Proton-Proton Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2015BG
publication_name: EPJ C75 318
doi: 10.1140/epjc/s10052-015-3518-2
inspire_id: 1351762
title:
Search for Supersymmetry in Events Containing a Same-Flavour Opposite-Sign Dilepton Pair, Jets, and Large Missing Transverse Momentum in sqrt(s) = 8 TeV pp Collisions with the ATLAS Detector


document_id: AAD 2015BX
publication_name: JHEP 1510 134
doi: 10.1007/JHEP10(2015)134
inspire_id: 1389857
title:
Summary of the ATLAS Experiment's Sensitivity to Supersymmetry after LHC Run 1  Interpreted in the Phenomenological MSSM


document_id: AAD 2016V
publication_name: PL B757 334
doi: 10.1016/j.physletb.2016.04.005
inspire_id: 1422615
title:
Search for New Phenomena in Final States with Large Jet Multiplicities and Missing Transverse Momentum with ATLAS using sqrt(s) = 13 TeV Proton-Proton Collisions


document_id: KHACHATRYAN 2016V
publication_name: PL B758 152
doi: 10.1016/j.physletb.2016.05.002
inspire_id: 1422778
title:
Search for Supersymmetry in the Multijet and Missing Transverse Momentum Final State in pp Collisions at 13 TeV


document_id: KHACHATRYAN 2016AM
publication_name: PR D93 092009
doi: 10.1103/PhysRevD.93.092009
inspire_id: 1420551
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 8 TeV in Final States with Boosted W Bosons and b Jets using Razor Variables


document_id: AAD 2016AD
publication_name: PR D94 032003
doi: 10.1103/PhysRevD.94.032003
inspire_id: 1466302
title:
Search for Pair Production of Gluinos Decaying Via stop and sbottom in Events with b-Jets and Large Missing Transverse Momentum in pp Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2016AY
publication_name: JHEP 1608 122
doi: 10.1007/JHEP08(2016)122
inspire_id: 1459054
title:
Search for Supersymmetry in pp Collisions at sqrt(s) = 13 TeV in the Single-Lepton Final State using the Sum of Masses of Large-Radius Jets


document_id: AABOUD 2016M
publication_name: EPJ C76 517
doi: 10.1140/epjc/s10052-016-4344-x
inspire_id: 1473744
title:
Search for Supersymmetry in a Final State Containing Two Photons and Missing Transverse Momentum in sqrt(s) = 13 TeV pp Collisions at the LHC using the ATLAS Detector


document_id: AAD 2016BG
publication_name: EPJ C76 565
doi: 10.1140/epjc/s10052-016-4397-x
inspire_id: 1458952
title:
Search for Gluinos in Events with an Isolated Lepton, Jets and Missing Transverse Momentum at sqrt(s) = 13 Te V with the ATLAS Detector


document_id: AABOUD 2016AC
publication_name: EPJ C76 683
doi: 10.1140/epjc/s10052-016-4481-2
inspire_id: 1477209
title:
Search for Squarks and Gluinos in Events with Hadronically Decaying tau leptons, jets and Missing Transverse Momentum in Proton-Proton Collisions at sqrt(s) = 13 TeV Recorded with the ATLAS Detector


document_id: KHACHATRYAN 2017AS
publication_name: PR D95 012011
doi: 10.1103/PhysRevD.95.012011
inspire_id: 1488581
title:
Search for Supersymmetry in Events with One Lepton and Multiple Jets in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2017AZ
publication_name: JHEP 1712 034
doi: 10.1007/JHEP12(2017)034
inspire_id: 1615205
title:
Search for New Phenomena with Large Jet Multiplicities and Missing Transverse Momentum using Large-Radius Jets and Flavour-Tagging at ATLAS in 13 TeV pp Collisions


document_id: SIRUNYAN 2018M
publication_name: PRL 120 241801
doi: 10.1103/PhysRevLett.120.241801
inspire_id: 1644788
title:
Search for Physics Beyond the Standard Model in Events with High-Momentum Higgs Bosons and Missing Transverse Momentum in Proton-Proton Collisions at 13 TeV


document_id: SIRUNYAN 2018AC
publication_name: PL B780 384
doi: 10.1016/j.physletb.2018.03.028
inspire_id: 1627612
title:
Search for supersymmetry in events with one lepton and multiple jets exploiting the angular correlation between the lepton and the missing transverse momentum in proton-proton collisions at $\sqrt{s} = $ 13 TeV


document_id: SIRUNYAN 2018AK
publication_name: PL B783 114
doi: 10.1016/j.physletb.2018.06.028
inspire_id: 1644901
title:
Search for $R$-parity violating supersymmetry in pp collisions at $\sqrt{s} = $ 13 TeV using b jets in a final state with a single lepton, many jets, and high sum of large-radius jet masses


document_id: AABOUD 2018AR
publication_name: JHEP 1806 107
doi: 10.1007/JHEP06(2018)107
inspire_id: 1634607
title:
Search for supersymmetry in final states with missing transverse momentum and multiple $b$-jets in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector


document_id: AABOUD 2018CF
publication_name: PL B785 136
doi: 10.1016/j.physletb.2018.08.021
inspire_id: 1667046
title:
Search for R-parity-violating supersymmetric particles in multi-jet final states produced in $p$-$p$ collisions at $\sqrt{s} =13$ TeV using the ATLAS detector at the LHC


document_id: AABOUD 2019I
publication_name: PR D99 012009
doi: 10.1103/PhysRevD.99.012009
inspire_id: 1688943
title:
Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector


document_id: SIRUNYAN 2020E
publication_name: PR D101 052010
doi: 10.1103/PhysRevD.101.052010
inspire_id: 1765844
title:
Search for supersymmetry in pp collisions at $\sqrt{s}=$ 13 TeV with 137 fb$^{-1}$ in final states with a single lepton using the sum of masses of large-radius jets


document_id: SIRUNYAN 2020BJ
publication_name: JHEP 2009 149
doi: 10.1007/JHEP09(2020)149
inspire_id: 1811111
title:
Search for supersymmetry in proton-proton collisions at $\sqrt{s} =$ 13 TeV in events with high-momentum Z bosons and missing transverse momentum


document_id: AAD 2020AL
publication_name: JHEP 2010 062
doi: 10.1007/JHEP10(2020)062
inspire_id: 1811596
title:
Search for new phenomena in final states with large jet multiplicities and missing transverse momentum using $ \sqrt{s} $ = 13 TeV proton-proton collisions recorded by ATLAS in Run 2 of the LHC


document_id: AAD 2021X
publication_name: JHEP 2107 173
doi: 10.1007/JHEP07(2021)173
inspire_id: 1856547
title:
A search for the decays of stopped long-lived particles at $ \sqrt{\mathrm{s}} $ = 13 TeV with the ATLAS detector


document_id: AAD 2023AB
publication_name: JHEP 2307 021
doi: 10.1007/JHEP07(2023)021
inspire_id: 2094882
title:
Search for new phenomena in final states with photons, jets and missing transverse momentum in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector


document_id: AAD 2023AL
publication_name: EPJ C83 561
doi: 10.1140/epjc/s10052-023-11543-6
inspire_id: 2182381
title:
Search for supersymmetry in final states with missing transverse momentum and three or more b-jets in 139 fb$^{-1}$ of proton–proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector


document_id: TUMASYAN 2023AY
publication_name: JHEP 2309 149
doi: 10.1007/JHEP09(2023)149
inspire_id: 2182749
title:
Search for supersymmetry in final states with a single electron or muon using angular correlations and heavy-object identification in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: HAYRAPETYAN 2024P
publication_name: PR D109 112005
doi: 10.1103/PhysRevD.109.112005
inspire_id: 2761908
title:
Search for long-lived particles using displaced vertices and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: AAD 2024AF
publication_name: JHEP 2405 003
doi: 10.1007/JHEP05(2024)003
inspire_id: 2752508
title:
A search for R-parity-violating supersymmetry in final states containing many jets in $pp$ collisions at $\sqrt{s} = 13\,\text{TeV}$ with the ATLAS detector


document_id: FARRAR 1985
publication_name: PRL 55 895
doi: 10.1103/PhysRevLett.55.895
inspire_id: 16534
title:
Comment on BALL 1984 ``Mass and Lifetime Limits on Supersymmetric Particles from a Proton Beam Dump Experiment''


document_id: ARNOLD 1987
publication_name: PL B186 435
doi: 10.1016/0370-2693(87)90323-6
inspire_id: 235850
title:
Experimental Search for Associated Gluino Production and Decay in 350 GeV/c pi- Emulsion Interactions


document_id: FARRAR 1978
publication_name: PL 76B 575
doi: 10.1016/0370-2693(78)90858-4
inspire_id: 6487
title:
Phenomenology of the Production, Decay, and Detection of New Hadronic States Associated with Supersymmetry


document_id: ADAMS 1997B
publication_name: PRL 79 4083
doi: 10.1103/PhysRevLett.79.4083
inspire_id: 448840
title:
Search for Light Gluinos via the Spontaneous Appearance of pi+ pi- Pairs with an 800 GeV/c Proton Beam at Fermilab


document_id: HEISTER 2003
publication_name: EPJ C27 1
doi: 10.1140/epjc/s2002-01114-2
inspire_id: 587910
title:
Measurements of the Strong Coupling Constant and the QCD Color Factors using Four Jet Observables from Hadronic Z Decays


document_id: ABDALLAH 2003G
publication_name: EPJ C29 285
doi: 10.1140/epjc/s2003-01198-0
inspire_id: 620250
title:
A Study of the Energy Evolution of Event Shape Share Distributions and their Means with the DELPHI Detector at LEP


document_id: AABOUD 2016C
publication_name: PR D93 112015
doi: 10.1103/PhysRevD.93.112015
inspire_id: 1448101
title:
Search for Metastable Heavy Charged Particles with Large Ionization Energy Loss in pp Collisions at sqrt(s) = 13 TeV using the ATLAS Experiment


document_id: AABOUD 2018S
publication_name: PR D97 052012
doi: 10.1103/PhysRevD.97.052012
inspire_id: 1630632
title:
Search for long-lived, massive particles in events with displaced vertices and missing transverse momentum in $\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector


document_id: AABOUD 2019C
publication_name: PL B788 96
doi: 10.1016/j.physletb.2018.10.055
inspire_id: 1686832
title:
Search for heavy charged long-lived particles in proton-proton collisions at $\sqrt{s} = 13$ TeV using an ionisation measurement with the \mbox{ATLAS} detector


document_id: SIRUNYAN 2019BT
publication_name: PL B797 134876
doi: 10.1016/j.physletb.2019.134876
inspire_id: 1740108
title:
Search for long-lived particles using nonprompt jets and missing transverse momentum with proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: AFFOLDER 2000J
publication_name: PRL 85 1378
doi: 10.1103/PhysRevLett.85.1378
inspire_id: 525204
title:
Limits on Gravitino Production and New Processes with Large Missing Transverse Energy in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ACOSTA 2002H
publication_name: PRL 89 281801
doi: 10.1103/PhysRevLett.89.281801
inspire_id: 586970
title:
Limits on Extra Dimensions and New Particle Production in the Exclusive Photon and Missing Energy Signature in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABACHI 1997
publication_name: PRL 78 2070
doi: 10.1103/PhysRevLett.78.2070
inspire_id: 427309
title:
Search for Diphoton Events with Large Missing Transverse Energy in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABBOTT 2000G
publication_name: PR D62 071701
doi: 10.1103/PhysRevD.62.071701
inspire_id: 527795
title:
Search for R-Parity Violation in Multilepton Final States in p - pbar Collisions at sqrt(s) = 1.8-TeV


document_id: ACOSTA 2004E
publication_name: PRL 93 061802
doi: 10.1103/PhysRevLett.93.061802
inspire_id: 650730
title:
Inclusive Search for Anomalous Production of High pT Like-sign Lepton Pairs in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABULENCIA 2006P
publication_name: PRL 97 031801
doi: 10.1103/PhysRevLett.97.031801
inspire_id: 717570
title:
Search for New Physics in Lepton+Photon+X Events with 305 pb**-1 of p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2010N
publication_name: PRL 105 211802
doi: 10.1103/PhysRevLett.105.211802
inspire_id: 865685
title:
Search for Events with Leptonic Jets and Missing Transverse Energy in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2011AA
publication_name: EPJ C71 1828
doi: 10.1140/epjc/s10052-011-1828-6
inspire_id: 939560
title:
Search for Massive Colored Scalars in Four-Jet Final States in sqrt(s) = 7 TeV  Proton-Proton Collisions with the ATLAS Detector


document_id: AABOUD 2016AF
publication_name: JHEP 1609 175
doi: 10.1007/JHEP09(2016)175
inspire_id: 1478981
title:
Dark Matter Interpretations of ATLAS Searches for the Electroweak Production of Supersymmetric Particles in sqrt(s) = 8 TeV Proton-Proton Collisions


document_id: AAD 2024AH
publication_name: JHEP 2405 106
doi: 10.1007/JHEP05(2024)106
inspire_id: 2755168
title:
ATLAS Run 2 searches for electroweak production of supersymmetric particles interpreted within the pMSSM


document_id: ABE 1999H
publication_name: PRL 82 3206
doi: 10.1103/PhysRevLett.82.3206
inspire_id: 478880
title:
Search for Third Generation Leptoquarks from Technicolor Models in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: AFFOLDER 2000F
publication_name: PRL 84 1110
doi: 10.1103/PhysRevLett.84.1110
inspire_id: 499755
title:
Search for Technicolor Particles in Lepton Plus Two Jets and Multijet Channels in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: AAD 2015Q
publication_name: PL B743 15
doi: 10.1016/j.physletb.2015.02.015
inspire_id: 1339624
title:
Search for Pair-Produced Long-Lived Neutral Particles Decaying in the ATLAS Hadronic Calorimeter in pp Collisions at sqrt(s) = 8 TeV


document_id: BUSKULIC 1993Q
publication_name: ZPHY C59 215
doi: 10.1007/BF01566686
inspire_id: 354297
title:
Search for Contact Interactions in the Reactions e+ e- --> lepton+ lepton- and e+ e- --> gamma gamma


document_id: BOURILKOV 2001
publication_name: PR D64 071701
doi: 10.1103/PhysRevD.64.071701
inspire_id: 555541
title:
Hint for Axial Vector Contact Interactions in the Data on e+ e- --> e+ e- (gamma) at Center-of-mass Energies 192 -- 208 GeV


document_id: HOWELL 1992
publication_name: PL B291 206
doi: 10.1016/0370-2693(92)90145-T
inspire_id: 336076
title:
Cross Sections and Charged Asymmetries for e+ e- --> mu+ mu- and e+ e- --> tau+ tau- Reactions at sqrt(s) = 52-61.4 GeV


document_id: VELISSARIS 1994
publication_name: PL B331 227
doi: 10.1016/0370-2693(94)90967-9
inspire_id: 373861
title:
Measurements of Cross Section and Charge Asymmetry for e+ e- --> mu+ mu- and e+ e- --> tau+ tau- at sqrt(s) = 57.8 GeV


document_id: HAGIWARA 1989
publication_name: PL B219 369
doi: 10.1016/0370-2693(89)90406-1
inspire_id: 276591
title:
Limits on Lepton-Quark Contact Interactions from the Quark Forward-Backward Asymmetry in e+ e- Annihilation


document_id: ABBOTT 1999D
publication_name: PRL 82 4769
doi: 10.1103/PhysRevLett.82.4769
inspire_id: 480590
title:
Measurement of the High Mass Drell-Yan Cross Section and Limits on Quark Electron Compositeness Scales


document_id: CHEKANOV 2004B
publication_name: PL B591 23
doi: 10.1016/j.physletb.2004.03.081
inspire_id: 636690
title:
Search for Contact Interactions, Large Extra Dimensions and Finite Quark Radius in e p Collisions at HERA


document_id: AAD 2012AB
publication_name: PL B712 40
doi: 10.1016/j.physletb.2012.04.026
inspire_id: 1081998
title:
Search for Contact Interactions in Dilepton Events from pp Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2013E
publication_name: PR D87 015010
doi: 10.1103/PhysRevD.87.015010
inspire_id: 1198341
title:
Search for Contact Interactions and Large Extra Dimensions in Dilepton Events from pp Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2014BE
publication_name: EPJ C74 3134
doi: 10.1140/epjc/s10052-014-3134-6
inspire_id: 1305430
title:
Search for Contact Interactions and Large Extra Dimensions in the Dilepton Channel using Proton-Proton Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: SIRUNYAN 2019AC
publication_name: JHEP 1904 114
doi: 10.1007/JHEP04(2019)114
inspire_id: 1711231
title:
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: AAD 2021AU
publication_name: PRL 127 141801
doi: 10.1103/PhysRevLett.127.141801
inspire_id: 1866043
title:
Search for New Phenomena in Final States with Two Leptons and One or No $b$-Tagged Jets at $\sqrt{s} = 13$ TeV Using the ATLAS Detector


document_id: AAD 2011E
publication_name: PR D84 011101
doi: 10.1103/PhysRevD.84.011101
inspire_id: 897028
title:
Search for Contact Interactions in Dimuon Events from pp Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2011F
publication_name: PRL 106 201804
doi: 10.1103/PhysRevLett.106.201804
inspire_id: 889175
title:
Measurement of Dijet Angular Distributions and Search for Quark Compositeness in pp Collisions at sqrt(s) = 7 TeV


document_id: ARNISON 1986D
publication_name: PL B177 244
doi: 10.1016/0370-2693(86)91065-8
inspire_id: 230633
title:
Angular Distributions for High Mass Jet Pairs and a Limit on the Energy Scale of Compositeness for Quarks from the CERN p pbar Collider


document_id: ABBOTT 1999C
publication_name: PRL 82 2457
doi: 10.1103/PhysRevLett.82.2457
inspire_id: 473420
title:
The Dijet Mass Spectrum and a Search for Quark Compositeness in pbar p Collisions at sqrt(s) = 1.8 TeV


document_id: ABAZOV 2009AE
publication_name: PRL 103 191803
doi: 10.1103/PhysRevLett.103.191803
inspire_id: 824127
title:
Measurement of Dijet Angular Distributions at sqrt(s)=1.96 TeV and Searches for Quark Compositeness and Extra Spatial Dimensions


document_id: AAD 2011
publication_name: PL B694 327
doi: 10.1016/j.physletb.2010.10.021
inspire_id: 871487
title:
Search for Quark Contact Interactions in Dijet Angular Distributions in pp Collisions at sqrt(s) = 7 TeV Measured with the ATLAS Detector


document_id: CHATRCHYAN 2013AN
publication_name: PR D87 052017
doi: 10.1103/PhysRevD.87.052017
inspire_id: 1215599
title:
Search for Contact Interactions using the Inclusive Jet pT Spectrum in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2015L
publication_name: PRL 114 221802
doi: 10.1103/PhysRevLett.114.221802
inspire_id: 1357594
title:
Search for New Phenomena in Dijet Angular Distributions in Proton-Proton Collisions at sqrt(s) = 8 TeV Measured with the ATLAS Detector


document_id: KHACHATRYAN 2015J
publication_name: PL B746 79
doi: 10.1016/j.physletb.2015.04.042
inspire_id: 1327224
title:
Search for Quark Contact Interactions and Extra Spatial Dimensions using Dijet Angular Distributions in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: SIRUNYAN 2017F
publication_name: JHEP 1707 013
doi: 10.1007/JHEP07(2017)013
inspire_id: 1519995
title:
Search for New Physics with Dijet Angular Distributions in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2018AV
publication_name: JHEP 1807 089
doi: 10.1007/JHEP07(2018)089
inspire_id: 1664317
title:
Search for pair production of up-type vector-like quarks and for four-top-quark events in final states with multiple $b$-jets with the ATLAS detector


document_id: SIRUNYAN 2018DD
publication_name: EPJ C78 789
doi: 10.1140/epjc/s10052-018-6242-x
inspire_id: 1663452
title:
Search for new physics in dijet angular distributions using proton–proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models


document_id: ABREU 1996K
publication_name: PL B380 480
doi: 10.1016/0370-2693(96)00672-7
inspire_id: 418939
title:
Study of Radiative Leptonic Events with Hard Photons and Search for Excited Charged Leptons at sqrt(s) = 130-136 GeV


document_id: GOLUBEV 1985B
publication_name: SJNP 41 752
inspire_id: 202873
title:
Test of Quantum Electrodynamics in the Compton Scattering of Quasireal Photons by Electrons and Positrons at the VEPP-2M Storage Ring


document_id: ACOSTA 2005B
publication_name: PRL 94 101802
doi: 10.1103/PhysRevLett.94.101802
inspire_id: 661115
title:
Search for Excited and Exotic Electrons in the e gamma Decay Channel in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2013BB
publication_name: NJP 15 093011
doi: 10.1088/1367-2630/15/9/093011
inspire_id: 1246787
title:
Search for Excited Electrons and Muons in sqrt(s) = 8 TeV Proton-Proton Collisions with the ATLAS Detector


document_id: SIRUNYAN 2019Z
publication_name: JHEP 1904 015
doi: 10.1007/JHEP04(2019)015
inspire_id: 1702433
title:
Search for excited leptons in $\ell\ell\gamma$ final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AABOUD 2019AZ
publication_name: EPJ C79 803
doi: 10.1140/epjc/s10052-019-7295-1
inspire_id: 1738845
title:
Search for excited electrons singly produced in proton–proton collisions at $\sqrt{s}=13$ TeV with the ATLAS experiment at the LHC


document_id: SIRUNYAN 2020AJ
publication_name: JHEP 2005 052
doi: 10.1007/JHEP05(2020)052
inspire_id: 1775563
title:
Search for an excited lepton that decays via a contact interaction to a lepton and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: HANSON 1973
publication_name: LNC 7 587
doi: 10.1007/BF02727692
inspire_id: 85407
title:
Experimental Test of Quantum Electrodynamics for the Reaction e+ e- --> gamma gamma at 4 GeV Center-of-mass Energy


document_id: ABREU 2000A
publication_name: PL B491 67
doi: 10.1016/S0370-2693(00)01013-3
inspire_id: 534257
title:
Determination of the e+ e- --> gamma gamma ( gamma ) Cross Section at Ecm Ranging from 189 to 202 GeV


document_id: ABULENCIA,A 2006B
publication_name: PRL 97 191802
doi: 10.1103/PhysRevLett.97.191802
inspire_id: 719681
title:
Search for Excited and Exotic Muons in the mu gamma Decay Channel in p pbar Collisions at sqrt(s)=1.96 TeV


document_id: AAD 2016BM
publication_name: NJP 18 073021
doi: 10.1088/1367-2630/18/7/073021
inspire_id: 1416473
title:
A Search for an Excited Muon Decaying to a Muon and Two Jets in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: TUMASYAN 2023AL
publication_name: PL B843 137803
doi: 10.1016/j.physletb.2023.137803
inspire_id: 2671384
title:
Search for a heavy composite Majorana neutrino in events with dilepton signatures from proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: ABAZOV 2006F
publication_name: PR D74 011104
doi: 10.1103/PhysRevD.74.011104
inspire_id: 718809
title:
Search for a Heavy Resonance Decaying into a Z+jet Final State in p pbar Collisions at sqrt(s) =1.96 TeV using the D0 Detector


document_id: AAD 2010
publication_name: PRL 105 161801
doi: 10.1103/PhysRevLett.105.161801
inspire_id: 865423
title:
Search for New Particles in Two-Jet Final States in 7 TeV Proton-Proton Collisions with the ATLAS Detector at the LHC


document_id: AAD 2012S
publication_name: PL B708 37
doi: 10.1016/j.physletb.2012.01.035
inspire_id: 925933
title:
Search for New Physics in the Dijet Mass Distribution using 1 fb^{-1} of pp Collision Data at sqrt(s) = 7 TeV Collected by the ATLAS Detector


document_id: AAD 2012AO
publication_name: PRL 108 211802
doi: 10.1103/PhysRevLett.108.211802
inspire_id: 1081556
title:
Search for Production of Resonant States in the Photon-Jet Mass Distribution Using pp Collisions at sqrt(s) = 7 TeV Collected by the ATLAS Detector


document_id: CHATRCHYAN 2013AI
publication_name: PL B722 28
doi: 10.1016/j.physletb.2013.03.037
inspire_id: 1189049
title:
Search for Anomalous Production of Highly Boosted Z Bosons Decaying to Dimuons in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2014A
publication_name: PL B728 562
doi: 10.1016/j.physletb.2013.12.029
inspire_id: 1253852
title:
Search for New Phenomena in Photon + Jet Events Collected in Proton-Proton Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2014J
publication_name: PL B738 274
doi: 10.1016/j.physletb.2014.09.048
inspire_id: 1301560
title:
Search for Excited Quarks in the gamma + Jet Final State in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2016AI
publication_name: JHEP 1603 041
doi: 10.1007/JHEP03(2016)041
inspire_id: 1410580
title:
Search for New Phenomena with Photon + Jet Events in Proton-Proton Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: SIRUNYAN 2018AG
publication_name: PL B781 390
doi: 10.1016/j.physletb.2018.04.007
inspire_id: 1635896
title:
Search for excited quarks of light and heavy flavor in $\gamma +$ jet final states in proton–proton collisions at $\sqrt{s} =$ 13TeV


document_id: AABOUD 2018BA
publication_name: EPJ C78 102
doi: 10.1140/epjc/s10052-018-5553-2
inspire_id: 1627878
title:
Search for new phenomena in high-mass final states with a photon and a jet from $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector


document_id: TUMASYAN 2023BC
publication_name: JHEP 2312 189
doi: 10.1007/JHEP12(2023)189
inspire_id: 2659689
title:
Search for resonances in events with photon and jet final states in proton-proton collisions at $\sqrt{s}$= 13 TeV


document_id: BARTEL 1985K
publication_name: PL 160B 337
doi: 10.1016/0370-2693(85)91339-5
inspire_id: 216799
title:
A Measurement of the Total Cross Section and a Study of Inclusive Muon Production for the Process e+ e- --> hadrons in the Energy Range between 39.79 and 46.78 GeV


document_id: BEZERRA 2011
publication_name: PR D83 075004
doi: 10.1103/PhysRevD.83.075004
inspire_id: 891653
title:
Constraints on non-Newtonian Gravity from Measuring the Casimir Force in a Configuration with Nanoscale Rectangular Corrugations


document_id: HOYLE 2001
publication_name: PRL 86 1418
doi: 10.1103/PhysRevLett.86.1418
inspire_id: 536102
title:
Submillimeter Tests of the Gravitational Inverse Square Law: a Search for ``Large'' Extra Dimensions


document_id: TU 2007
publication_name: PRL 98 201101
doi: 10.1103/PhysRevLett.98.201101
inspire_id: 776368
title:
Null Test of Newtonian Inverse-Square Law at Submillimeter Range with a Dual-Modulation Torsion Pendulum


document_id: DECCA 2007A
publication_name: EPJ C51 963
doi: 10.1140/epjc/s10052-007-0346-z
inspire_id: 753887
title:
Novel Constraints on Light Elementary Particles and Extra-Dimensional Physics from the Casimir Effect


document_id: TRENKEL 2008
publication_name: PR D77 122001
doi: 10.1103/PhysRevD.77.122001
inspire_id: 788581
title:
Constraints on Composition Independent Yukawa Interactions Inferred from Measurements of the Newtonian Gravitational Constant


document_id: BEZERRA 2010
publication_name: PR D81 055003
doi: 10.1103/PhysRevD.81.055003
inspire_id: 845509
title:
Advance and Prospects in Constraining the Yukawa-type Corrections to Newtonian Gravity from the Casimir Effect


document_id: BERGE 2018
publication_name: PRL 120 141101
doi: 10.1103/PhysRevLett.120.141101
inspire_id: 1640573
title:
MICROSCOPE Mission: First Constraints on the Violation of the Weak Equivalence Principle by a Light Scalar Dilaton


document_id: HADDOCK 2018
publication_name: PR D97 062002
doi: 10.1103/PhysRevD.97.062002
inspire_id: 1642267
title:
Search for deviations from the inverse square law of gravity at nm range using a pulsed neutron beam


document_id: HANHART 2001
publication_name: PL B509 1
doi: 10.1016/S0370-2693(01)00544-5
inspire_id: 552813
title:
The Likelihood of GODs' Existence: Improving the SN1987a Constraint on the Size of Large Compact Dimensions


document_id: ACOSTA 2004C
publication_name: PRL 92 121802
doi: 10.1103/PhysRevLett.92.121802
inspire_id: 628308
title:
Search for Kaluza-Klein Graviton Emission in p pbar Collisions at sqrt(s) = 1.8 TeV using the Missing Energy Signature


document_id: ABULENCIA,A 2006
publication_name: PRL 97 171802
doi: 10.1103/PhysRevLett.97.171802
inspire_id: 715041
title:
Search for Large Extra Dimensions in the Production of Jets and Missing Transverse Energy in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2008S
publication_name: PRL 101 011601
doi: 10.1103/PhysRevLett.101.011601
inspire_id: 781380
title:
Search for Large Extra Dimensions via Single Photon Plus Missing Energy Final States at sqrt(s) = 1.96 TeV


document_id: DAS 2008
publication_name: PR D78 063011
doi: 10.1103/PhysRevD.78.063011
inspire_id: 777050
title:
Plasmon Annihilation into Kaluza-Klein Gravitons: New Astrophysical Constraints on Large Extra Dimensions?


document_id: AALTONEN 2008AC
publication_name: PRL 101 181602
doi: 10.1103/PhysRevLett.101.181602
inspire_id: 791132
title:
Search for Large Extra Dimensions in Final States Containing one Photon or Jet and Large Missing Transverse Energy Produced in p pbar Collisions at sqrt(s) = 1.96TeV


document_id: CHATRCHYAN 2011U
publication_name: PRL 107 201804
doi: 10.1103/PhysRevLett.107.201804
inspire_id: 914953
title:
Search for New Physics with a Monojet and Missing Transverse Energy in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2011S
publication_name: PL B705 294
doi: 10.1016/j.physletb.2011.10.006
inspire_id: 915920
title:
Search for New Phenomena with the Monojet and Missing Transverse Momentum Signature using the ATLAS Detector in sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: CHATRCHYAN 2012AP
publication_name: JHEP 1209 094
doi: 10.1007/JHEP09(2012)094
inspire_id: 1119567
title:
Search for Dark Matter and Large Extra Dimensions in Monojet Events in pp Collisions at sqrt(s) = 7 TeV


document_id: AAD 2013C
publication_name: PRL 110 011802
doi: 10.1103/PhysRevLett.110.011802
inspire_id: 1186740
title:
Search for Dark Matter Candidates and Large Extra Dimensions in Events with a Photon and Missing Transverse Momentum in pp Collision Data at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2013AD
publication_name: JHEP 1304 075
doi: 10.1007/JHEP04(2013)075
inspire_id: 1190892
title:
Search for Dark Matter Candidates and Large Extra Dimensions in Events with a Jet and Missing Transverse Momentum with the ATLAS Detector


document_id: KHACHATRYAN 2015AL
publication_name: EPJ C75 235
doi: 10.1140/epjc/s10052-015-3451-4
inspire_id: 1311223
title:
Search for Dark Matter, Extra Dimensions, and Unparticles in Monojet Events in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AABOUD 2016F
publication_name: JHEP 1606 059
doi: 10.1007/JHEP06(2016)059
inspire_id: 1442359
title:
Search for New Phenomena in Events with a Photon and Missing Transverse Momentum in pp Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: SIRUNYAN 2017AQ
publication_name: JHEP 1710 073
doi: 10.1007/JHEP10(2017)073
inspire_id: 1604886
title:
Search for New Physics in the Monophoton Final State in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: GERDES 2006
publication_name: PR D73 112008
doi: 10.1103/PhysRevD.73.112008
inspire_id: 712735
title:
Search for Large Extra Dimensions using Dielectron and Diphoton Events in p pbar Collisions at sqrt(s) = 1.8 TeV


document_id: ABAZOV 2009D
publication_name: PRL 102 051601
doi: 10.1103/PhysRevLett.102.051601
inspire_id: 796811
title:
Search for Large Extra Spatial Dimensions in the Dielectron and Diphoton Channels in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2012Y
publication_name: PL B710 538
doi: 10.1016/j.physletb.2012.03.022
inspire_id: 1080740
title:
Search for Extra Dimensions using Diphoton Events in 7 TeV Proton-Proton Collisions with the ATLAS Detector


document_id: CHATRCHYAN 2012J
publication_name: PL B711 15
doi: 10.1016/j.physletb.2012.03.029
inspire_id: 1089399
title:
Search for Large Extra Dimensions in Dimuon and Dielectron Events in pp Collisions at sqrt(s) = 7 TeV


document_id: CHATRCHYAN 2012R
publication_name: PRL 108 111801
doi: 10.1103/PhysRevLett.108.111801
inspire_id: 1079910
title:
Search for Signatures of Extra Dimensions in the Diphoton Mass Spectrum at the Large Hadron Collider


document_id: AAD 2013AS
publication_name: NJP 15 043007
doi: 10.1088/1367-2630/15/4/043007
inspire_id: 1197323
title:
Search for Extra Dimensions in Diphoton Events Using Proton-Proton Collisions Recorded at sqrt(s) = 7 TeV with the ATLAS Detector at the LHC


document_id: AAD 2011F
publication_name: PRL 106 121803
doi: 10.1103/PhysRevLett.106.121803
inspire_id: 881812
title:
Search for Diphoton Events with Large Missing Transverse Energy in 7 TeV Proton-Proton Collisions with the ATLAS Detector


document_id: AALTONEN 2011G
publication_name: PR D83 112008
doi: 10.1103/PhysRevD.83.112008
inspire_id: 890324
title:
Search for New Heavy Particles Decaying to ZZ --> llll, lljj in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AALTONEN 2011R
publication_name: PRL 107 051801
doi: 10.1103/PhysRevLett.107.051801
inspire_id: 893813
title:
Search for New Dielectron Resonances and Randall-Sundrum Gravitons at the Collider Detector at Fermilab


document_id: AALTONEN 2008S
publication_name: PR D78 012008
doi: 10.1103/PhysRevD.78.012008
inspire_id: 776993
title:
Search for New Heavy Particles Decaying to Z0 Z0 --> e e e e in p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2008J
publication_name: PRL 100 091802
doi: 10.1103/PhysRevLett.100.091802
inspire_id: 764554
title:
Search for Randall-Sundrum Gravitons with 1 fb^{-1} of Data from p pbar Collisions at sqrt(s) = 1.96 TeV


document_id: ABAZOV 2010F
publication_name: PRL 104 241802
doi: 10.1103/PhysRevLett.104.241802
inspire_id: 851527
title:
Search for Randall-Sundrum Gravitons in the Dielectron and Diphoton Final States with 5.4 fb**-1 of Data from p pbar Collisions at sqrt(s) = 1.96TeV


document_id: AAD 2012AD
publication_name: PL B712 331
doi: 10.1016/j.physletb.2012.05.020
inspire_id: 1092728
title:
Search for New Particles Decaying to ZZ using Final States with Leptons and Jets with the ATLAS Detector in sqrt(s) = 7 TeV Proton-Proton Collisions


document_id: AAD 2013A
publication_name: PL B718 860
doi: 10.1016/j.physletb.2012.11.040
inspire_id: 1127504
title:
Search for New Phenomena in the W W --> lepton nu lepton^' nu^' Final State in pp Collisions at sqrt(s) = 7 TeV with the ATLAS Detector


document_id: AAD 2015AD
publication_name: PR D92 032004
doi: 10.1103/PhysRevD.92.032004
inspire_id: 1362490
title:
Search for High-Mass Diphoton Resonances in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: SIRUNYAN 2019CF
publication_name: JHEP 1910 125
doi: 10.1007/JHEP10(2019)125
inspire_id: 1728701
title:
Search for resonances decaying to a pair of Higgs bosons in the $\mathrm{b\overline{b}q\overline{q}'}\ell\nu$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: SIRUNYAN 2020F
publication_name: PR D102 032003
doi: 10.1103/PhysRevD.102.032003
inspire_id: 1800735
title:
Search for resonant pair production of Higgs bosons in the bbZZ channel in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: TUMASYAN 2022U
publication_name: JHEP 2205 005
doi: 10.1007/JHEP05(2022)005
inspire_id: 1984855
title:
Search for heavy resonances decaying to a pair of Lorentz-boosted Higgs bosons in final states with leptons and a bottom quark pair at $ \sqrt{s} $= 13 TeV


document_id: TUMASYAN 2022C
publication_name: PL B832 137263
doi: 10.1016/j.physletb.2022.137263
inspire_id: 2005439
title:
Search for high-mass resonances decaying to a jet and a Lorentz-boosted resonance in proton-proton collisions at <math altimg=\"si1.svg\"><msqrt><mrow><mi>s</mi></mrow></msqrt><mo linebreak=\"goodbreak\" linebreakstyle=\"after\">=</mo><mn>13</mn><mspace width=\"0.2em\"/><mtext>TeV</mtext></math>


document_id: AAD 2013AW
publication_name: PR D88 072001
doi: 10.1103/PhysRevD.88.072001
inspire_id: 1249597
title:
Search for Microscopic Black Holes in a Like-Sign Dimuon final State using Large Track Multiplicity with the ATLAS Detector


document_id: AAD 2016N
publication_name: JHEP 1603 026
doi: 10.1007/JHEP03(2016)026
inspire_id: 1408744
title:
Search for Strong Gravity in Multijet Final States Produced in pp Collisions at sqrt(s) = 13 TeV using the ATLAS Detector at the LHC


document_id: AAD 2016O
publication_name: PL B760 520
doi: 10.1016/j.physletb.2016.07.030
inspire_id: 1468067
title:
Search for TeV-Scale Gravity Signatures in High-Mass Final States with Leptons and Jets with the ATLAS Detector at sqrt(s) = 13 TeV


document_id: SIRUNYAN 2018DA
publication_name: JHEP 1811 042
doi: 10.1007/JHEP11(2018)042
inspire_id: 1673362
title:
Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV


document_id: SIRUNYAN 2017CP
publication_name: PL B774 279
doi: 10.1016/j.physletb.2017.09.053
inspire_id: 1598036
title:
Search for black holes in high-multiplicity final states in proton-proton collisions at $ \\sqrt{s}=$13 TeV


document_id: AAD 2014AL
publication_name: PRL 112 091804
doi: 10.1103/PhysRevLett.112.091804
inspire_id: 1263762
title:
Search for Quantum Black Hole Production in High-Invariant-Mass Lepton+Jet Final States using pp Collisions at sqrt(s) = 8 TeV and the ATLAS Detector


document_id: AAD 2024S
publication_name: PR D109 032010
doi: 10.1103/PhysRevD.109.032010
inspire_id: 2682338
title:
Search for quantum black hole production in lepton+jet final states using proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector


document_id: JIANG 2018
publication_name: PRL 120 241301
doi: 10.1103/PhysRevLett.120.241301
inspire_id: 1657385
title:
Limits on Light Weakly Interacting Massive Particles from the First 102.8 kg ${\times}$ day Data of the CDEX-10 Experiment


document_id: YANG 2018
publication_name: CP C42 023002
doi: 10.1088/1674-1137/42/2/023002
inspire_id: 1631331
title:
Limits on light WIMPs with a 1 kg-scale germanium detector at 160 eVee physics threshold at the China Jinping Underground Laboratory


document_id: LIU 2019B
publication_name: PRL 123 161301
doi: 10.1103/PhysRevLett.123.161301
inspire_id: 1732511
title:
Constraints on Spin-Independent Nucleus Scattering with sub-GeV Weakly Interacting Massive Particle Dark Matter from the CDEX-1B Experiment at the China Jinping Underground Laboratory


document_id: APRILE 2019C
publication_name: PRL 123 241803
doi: 10.1103/PhysRevLett.123.241803
inspire_id: 1747114
title:
Search for Light Dark Matter Interactions Enhanced by the Migdal effect or Bremsstrahlung in XENON1T


document_id: AGUILAR-AREVALO 2020C
publication_name: PRL 125 241803
doi: 10.1103/PhysRevLett.125.241803
inspire_id: 1809457
title:
Results on low-mass weakly interacting massive particles from a 11 kg-day target exposure of DAMIC at SNOLAB


document_id: APRILE 2021
publication_name: PRL 126 091301
doi: 10.1103/PhysRevLett.126.091301
inspire_id: 1835591
title:
Search for Coherent Elastic Scattering of Solar $^8$B Neutrinos in the XENON1T Dark Matter Experiment


document_id: AKERIB 2021A
publication_name: PR D104 012011
doi: 10.1103/PhysRevD.104.012011
inspire_id: 1831397
title:
Improving sensitivity to low-mass dark matter in LUX using a novel electrode background mitigation technique


document_id: XU 2022
publication_name: PR D106 052008
doi: 10.1103/PhysRevD.106.052008
inspire_id: 2001953
title:
Constraints on sub-GeV dark matter boosted by cosmic rays from the CDEX-10 experiment at the China Jinping Underground Laboratory


document_id: ARMENGAUD 2022
publication_name: PR D106 062004
doi: 10.1103/PhysRevD.106.062004
inspire_id: 2048590
title:
Search for sub-GeV dark matter via the Migdal effect with an EDELWEISS germanium detector with NbSi transition-edge sensors


document_id: LIN 2009
publication_name: PR D79 061101
doi: 10.1103/PhysRevD.79.061101
inspire_id: 770155
title:
New Limits on Spin-Independent and Spin-Dependent Couplings of Low-Mass WIMP Dark Matter with a Germanium Detector at a Threshold of 220 eV


document_id: ZHAO 2013
publication_name: PR D88 052004
doi: 10.1103/PhysRevD.88.052004
inspire_id: 1238907
title:
First Results on Low-Mass WIMP from the CDEX-1 Experiment at the China Jinping Underground Laboratory


document_id: LIU 2014A
publication_name: PR D90 032003
doi: 10.1103/PhysRevD.90.032003
inspire_id: 1286737
title:
Limits on Light WIMPs with a Germanium Detector at 177 eVee (electron equivalent) Threshold at the China Jinping Underground Laboratory


document_id: YUE 2014
publication_name: PR D90 091701
doi: 10.1103/PhysRevD.90.091701
inspire_id: 1291361
title:
Limits on Light WIMPs from the CDEX-1 Experiment with a p-Type Point-Contact Germanium Detector at the China Jingping Underground Laboratory


document_id: AGNESE 2014A
publication_name: PRL 112 041302
doi: 10.1103/PhysRevLett.112.041302
inspire_id: 1253835
title:
CDMSlite: A Search for Low-Mass WIMPs using Voltage-Assisted Calorimetric Ionization Detection in the SuperCDMS Experiment


document_id: AGNESE 2016
publication_name: PRL 116 071301
doi: 10.1103/PhysRevLett.116.071301
inspire_id: 1392432
title:
New Results from the Search for Low-Mass Weakly Interacting Massive Particles with the CDMS Low Ionization Threshold Experiment


document_id: BARBOSA-DE-SOUZA 2017
publication_name: PR D95 032006
doi: 10.1103/PhysRevD.95.032006
inspire_id: 1422186
title:
First Search for a Dark Matter Annual Modulation Signal with NaI(Tl) in the Southern Hemisphere by DM-Ice17


document_id: KIM 2019A
publication_name: JHEP 1903 194
doi: 10.1007/JHEP03(2019)194
inspire_id: 1678354
title:
Limits on Interactions between Weakly Interacting Massive Particles and Nucleons Obtained with NaI(Tl) crystal Detectors


document_id: YANG 2019
publication_name: PRL 123 221301
doi: 10.1103/PhysRevLett.123.221301
inspire_id: 1732624
title:
Search for Light Weakly-Interacting-Massive-Particle Dark Matter by Annual Modulation Analysis with a Point-Contact Germanium Detector at the China Jinping Underground Laboratory


document_id: GIULIANI 2005
publication_name: PRL 95 101301
doi: 10.1103/PhysRevLett.95.101301
inspire_id: 680731
title:
Are Direct Search Experiments Sensitive to All Spin-Independent Weakly Interacting Massive Particles?


document_id: AJELLO 2011
publication_name: PR D84 032007
doi: 10.1103/PhysRevD.84.032007
inspire_id: 919394
title:
Constraints on Dark Matter Models from a Fermi LAT Search for High-Energy Cosmic-Ray Electrons from the Sun


document_id: ADHIKARI 2020
publication_name: PR D102 082001
doi: 10.1103/PhysRevD.102.082001
inspire_id: 1798532
title:
Constraints on dark matter-nucleon effective couplings in the presence of kinematically distinct halo substructures using the DEAP-3600 detector


document_id: ABREU 2023
publication_name: PRL 130 061001
doi: 10.1103/PhysRevLett.130.061001
inspire_id: 2054096
title:
Limits to Gauge Coupling in the Dark Sector Set by the Nonobservation of Instanton-Induced Decay of Super-Heavy Dark Matter in the Pierre Auger Observatory Data


document_id: ABDELHAMEED 2020A
publication_name: EPJ C80 834
doi: 10.1140/epjc/s10052-020-8329-4
inspire_id: 1794516
title:
Cryogenic characterization of a $\hbox {LiAlO}_{2}$ crystal and new results on spin-dependent dark matter interactions with ordinary matter


document_id: MIUCHI 2003
publication_name: ASP 19 135
doi: 10.1016/S0927-6505(02)00192-5
inspire_id: 585924
title:
First Results from Dark Matter Search Experiment with LiF Bolometer at Kamioka Underground Laboratory


document_id: AHLEN 2011
publication_name: PL B695 124
doi: 10.1016/j.physletb.2010.11.041
inspire_id: 858353
title:
First Dark Matter Search Results from a Surface Run of the 10-L DMTPC (Dark Matter Time Projection Chamber) Directional Dark Matter Detector


document_id: KHACHATRYAN 2016AJ
publication_name: PR D93 052011
doi: 10.1103/PhysRevD.93.052011
inspire_id: 1407148
title:
Search for Dark Matter and Unparticles Produced in Association with a Z Boson in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: FU 2018
publication_name: PRL 120 049902 (errat.)
doi: 10.1103/PhysRevLett.120.049902
inspire_id: 1499474
title:
Spin-Dependent Weakly-Interacting-Massive-Particle?Nucleon Cross Section Limits from First Data of PandaX-II Experiment


document_id: ABBASI 2010
publication_name: PR D81 057101
doi: 10.1103/PhysRevD.81.057101
inspire_id: 834994
title:
Limits on a Muon Flux  from Kaluza-Klein Dark Matter Annihilations in the Sun from the IceCube 22-string Detector


document_id: ABRAMOFF 2019
publication_name: PRL 122 161801
doi: 10.1103/PhysRevLett.122.161801
inspire_id: 1717756
title:
SENSEI: Direct-Detection Constraints on Sub-GeV Dark Matter from a Shallow Underground Run Using a Prototype Skipper-CCD


document_id: AGOSTINI 2022A
publication_name: PRL 129 089901
doi: 10.1103/PhysRevLett.129.089901
inspire_id: 1798379
title:
First Search for Bosonic Superweakly Interacting Massive Particles with Masses up to 1  MeV/$c^2$ with GERDA


document_id: ZHANG 2024A
publication_name: PRL 132 171001
doi: 10.1103/PhysRevLett.132.171001
inspire_id: 2703052
title:
Experimental Limits on Solar Reflected Dark Matter with a New Approach on Accelerated Dark Matter-Electron Analysis in Semiconductors


document_id: QUENBY 1995
publication_name: PL B351 70
doi: 10.1016/0370-2693(95)00355-O
inspire_id: 405549
title:
Results from the First Stage of a UK Galactic Dark Matter Search using Low Background Sodium Iodide Detectors


document_id: SMITH 1996
publication_name: PL B379 299
doi: 10.1016/0370-2693(96)00350-4
inspire_id: 429761
title:
Improved Dark Matter Limits from Pulse Shape Discrimination in a Low Background Sodium Iodide Detector at the Boulby Mine


document_id: ALESSANDRELLO 1996
publication_name: PL B384 316
doi: 10.1016/0370-2693(96)00573-4
inspire_id: 431914
title:
Preliminary Results on the Performance of a TeO(2) Thermal Detector in a Search for Direct Interactions of WIMPs


document_id: BELLI 2000
publication_name: PR D61 023512
doi: 10.1103/PhysRevD.61.023512
inspire_id: 497413
title:
Extending the DAMA Annual Modulation Region by Inclusion of the Uncertainties in the Astrophysical Velocities


document_id: BELLI 2002
publication_name: PR D66 043503
doi: 10.1103/PhysRevD.66.043503
inspire_id: 584648
title:
Effect of the Galactic Halo Modeling on the DAMA/NaI Annual Modulation Result: an Extended Analysis of the Data for WIMPs with a Purely Spin Independent Coupling


document_id: SAVAGE 2004
publication_name: PR D70 123513
doi: 10.1103/PhysRevD.70.123513
inspire_id: 656949
title:
Can WIMP Spin Dependent Couplings Explain DAMA Data, in Light of Null Results from other Experiments?


document_id: DERBIN 1999
publication_name: PAN 62 1886
inspire_id: 514920
title:
Searches for Strongly Interacting Massive Particles by Means of Semiconductor Detectors Positioned on the Earth's Surface


document_id: BERNABEI 1999D
publication_name: PRL 83 4918
doi: 10.1103/PhysRevLett.83.4918
inspire_id: 513688
title:
Extended Limits on Neutral Strongly Interacting Massive Particles and Nuclearites from NaI(Tl) Scintillators


document_id: APRILE 2017D
publication_name: PR D96 042004
doi: 10.1103/PhysRevD.96.042004
inspire_id: 1598422
title:
Effective Field Theory Search for High-Energy Nuclear Recoils using the XENON100 Dark Matter Detector


document_id: ADHIKARI 2022
publication_name: PRL 128 011801
doi: 10.1103/PhysRevLett.128.011801
inspire_id: 1909079
title:
First Direct Detection Constraints on Planck-Scale Mass Dark Matter with Multiple-Scatter Signatures Using the DEAP-3600 Detector


document_id: ADAMS 2023
publication_name: PR D108 062003
doi: 10.1103/PhysRevD.108.062003
inspire_id: 2625689
title:
Search for inelastic dark matter-nucleus scattering with the PICO-60 CF$_{3}$I and C$_{3}$F$_{8}$ bubble chambers


document_id: ACKERMANN 2011
publication_name: PRL 107 241302
doi: 10.1103/PhysRevLett.107.241302
inspire_id: 924256
title:
Constraining Dark Matter Models from a Combined Analysis of Milky Way Satellites with the Fermi Large Area Telescope


document_id: ACKERMANN 2012
publication_name: PR D86 022002
doi: 10.1103/PhysRevD.86.022002
inspire_id: 1114411
title:
Fermi LAT (Large Area Telescope) Search for Dark Matter in Gamma-Ray Lines and the Inclusive Photon Spectrum


document_id: ACKERMANN 2013A
publication_name: PR D88 082002
doi: 10.1103/PhysRevD.88.082002
inspire_id: 1235384
title:
Search for Gamma-Ray Spectral Lines with the Fermi Large Area Telescope and Dark  Matter Implications


document_id: ACKERMANN 2014
publication_name: PR D89 042001
doi: 10.1103/PhysRevD.89.042001
inspire_id: 1256578
title:
Dark Matter Constraints from Observations of 25 Milky Way Satellite Galaxies with the Fermi Large Area Telescope


document_id: LI 2016
publication_name: PR D93 043518
doi: 10.1103/PhysRevD.93.043518
inspire_id: 1407111
title:
Search for Gamma-Ray Emission from Eight dwarf Spheroidal Galaxy Candidates Discovered in Year Two of Dark Energy Survey with Fermi-LAT Data


document_id: CAPUTO 2016
publication_name: PR D93 062004
doi: 10.1103/PhysRevD.93.062004
inspire_id: 1425917
title:
Search for Gamma-ray Emission from Dark Matter Annihilation in the Small Magellanic Cloud with the Fermi Large Area Telescope


document_id: SHIRASAKI 2016
publication_name: PR D94 063522
doi: 10.1103/PhysRevD.94.063522
inspire_id: 1474652
title:
Cosmological Constraints on Dark Matter Annihilation and Decay: Cross-Correlation Analysis of the Extragalactic gamma-ray Background and Cosmic Shear


document_id: FORNASA 2016
publication_name: PR D94 123005
doi: 10.1103/PhysRevD.94.123005
inspire_id: 1484138
title:
Angular Power Spectrum of the Diffuse Gamma-Ray Emission as Measured by the Fermi Large Area Telescope and Constraints on its Dark Matter Interpretation


document_id: AVRORIN 2017
publication_name: JETP 125 80
doi: 10.1134/S1063776117070135
inspire_id: 1502894
title:
Dark Matter Constraints from an Observation of dSphs (dwarf spheroidal galaxies) and the LMC (Large Magellanic Cloud) with the Baikal NT200


document_id: BISWAS 2017
publication_name: JCAP 1711 003
doi: 10.1088/1475-7516/2017/11/003
inspire_id: 1597379
title:
Constraints on Dark Matter Models from the Observation of Triangulum-II with the Fermi Large Area Telescope


document_id: LI 2018B
publication_name: PR D97 122001
doi: 10.1103/PhysRevD.97.122001
inspire_id: 1673727
title:
Search for gamma-ray emission from the nearby dwarf spheroidal galaxies with 9 years of Fermi-LAT data


document_id: MAZZIOTTA 2018
publication_name: PR D98 022006
doi: 10.1103/PhysRevD.98.022006
inspire_id: 1644077
title:
Search for features in the cosmic-ray electron and positron spectrum measured by the Fermi Large Area Telescope


document_id: QUEIROZ 2019
publication_name: JCAP 1904 048
doi: 10.1088/1475-7516/2019/04/048
inspire_id: 1717733
title:
Search for Semi-Annihilating Dark Matter with Fermi-LAT, H.E.S.S., Planck, and the Cherenkov Telescope Array


document_id: MAZZIOTTA 2020
publication_name: PR D102 022003
doi: 10.1103/PhysRevD.102.022003
inspire_id: 1799946
title:
Search for dark matter signatures in the gamma-ray emission towards the Sun with the Fermi Large Area Telescope


document_id: GUO 2023
publication_name: PR D107 103011
doi: 10.1103/PhysRevD.107.103011
inspire_id: 2159103
title:
Constraints on dark matter annihilation from the FAST observation of the Coma Berenices dwarf galaxy


document_id: CAO 2024
publication_name: PRL 133 061001
doi: 10.1103/PhysRevLett.133.061001
inspire_id: 2797786
title:
Constraints on Ultra Heavy Dark Matter Properties from Dwarf Spheroidal Galaxies with LHAASO Observations


document_id: ZAKHAROV 2024A
publication_name: PR D110 123026
doi: 10.1103/PhysRevD.110.123026
inspire_id: 2811334
title:
Constraints on the parameters of keV-scale mass annihilating Dark Matter obtained with SRG/ART-XC observations


document_id: ACHARYYA 2024
publication_name: PR D110 063034
doi: 10.1103/PhysRevD.110.063034
inspire_id: 2810562
title:
An indirect search for dark matter with a combined analysis of dwarf spheroidal galaxies from VERITAS


document_id: AALTONEN 2012K
publication_name: PRL 108 201802
doi: 10.1103/PhysRevLett.108.201802
inspire_id: 1090723
title:
Search for a Dark Matter Candidate Produced in Association with a Single Top Quark in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AALTONEN 2012M
publication_name: PRL 108 211804
doi: 10.1103/PhysRevLett.108.211804
inspire_id: 1092730
title:
Search for Dark Matter in Events with One Jet and Missing Transverse Energy in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: CHATRCHYAN 2012T
publication_name: PRL 108 261803
doi: 10.1103/PhysRevLett.108.261803
inspire_id: 1103032
title:
Search for Dark Matter and Large Extra Dimensions in pp Collisions Yielding a Photon and Missing Transverse Energy


document_id: KHACHATRYAN 2015AG
publication_name: JHEP 1506 121
doi: 10.1007/JHEP06(2015)121
inspire_id: 1359293
title:
Search for the Production of Dark Matter in Association with Top-Quark Pairs in the Single-Lepton Final State in Proton-Proton Collisions at sqrt(s) = 8 TeV


document_id: AAD 2015AS
publication_name: EPJ C75 92
doi: 10.1140/epjc/s10052-015-3306-z
inspire_id: 1322381
title:
Search for Dark Matter in Events with Heavy Quarks and Missing Transverse Momentum in pp Collisions with the ATLAS Detector


document_id: AAD 2015CF
publication_name: PRL 115 131801
doi: 10.1103/PhysRevLett.115.131801
inspire_id: 1374488
title:
Search for Dark Matter in Events with Missing Transverse Momentum and a Higgs Boson Decaying to Two Photons in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2016M
publication_name: PR D93 072007
doi: 10.1103/PhysRevD.93.072007
inspire_id: 1399193
title:
Search for Dark Matter Produced in Association with a Higgs Boson Decaying to Two Bottom Quarks in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: AAD 2014BK
publication_name: PRL 112 041802
doi: 10.1103/PhysRevLett.112.041802
inspire_id: 1254228
title:
Search for Dark Matter in Events with a Hadronically Decaying W or Z Boson and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV with the ATLAS Detector


document_id: KHACHATRYAN 2016BZ
publication_name: JHEP 1612 083
doi: 10.1007/JHEP12(2016)083
inspire_id: 1477207
title:
Search for Dark Matter in Proton-Proton Collisions at 8 TeV with Missing Transverse Momentum and Vector Boson Tagged Jets


document_id: KHACHATRYAN 2016CA
publication_name: JHEP 1612 088
doi: 10.1007/JHEP12(2016)088
inspire_id: 1436367
title:
Search for Dark Matter Particles in Proton-Proton Collisions at sqrt(s) = 8 TeV using the Razor Variables


document_id: AABOUD 2016AD
publication_name: PL B763 251
doi: 10.1016/j.physletb.2016.10.042
inspire_id: 1479947
title:
Search for Dark Matter Produced in Association with a Hadronically Decaying Vector Boson in pp Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: AABOUD 2017A
publication_name: PL B765 11
doi: 10.1016/j.physletb.2016.11.035
inspire_id: 1486673
title:
Search for Dark Matter in Association with a Higgs Boson Decaying to b-Quarks in pp Collisions at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: SIRUNYAN 2017
publication_name: JHEP 1703 061
doi: 10.1007/JHEP03(2017)061
inspire_id: 1508174
title:
Search for Dark Matter and Unparticles in Events with a Z Boson and Missing Transverse Momentum in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: SIRUNYAN 2017G
publication_name: JHEP 1707 014
doi: 10.1007/JHEP07(2017)014
inspire_id: 1516193
title:
Search for Dark Matter Produced with an Energetic Jet or a Hadronically Decaying W or Z Boson at sqrt(s) = 13 TeV


document_id: AABOUD 2017R
publication_name: EPJ C77 393
doi: 10.1140/epjc/s10052-017-4965-8
inspire_id: 1591328
title:
Search for Dark Matter at sqrt(s) = 13 TeV in Final States Containing an Energetic Photon and Large Missing Transverse Momentum with the ATLAS Detector


document_id: KHACHATRYAN 2017AV
publication_name: JHEP 1708 035 (errat.)
doi: 10.1007/JHEP08(2017)035
inspire_id: 1477207
title:
Erratum to KHACHATRYAN 2016BZ: Search for Dark Matter in Proton-Proton Collisions at 8 TeV with Missing Transverse Momentum and Vector Boson Tagged Jets


document_id: AABOUD 2017AM
publication_name: PRL 119 181804
doi: 10.1103/PhysRevLett.119.181804
inspire_id: 1608773
title:
Search for Dark Matter Produced in Association with a Higgs Boson Decaying to bbbar using 36 fb^{-1} of pp Collisions at sqrt(s)=13 TeV with the ATLAS Detector


document_id: AABOUD 2017AQ
publication_name: PR D96 112004
doi: 10.1103/PhysRevD.96.112004
inspire_id: 1604888
title:
Search for Dark Matter in Association with a Higgs Boson Decaying to Two Photons at sqrt(s) = 13 TeV with the ATLAS Detector


document_id: SIRUNYAN 2017BB
publication_name: EPJ C77 845
doi: 10.1140/epjc/s10052-017-5317-4
inspire_id: 1603635
title:
Search for Dark Matter Produced in Association with Heavy-Flavor Quark Pairs in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: AABOUD 2018A
publication_name: EPJ C78 18
doi: 10.1140/epjc/s10052-017-5486-1
inspire_id: 1633591
title:
Search for Dark Matter Produced in Association with Bottom or Top Quarks in sqrt(s) = 13 TeV pp Collisions with the ATLAS Detector


document_id: SIRUNYAN 2018BF
publication_name: JHEP 1806 027
doi: 10.1007/JHEP06(2018)027
inspire_id: 1650462
title:
Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at $ \sqrt{s}=13 $ TeV


document_id: KHACHATRYAN 2018
publication_name: PR D97 099903
doi: 10.1103/PhysRevD.97.099903
inspire_id: 1407148
title:
Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at $\sqrt s=$ 8  TeV


document_id: SIRUNYAN 2018CU
publication_name: JHEP 1801 056
doi: 10.1007/JHEP01(2018)056
inspire_id: 1508174
title:
Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV


document_id: SIRUNYAN 2018DH
publication_name: JHEP 1809 046
doi: 10.1007/JHEP09(2018)046
inspire_id: 1677677
title:
Search for dark matter produced in association with a Higgs boson decaying to $\gamma\gamma$ or $\tau^+\tau^-$ at $\sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2019C
publication_name: PRL 122 011803
doi: 10.1103/PhysRevLett.122.011803
inspire_id: 1682779
title:
Search for dark matter particles produced in association with a top quark pair at $\sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2019O
publication_name: JHEP 1902 074
doi: 10.1007/JHEP02(2019)074
inspire_id: 1696608
title:
Search for new physics in final states with a single photon and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: SIRUNYAN 2019X
publication_name: JHEP 1903 141
doi: 10.1007/JHEP03(2019)141
inspire_id: 1712378
title:
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at $ \sqrt{s}=13 $ TeV


document_id: AABOUD 2019Q
publication_name: JHEP 1905 041
doi: 10.1007/JHEP05(2019)041
inspire_id: 1711243
title:
Search for large missing transverse momentum in association with one top-quark in proton-proton collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector


document_id: AABOUD 2019AA
publication_name: EPJ C79 120
doi: 10.1140/epjc/s10052-019-6540-y
inspire_id: 1683114
title:
A strategy for a general search for new phenomena using data-derived signal regions and its application within the ATLAS experiment


document_id: SIRUNYAN 2020X
publication_name: JHEP 2003 025
doi: 10.1007/JHEP03(2020)025
inspire_id: 1747894
title:
Search for dark matter particles produced in association with a Higgs boson in proton-proton collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV


document_id: TUMASYAN 2022AG
publication_name: EPJ C82 213
doi: 10.1140/epjc/s10052-022-10095-5
inspire_id: 1864485
title:
Search for strongly interacting massive particles generating trackless jets in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $


document_id: AKIMOV 2023
publication_name: PRL 130 051803
doi: 10.1103/PhysRevLett.130.051803
inspire_id: 1950121
title:
First Probe of Sub-GeV Dark Matter beyond the Cosmological Expectation with the COHERENT CsI Detector at the SNS


document_id: LIN 2023C
publication_name: PRL 130 111801
doi: 10.1103/PhysRevLett.130.111801
inspire_id: 2155167
title:
Search for the Pair Production of Dark Particles <math display=\"inline\"><mi>X</mi></math> with <math display=\"inline\"><msubsup><mi>K</mi><mi>L</mi><mn>0</mn></msubsup><mo stretchy=\"false\">→</mo><mi>X</mi><mi>X</mi></math>, <math display=\"inline\"><mi>X</mi><mo stretchy=\"false\">→</mo><mi>γ</mi><mi>γ</mi></math>


document_id: HAYRAPETYAN 2024B
publication_name: PRL 132 041802
doi: 10.1103/PhysRevLett.132.041802
inspire_id: 2661228
title:
Search for inelastic dark matter in events with two displaced muons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV


document_id: AAD 2024BA
publication_name: JHEP 2408 223
doi: 10.1007/JHEP08(2024)223
inspire_id: 2765017
title:
Differential cross-sections for events with missing transverse momentum and jets measured with the ATLAS detector in 13 TeV proton-proton collisions


document_id: AALTONEN 2009AF
publication_name: PR D80 011102
doi: 10.1103/PhysRevD.80.011102
inspire_id: 822073
title:
Searching the Inclusive leptongamma notET + b-Quark Signature for Radiative Top Quark Decay and non-Standard-Model Processes


document_id: AALTONEN 2014J
publication_name: PR D89 092001
doi: 10.1103/PhysRevD.89.092001
inspire_id: 1282906
title:
Invariant-Mass Distribution of Jet Pairs Produced in Association with a W Boson in ppbar Collisions at sqrt(s) = 1.96 TeV using the Full CDF Run II Data Set


document_id: AALTONEN 2011M
publication_name: PRL 106 171801
doi: 10.1103/PhysRevLett.106.171801
inspire_id: 894999
title:
Invariant Mass Distribution of Jet Pairs Produced in Association with a W Boson in ppbar Collisions at sqrt(s) = 1.96 TeV


document_id: AAD 2011AG
publication_name: NJP 13 053044
doi: 10.1088/1367-2630/13/5/053044
inspire_id: 893264
title:
A Search for New Physics in Dijet Mass and Angular Distributions in pp Collisions at sqrt(s) = 7 TeV Measured with the ATLAS Detector


document_id: AKESSON 1991
publication_name: ZPHY C52 219
doi: 10.1007/BF01560439
inspire_id: 302922
title:
A Search for Weakly Interacting Neutral Particles in Missing Energy Events on 450 GeV/c p N Collisions


document_id: GALLAS 1995
publication_name: PR D52 6
doi: 10.1103/PhysRevD.52.6
inspire_id: 385205
title:
Search for Neutral Weakly Interacting Massive Particles in the Fermilab Tevatron Wide Band Neutrino Beam


document_id: KRASZNAHORKAY 2016
publication_name: PRL 116 042501
doi: 10.1103/PhysRevLett.116.042501
inspire_id: 1358248
title:
Observation of Anomalous Internal Pair Creation in Be8 : A Possible Indication of a Light, Neutral Boson


document_id: AABOUD 2019H
publication_name: PR D99 012008
doi: 10.1103/PhysRevD.99.012008
inspire_id: 1692387
title:
A search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector


document_id: SIRUNYAN 2020AY
publication_name: PL B808 135578
doi: 10.1016/j.physletb.2020.135578
inspire_id: 1780982
title:
Measurement of the $\Upsilon$(1S) pair production cross section and search for resonances decaying to $\Upsilon$(1S)$\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 13 TeV


document_id: AAD 2023P
publication_name: JHEP 2307 176
doi: 10.1007/JHEP07(2023)176
inspire_id: 2626407
title:
Model-independent search for the presence of new physics in events including $H\rightarrow\gamma\gamma$ with $\sqrt{s}$ = 13 TeV pp data recorded by the ATLAS detector at the LHC


document_id: TUMASYAN 2023BF
publication_name: EPJ C83 827
doi: 10.1140/epjc/s10052-023-11687-5
inspire_id: 2639338
title:
A search for new physics in central exclusive production using the missing mass technique with the CMS detector and the CMS-TOTEM precision proton spectrometer


document_id: AAD 2024E
publication_name: PRL 132 081801
doi: 10.1103/PhysRevLett.132.081801
inspire_id: 2674351
title:
Search for new phenomena in two-body invariant mass distributions using unsupervised machine learning for anomaly detection at $\sqrt{s} = 13$ TeV with the ATLAS detector


document_id: ANDREEV 2022A
publication_name: PRL 129 161801
doi: 10.1103/PhysRevLett.129.161801
inspire_id: 2119984
title:
Search for a New <math display=\"inline\"><mi>B</mi><mo>-</mo><mi>L</mi></math> <math display=\"inline\"><msup><mi>Z</mi><mo>′</mo></msup></math> Gauge Boson with the NA64 Experiment at CERN


document_id: AAD 2015BJ
publication_name: EPJ C75 362
doi: 10.1140/epjc/s10052-015-3534-2
inspire_id: 1360282
title:
Search for Heavy Long-Lived Multi-Charged Particles in pp Collisions at sqrt(s) = 8 TeV using the ATLAS Detector


document_id: AAD 2023BT
publication_name: PL B847 138316
doi: 10.1016/j.physletb.2023.138316
inspire_id: 2648109
title:
Search for heavy long-lived multi-charged particles in the full LHC Run 2 $pp$ collision data at $\sqrt{s}$ = 13 TeV using the ATLAS detector


document_id: AKTAS 2004C
publication_name: EPJ C36 413
doi: 10.1140/epjc/s2004-01978-x
inspire_id: 647349
title:
Measurement of Anti-Deuteron Photoproduction and a Search for Heavy Stable Charged Particles at HERA


document_id: AAD 2013AH
publication_name: PL B722 305
doi: 10.1016/j.physletb.2013.04.036
inspire_id: 1215605
title:
Search for Long-Lived, Multi-Charged Particles in pp Collisions at sqrt(s) = 7 TeV using the ATLAS Detector


document_id: SIRUNYAN 2017B
publication_name: JHEP 1704 136
doi: 10.1007/JHEP04(2017)136
inspire_id: 1504209
title:
Search for Electroweak Production of a Vector-Like Quark Decaying to a top Quark and a Higgs Boson using Boosted Topologies in Fully Hadronic Final States


document_id: SIRUNYAN 2017C
publication_name: JHEP 1705 029
doi: 10.1007/JHEP05(2017)029
inspire_id: 1510567
title:
Search for Single Production of Vector-Like Quarks Decaying to a Z Boson and a Top or a Bottom Quark in Proton-Proton Collisions at sqrt(s) = 13 TeV


document_id: SIRUNYAN 2021T
publication_name: EPJ C81 629
doi: 10.1140/epjc/s10052-021-09236-z
inspire_id: 1821763
title:
MUSiC: a model-unspecific search for new physics in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $


document_id: HAYRAPETYAN 2023F
publication_name: JHEP 2312 068
doi: 10.1007/JHEP12(2023)068
inspire_id: 2683863
title:
Search for physics beyond the standard model in top quark production with additional leptons in the context of effective field theory


document_id: ALEKSEEV 1976B
publication_name: SJNP 23 633
inspire_id: 1247504
title:
Search for Metastable States with Lifetime Greater than 5 msec in a Lead Target Bombarded by 60 - 70 GeV Protons


document_id: SIRUNYAN 2018AW
publication_name: JHEP 1805 127
doi: 10.1007/JHEP05(2018)127
inspire_id: 1645630
title:
Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at $\sqrt{s}=$ 13 TeV


document_id: AABOUD 2019AE
publication_name: EPJ C79 481
doi: 10.1140/epjc/s10052-019-6962-6
inspire_id: 1719200
title:
Search for long-lived neutral particles in $pp$ collisions at $\sqrt{s}$ = 13 TeV that decay into displaced hadronic jets in the ATLAS calorimeter


document_id: AABOUD 2019AK
publication_name: PRL 122 151801
doi: 10.1103/PhysRevLett.122.151801
inspire_id: 1702261
title:
Search for the Production of a Long-Lived Neutral Particle Decaying within the ATLAS Hadronic Calorimeter in Association with a $Z$ Boson from $pp$ Collisions at $\sqrt{s} =$ 13  TeV


document_id: AABOUD 2019AM
publication_name: PR D99 052003
doi: 10.1103/PhysRevD.99.052003
inspire_id: 1707957
title:
Search for heavy long-lived multicharged particles in proton-proton collisions at $\sqrt{s}$ = 13  TeV using the ATLAS detector


document_id: AABOUD 2019AO
publication_name: PR D99 052005
doi: 10.1103/PhysRevD.99.052005
inspire_id: 1704138
title:
Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$  TeV that decay into displaced hadronic jets in the ATLAS muon spectrometer


document_id: AAD 2020J
publication_name: PR D101 052013
doi: 10.1103/PhysRevD.101.052013
inspire_id: 1767646
title:
Search for long-lived neutral particles produced in $pp$ collisions at $\sqrt{s} = 13$ TeV decaying into displaced hadronic jets in the ATLAS inner detector and muon spectrometer


document_id: AAD 2020P
publication_name: EPJ C80 450
doi: 10.1140/epjc/s10052-020-7997-4
inspire_id: 1752519
title:
Search for light long-lived neutral particles produced in $pp$ collisions at $\sqrt{s} =$ 13 TeV and decaying into collimated leptons or light hadrons with the ATLAS detector


document_id: TUMASYAN 2021
publication_name: PRL 127 261804
doi: 10.1103/PhysRevLett.127.261804
inspire_id: 1883075
title:
Search for Long-Lived Particles Decaying in the CMS End Cap Muon Detectors in Proton-Proton Collisions at $\sqrt s$ =13  TeV


document_id: AAD 2021BA
publication_name: JHEP 2111 229
doi: 10.1007/JHEP11(2021)229
inspire_id: 1882568
title:
Search for exotic decays of the Higgs boson into long-lived particles in $pp$ collisions at $ \sqrt{s} $ = 13 TeV using displaced vertices in the ATLAS inner detector


document_id: AAD 2022H
publication_name: PR D106 032005
doi: 10.1103/PhysRevD.106.032005
inspire_id: 2040545
title:
Search for events with a pair of displaced vertices from long-lived neutral particles decaying into hadronic jets in the ATLAS muon spectrometer in pp collisions at $\sqrt s$=13  TeV


document_id: TUMASYAN 2022M
publication_name: JHEP 2203 160
doi: 10.1007/JHEP03(2022)160
inspire_id: 1954276
title:
Search for long-lived particles produced in association with a Z boson in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: AAD 2022K
publication_name: JHEP 2206 005
doi: 10.1007/JHEP06(2022)005
inspire_id: 2043503
title:
Search for neutral long-lived particles in $pp$ collisions at $ \sqrt{s} $ = 13 TeV that decay into displaced hadronic jets in the ATLAS calorimeter


document_id: TUMASYAN 2023G
publication_name: JHEP 2305 228
doi: 10.1007/JHEP05(2023)228
inspire_id: 2083735
title:
Search for long-lived particles decaying to a pair of muons in proton-proton collisions at $ \sqrt{s} $ = 13 TeV


document_id: AAD 2023AR
publication_name: PR D108 032016
doi: 10.1103/PhysRevD.108.032016
inspire_id: 2146266
title:
Search for displaced photons produced in exotic decays of the Higgs boson using 13 TeV $pp$ collisions with the ATLAS detector


document_id: ALVIS 2018
publication_name: PRL 120 211804
doi: 10.1103/PhysRevLett.120.211804
inspire_id: 1651234
title:
First Limit on the Direct Detection of Lightly Ionizing Particles for Electric Charge as Low as e/1000 with the Majorana Demonstrator


document_id: AAD 2012AK
publication_name: PL B716 122
doi: 10.1016/j.physletb.2012.08.009
inspire_id: 1111820
title:
Search for TeV-Scale Gravity Signatures in Final States with Leptons and Jets with the ATLAS Detector at sqrt(s) = 7 TeV.


document_id: AAD 2014C
publication_name: JHEP 1408 103
doi: 10.1007/JHEP08(2014)103
inspire_id: 1296834
title:
Search for Microscopic Black Holes and String Balls in Final States with Leptons and Jets with the ATLAS Detector at sqrt(s) = 8 TeV


document_id: AAD 2015AN
publication_name: JHEP 1507 032
doi: 10.1007/JHEP07(2015)032
inspire_id: 1357199
title:
Search for Low-Scale Gravity Signatures in Multi-Jet Final States with the ATLAS Detector at sqrt(s) = 8 TeV


# pdgfootnote

pdgid: S000M
text:
MALTA 2024 gives an upper limit on the photon mass by analysing the gravitational time delay  in a weak-field approximation using Doppler-tracking data from the Cassini mission.


pdgid: S000M
text:
YAN 2024A put constraints on the photon mass modelling non-zero-mass effects on the Jupiter  magnetic field and  using data of the JUNO Mission.


pdgid: S000M
text:
WANG 2023B use fast radio burst photon mass dependent dispersion relation to determine an  upper limit of the photon mass.


pdgid: S000M
text:
MALTA 2022 consider the effect of a finite photon mass on Schumann resonances in the  Earth-ionosphere cavity, improve limit by KROLL 1971A  by considering realistic conductivity  profiles for the atmosphere.


pdgid: S000M
text:
BONETTI 2017 uses frequency-dependent time delays of repeating FRB with well-determined  redshift, assuming the DM is caused by expected dispersion in IGM. There are several uncertainties,  leading to mass limit 2.2E-14 eV.


pdgid: S000M
text:
BONETTI 2016 uses frequency-dependent time delays of FRB, assuming the DM is caused by  expected dispersion in IGM. There are several uncertainties, leading to mass limit 1.8E-14 eV,  if indeed the FRB is at the initially reported redshift.


pdgid: S000M
text:
RETINO 2016 looks for deviations from Ampere's law in the solar wind, using Cluster four  spacecraft data. Authors quote a range of limits from 1.9E-15 eV to 7.9E-14 eV depending on  the assumptions of the vector potential from the interplanetary magnetic field.


pdgid: S000M
text:
EGOROV 2014 studies chromatic dispersion of lensed quasar positions (``gravitational rainbows'') that could be produced by any of  several mechanisms, among them via photon mass. Limit not competitive but obtained on cosmological distance scales.


pdgid: S000M
text:
ACCIOLY 2010 limits come from possible alterations of anomalous magnetic moment of electron and  gravitational deflection of electromagnetic radiation. Reported limits are not "claimed" by the authors and in any case are not competitive.


pdgid: S000M
text:
When trying to measure mass() one must distinguish between measurements performed on large and small  scales. If the photon acquires mass by the Higgs mechanism, the large-scale behavior of the photon  might be effectively Maxwellian. If, on the other hand, one postulates the Proca regime for all scales,  the very existence of the galactic field implies mass() < E-26 eV, as correctly calculated  by YAMAGUCHI 1959 and CHIBISOV 1976.


pdgid: S000M
text:
TU 2006 continues the work of LUO 2003, with extended LAKES 1998 method, reporting the improved  limit mu^2()A = 0.7+-1.7E-13 T/m if A = 0.2 muG out to 4E22 m. Reported  result mu = 0.9+-1.5E-52 g reduces to the frequentist mass limit 1.2E-19 eV  (FELDMAN 1998). While the results of the torsion balance method give a value for the local  limit on mu^2()A, the deduced limit on the photon mass mu is open to question. See the  discussions in TU 2005 and GOLDHABER 2003.


pdgid: S000M
text:
FULLEKRUG 2004 adopted KROLL 1971A method with newer and better Schumann resonance data. Result questionable because assumed frequency shift with photon mass is assumed to be linear. It is quadratic according to theorem by GOLDHABER 1971B, KROLL 1971, and PARK 1971.


pdgid: S000M
text:
LUO 2003 extends LAKES 1998 technique to set a limit on mu^2()A, where mu**-1 is the Compton wavelength lambdabar(C) of the massive photon and  A is the ambient vector potential. The important departure is that the apparatus rotates, removing sensitivity to the direction of A. They take  A = 10**12 Tm, due to ``cluster level fields.'' But see comment of GOLDHABER 2003 and reply by LUO 2003B.


pdgid: S000M
text:
LAKES 1998 reports limits on torque on a toroid Cavendish balance, obtaining a limit on mu**2A<2E-9Tm/m**2 via the Maxwell-Proca equations, where mu**-1 is the characteristic length associated with the photon mass and A is the ambient vector potential in the Lorentz gauge. Assuming A ~~1E12Tm due to cluster fields he obtains mu**-1 >2E10m, corresponding to mu< 1E-17 eV. A more conservative limit, using A ~~(1 muG)x(600 pc) based on the galactic field, is mu**-1 > 1E9m or  mu < 2E-16 eV.


pdgid: S000M
text:
FISCHBACH 1994 analysis is based on terrestrial magnetic fields; approach analogous to DAVIS 1975. Similar result based on  a much smaller planet probably follows from more precise B field mapping. ``Secure limit, best by this method'' (per GOLDHABER 2010).


pdgid: S000M
text:
CHERNIKOV 1992, motivated by possibility that photon exhibits mass only below some unknown critical temperature, searches for departure from Ampere's Law at 1.24 K. See also RYAN 1985.


pdgid: S000M
text:
RYAN 1985, motivated by possibility that photon exhibits mass only below some unknown critical temperature, sets mass limit at < 1.5+-1.4E-42 g based on Coulomb's Law departure limit at 1.36 K. We report the result as frequentist 90% CL (FELDMAN 1998).


pdgid: S000M
text:
CHIBISOV 1976 depends in critical way on assumptions such as applicability of virial theorem.  Some of the arguments given only in unpublished references.


pdgid: S000M
text:
DAVIS 1975 analysis of Pioneer-10 data on Jupiter's magnetic field. ``Secure limit, best by this method'' (per GOLDHABER 2010).


pdgid: S000M
text:
FRANKEN 1971 method is of dubious validity (KROLL 1971A, JACKSON 1999, GOLDHABER 2010, and references therein).


pdgid: S000M
text:
KROLL 1971A used low frequency Schumann resonances in cavity between the conducting earth and resistive ionosphere,  overcoming objections to resonant-cavity methods (JACKSON 1999, GOLDHABER 2010, and references therein). ``Secure limit, best by this method'' (per GOLDHABER 2010).


pdgid: S000M
text:
WILLIAMS 1971 is landmark test of Coulomb's law. ``Secure limit, best by this method'' (per GOLDHABER 2010).


pdgid: S000Q
text:
ALTSCHUL 2007B looks for Aharonov-Bohm phase shift in addition to geometric phase shift in radio interference fringes (VSOP mission).


pdgid: S000Q
text:
CAPRINI 2005 uses isotropy of the cosmic microwave background to place stringent limits  on possible charge asymmetry of the Universe. Charge limits are set on the photon, neutrino,  and dark matter particles. Valid if charge asymmetries produced by different particles are not anticorrelated.


pdgid: S000Q
text:
KOBYCHEV 2005 considers a variety of observable effects of photon charge for extragalactic  compact radio sources.  Best limits if source observed through a foreground cluster of galaxies.


pdgid: S000Q
text:
SEMERTZIDIS 2003 reports the first laboratory limit on the photon charge in the last 30 years.  Straightforward improvements in the apparatus could attain a sensitivity of 10**-20e.


pdgid: S000Q
text:
SIVARAM 1995 requires that CMB photon charge density not overwhelm gravity. Result scales as Omega(M)h**2.


pdgid: S000Q
text:
RAFFELT 1994 notes that COCCONI 1988 neglects the fact that the time delay due to dispersion by free electrons in the interstellar medium has the same photon energy dependence as that due to bending of a charged photon in the magnetic field.  His limit is based on the assumption that the entire observed dispersion is due to photon charge.  It is a factor of 200 less stringent than the COCCONI 1988 limit.


pdgid: G033M
text:
ABBOTT 2021 assumed modified gravitational-wave dispersion to establish a limit on graviton  mass, using LIGO-Virgo O1-O3a binary black hole (BBH) events.


pdgid: G033M
text:
DEFELICE 2024 limits graviton mass in context of the "extended Minimal Theory of Massive  Gravity" recently proposed by two of the authors, using constraints from Planck-CMB, BAO and SNe1a.


pdgid: G033M
text:
WANG 2024 investigates sensitivity to the graviton mass of overlap reduction functions due to  stochastic gravitational wave background in the nano-Hertz band as observed in pulsar timing arrays.


pdgid: G033M
text:
DEFELICE 2021 studies the normal branch of the Minimal Theory of Massive Gravity (MTMG) to  find that  after five parameters are adjusted to obtain agreement with all presently available  data,  today's  squared mass m_{{g}}^2 = 2.5+4.5-4.8E-67 eV**2  or m_{{g}} < 8.4E-33 eV,  both at  the 95% CL.


pdgid: G033M
text:
BERNUS 2020 use the latest solution of the ephemeris INPOP (19a) in order to improve the  constraint in BERNUS 2019  on the existence of a Yukawa suppression to the Newtonian  potential, generically associated to a gravitons mass.


pdgid: G033M
text:
SHAO 2020 sets limit, 95% CL, based on non-observation of excess gravitational  radiation in 14 well-timed binary pulsars in the context of the cubic Galileon model.


pdgid: G033M
text:
ABBOTT 2019, ABBOTT 2017, and ABBOTT 2016 assumed modified gravitational waves  dispersion to establish limits on graviton  mass.


pdgid: G033M
text:
BERNUS 2019 use the planetary ephemeris INPOP 17b to constraint the existence of a Yukawa  suppression to the Newtonian potential, generically associated to a gravitons mass.


pdgid: G033M
text:
MIAO 2019 90% CL limit is based on orbital period decay rates of 9 binary pulsars using  a Bayesian prior uniform in graviton mass. Limit becomes < 5.2E-21 eV for a prior  uniform in ln(mass(g)).


pdgid: G033M
text:
RANA 2018 limit, 68% CL, obtained using weak lensing mass profiles out   to the radius  at which the cluster density falls to 200 times  the critical density of the Universe. Limit is  based on the fractional change between Newtonian and Yukawa accelerations for the 50 most massive  galaxy clusters in the Local Cluster Substructure Survey. Limits for other CL's and other density  cuts are also given.


pdgid: G033M
text:
RANA 2018 limit, 68% CL, obtained using mass measurements via the SZ effect out to the  radius at which the cluster density falls to 500 times the critical density of the Universe for 182  optically confirmed galaxy clusters in an Altacama Cosmology Telescope survey. Limits for other  CL's and other density cuts are also given.


pdgid: G033M
text:
WILL 2018 limit from perihelion advances of the planets, notably Earth, Mars, and Saturn.   Alternate analysis yields < 6E-24.


pdgid: G033M
text:
ZAKHAROV 2016 constrains range of Yukawa gravity interaction from S2 star orbit about black  hole at Galactic center. The limit is < 2.9E-21 eV for delta = 100.


pdgid: G033M
text:
GRUZINOV 2005 uses the DGP model (DVALI 2000) showing that non-perturbative effects  restore continuity with Einstein's equations as the gravition mass approaches zero, then bases his  limit on Solar System observations.


pdgid: G033M
text:
CHOUDHURY 2004 concludes from a study of weak-lensing data that masses heavier than about the inverse of 100 Mpc seem to be ruled out if the gravitation field has the Yukawa form.


pdgid: G033M
text:
GERSHTEIN 2004 use non-Einstein field relativistic theory of gravity (RTG), with a massive  graviton, to obtain the 95% CL mass limit implied by the value of  Omega(tot) = 1.02+-0.02 current at the time of publication.


pdgid: G033M
text:
As of 2020, limits on dP/dt are now about 0.1% (see T. Damour, ``Experimental tests of  gravitational theory,'' in this Review).


pdgid: G033M
text:
FINN 2002 analyze the orbital decay rates of PSRB1913+16 and PSRB1534+12 with a possible graviton mass as a parameter.  The combined frequentist mass limit is at 90%CL.


pdgid: G033M
text:
GOLDHABER 1974 establish this limit considering the binding of galactic clusters, corrected  to Planck h_{{0}}() = 0.67.


pdgid: S043M
text:
AAIJ 2022C analyse W production in the muon decay channel, with the transverse momentum   of the muon required to be between 28 and 52 GeV. Analysing the distribution of the muon charge   divided by the muon transverse momentum of approximately 2.4 million selected W candidates, a   value of M_{{W}} = 80354+-23(stat.)+-10(exp.)+-17(theo.)+-9(PDF) MeV is obtained;   we combine the three systematic uncertainties in quadrature.


pdgid: S043M
text:
AALTONEN 2022 select a data sample of about 4 million W boson candidates in 8.8  fb**-1 of Run-II data. The mass is determined using the transverse mass, transverse lepton  momentum and transverse missing momentum distributions of W decays into electrons or muons,  accounting for correlations. This measurement supersedes AALTONEN 2012E, but is not used in  OUR EVALUATION.


pdgid: S043M
text:
AABOUD 2018J select 4.61M W+ --> mu+ nu_mu, 3.40M W+ --> e+ nu_e,  3.23M W- --> mu- nubar_mu and  2.49M W- --> e- nubar_e events in 4.6 fb**-1 p p data at 7 TeV. The W mass is  determined using the transverse mass and transverse lepton momentum distributions, accounting for  correlations. The systematic error includes 0.011 GeV experimental and 0.014 GeV modelling  uncertainties.


pdgid: S043M
text:
ABDALLAH 2008A use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu and  W+ W- --> q qbar q qbar events for energies 172 GeV and above. The W mass was also extracted from  the dependence of the W W cross section close to the production threshold and combined appropriately  to obtain the final result. The systematic error includes +-0.025 GeV due to final state interactions  and +-0.009 GeV due to LEP energy uncertainty.


pdgid: S043M
text:
ABBIENDI 2006 use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu_lepton and W+ W- --> q qbar q qbar events. The result quoted here is obtained combining this mass value with the results using W+ W- --> lepton nu_lepton lepton^'nu(lepton^') events in the energy range 183 -- 207 GeV (ABBIENDI 2003C) and the dependence of the WW production cross-section on mass(W) at threshold.  The systematic error includes +-0.009 GeV due to the uncertainty on the LEP beam energy.


pdgid: S043M
text:
ACHARD 2006 use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu_lepton and W+ W- --> q qbar q qbar events in the C.M. energy range 189 -- 209 GeV. The result quoted here is obtained combining this mass value with the results obtained from a direct W mass reconstruction at 172 and 183 GeV and with those from the dependence of the W W production cross-section on mass(W) at 161 and 172 GeV (ACCIARRI 1999).


pdgid: S043M
text:
SCHAEL 2006 use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu_lepton and  W+ W- --> q qbar q qbar events in the C.M. energy range 183 -- 209 GeV. The result quoted here  is obtained combining this mass value with those obtained from the dependence of the W pair production  cross-section on mass(W) at 161 and 172 GeV (BARATE 1997 and BARATE 1997S respectively).  The systematic error includes +-0.009 GeV due to possible effects of final state interactions  in the q qbar q qbar channel and +-0.009 GeV due to the uncertainty on the LEP beam energy.


pdgid: S043M
text:
ABAZOV 2002D improve the measurement of the W-boson mass including W --> e nu_e events in which the electron is close to a boundary of a central electromagnetic calorimeter module.  Properly combining the results obtained by fitting m(T)(W), p(T)(e), and p(T)(nu), this sample provides a mass value of 80.574+-0.405 GeV. The value reported here is a combination of this measurement with all previous D0 W-boson mass measurements.


pdgid: S043M
text:
AAD 2024CJ provides an improved determination of the W boson mass using the same data as  analysed for AABOUD 2018J, thus superseding that W boson mass measurement. The  distributions of the transverse lepton momentum and of the transverse mass are analysed to  determine the W boson mass.


pdgid: S043M
text:
ANDREEV 2018A obtain this result in a combined electroweak and QCD analysis using all  deep-inelastic e+ p and e- p neutral current and charged current scattering cross sections  published by the H1 Collaboration, including data with longitudinally polarized lepton beams.


pdgid: S043M
text:
AALTONEN 2012E select 470k W -->e nu decays and 625k W --> mu nu decays in 2.2 fb**-1 of Run-II data.  The mass is determined using the transverse mass, transverse lepton momentum and transverse  missing energy distributions, accounting for correlations. This result supersedes AALTONEN 2007F.  AALTONEN 2014D gives more details on the procedures followed by the authors. This measurement  is superseded by AALTONEN 2022.


pdgid: S043M
text:
ABAZOV 2012F select 1677k W --> e nu decays in 4.3 fb**-1 of Run-II data. The mass is determined using   the transverse mass and transverse lepton momentum distributions, accounting for correlations.


pdgid: S043M
text:
ABAZOV 2009AB study the transverse mass, transverse electron momentum, and transverse missing energy in a sample of 0.5 million W --> e nu decays selected in Run-II data. The quoted result combines all three methods, accounting for correlations.


pdgid: S043M
text:
AALTONEN 2007F obtain high purity W --> e nu_e and W --> mu nu_mu candidate samples totaling 63,964 and 51,128 events respectively. The W mass value quoted above is derived by simultaneously fitting the transverse mass and the lepton, and neutrino p(T) distributions.


pdgid: S043M
text:
AKTAS 2006 fit the Q**2 dependence (300 < Q**2 < 30,000 GeV**2)  of the charged-current differential cross section with a propagator mass. The first error is experimental and the second corresponds to uncertainties due to input parameters and model assumptions.


pdgid: S043M
text:
CHEKANOV 2002C fit the Q**2 dependence (200<Q**2<60000 GeV**2) of the charged-current differential cross sections with a propagator mass fit. The last error is due to the uncertainty on the probability density functions.


pdgid: S043M
text:
AFFOLDER 2001E fit the transverse mass spectrum of 30115  W --> e nu_e events (M(W)= 80.473+-0.065+-0.092 GeV) and of 14740 W --> mu nu_mu events  (M(W)= 80.465+-0.100+-0.103 GeV) obtained in the run IB (1994-95). Combining  the electron and muon results, accounting for correlated uncertainties, yields  M(W)= 80.470+-0.089 GeV. They combine this value with their measurement of  ABE 1995P reported in run IA (1992-93) to obtain the quoted value.


pdgid: S043M
text:
BREITWEG 2000D fit the Q**2 dependence (200 < Q**2< 22500 GeV**2) (200<Q**2<22500 GeV**2) of the charged-current differential cross sections with a propagator mass fit. The last error is due to the uncertainty on the probability density functions.


pdgid: S043M
text:
ALITTI 1992B result has two contributions to the systematic error (+-0.83); one (+-0.81) cancels in mass(W)/mass(Z) and one (+-0.17) is noncancelling.  These were added in quadrature.  We choose the ALITTI 1992B value without using the LEP mass(Z) value, because we perform our own combined fit.


pdgid: S043M
text:
There are two contributions to the systematic error (+-0.84):  one (+-0.81) which cancels in mass(W)/mass(Z) and one (+-0.21) which is non-cancelling.  These were added in quadrature.


pdgid: S043MR
text:
This value was obtained using the world average values of mass(Z) and mass(W) as presented in these listings.


pdgid: S043MR
text:
ABBOTT 1998N obtain this from a study of 28323 W --> e nu_e and 3294 Z --> e+ e- decays.  Of this latter sample, 2179 events are used to calibrate the electron energy scale.


pdgid: S043MR
text:
ABBOTT 1998P obtain this from a study of 5982 W --> e nu_e events. The systematic error includes an uncertainty of +-0.00175 due to the electron energy scale.


pdgid: S043MD
text:
AABOUD 2018J select 4.61M W+ --> mu+ nu_mu, 3.40M W+ --> e+ nu_e, 3.23M W- --> mu- nubar_mu  and 2.49M W- --> e- nubar_e events in 4.6 fb**-1 p p data at 7 TeV. The W mass is  determined using the transverse mass and transverse lepton momentum distributions, accounting for  correlations. The systematic error includes 0.007 GeV experimental and 0.024 GeV modelling  uncertainties.


pdgid: S043W
text:
AAD 2024CJ provides an improved determination of the W boson mass using the same data as  analysed for AABOUD 2018J. In addition, the distributions of the transverse lepton momentum  and of the transverse mass are analysed to determine the W boson width.


pdgid: S043W
text:
SCHAEL 2013A result combines the measurements from the LEP experiments ALEPH (SCHAEL 2006),  DELPHI(ABDALLAH 2008A), L3 (ACHARD 2006) and OPAL(ABBIENDI 2006). The average of  these four results takes correlations into account and has a chi^2 probability of 27%.


pdgid: S043W
text:
TEVEWWG 2010 result combines the measurements from the Tevtatron experiments CDF (ABE 1995C,  AFFOLDER 2000M, AALTONEN 2008B) and D0 (ABAZOV 2002E, ABAZOV 2009AK). The  average of these five results takes correlations into account and has a chi^2 probability of  84%.


pdgid: S043W
text:
ABAZOV 2009AK obtain this result fitting the high-end tail (100-200 GeV) of the transverse mass spectrum in W --> e nu decays.


pdgid: S043W
text:
AALTONEN 2008B obtain this result fitting the high-end tail (90 -- 200 GeV) of the transverse mass spectrum in semileptonic W --> e nu_e and W --> mu nu_mu decays.


pdgid: S043W
text:
ABDALLAH 2008A use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu and W+ W- --> q qbar q qbar events. The systematic error includes +-0.065 GeV due to final state interactions.


pdgid: S043W
text:
ABBIENDI 2006 use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu_lepton and W+ W- --> q qbar q qbar events. The systematic error includes +-0.003 GeV due to the uncertainty on the LEP beam energy.


pdgid: S043W
text:
ACHARD 2006 use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu_lepton and W+ W- --> q qbar q qbar events in the C.M. energy range 189 -- 209 GeV. The result quoted here is obtained combining this value of the width with the result obtained from a direct W mass reconstruction at 172 and 183 GeV (ACCIARRI 1999).


pdgid: S043W
text:
SCHAEL 2006 use direct reconstruction of the kinematics of W+ W- --> q qbar lepton nu_lepton and W+ W- --> q qbar q qbar events. The systematic error includes +-0.05 GeV due to possible effects of final state interactions in the q qbar q qbar channel and +-0.01 GeV due to the uncertainty on the LEP beam energy.


pdgid: S043W
text:
ABAZOV 2002E obtain this result fitting the high-end tail (90 -- 200 GeV) of the transverse-mass spectrum in semileptonic W --> e nu_e decays.


pdgid: S043W
text:
ABBOTT 2000B measure R = 10.43+-0.27 for the W --> e nu_e decay channel.  They use the SM theoretical predictions for sigma(W)/sigma(Z) and Gamma(W --> e nu_e) and the world average for B(Z --> e e). The value quoted here is obtained combining this result (2.169+-0.070 GeV) with that of ABBOTT 1999H.


pdgid: S043W
text:
AFFOLDER 2000M fit the high transverse mass (100 -- 200GeV) W --> e nu_e and W --> mu nu_mu events to obtain Gamma(W)= 2.04+-0.11(stat)+-0.09(syst) GeV.  This is combined with the earlier CDF measurement (ABE 1995C) to obtain the quoted result.


pdgid: S043W
text:
ABE 1995W measured R = 10.90+-0.32+-0.29.  They use mass(W)=80.23+-0.18 GeV, CS(W)/CS(Z) = 3.35+-0.03, Gamma(W --> e nu) = 225.9+-0.9 MeV, Gamma(Z --> e+ e-) = 83.98+-0.18 MeV, and Gamma(Z) = 2.4969+-0.0038 GeV.


pdgid: S043W
text:
ALITTI 1992 measured R = 10.4+0.7-0.6+-0.3.  The values of CS(Z) and CS(W) come from O(alpha(s)**2) calculations using mass(W) = 80.14+-0.27 GeV, and mass(Z) = 91.175+-0.021 GeV along with the corresponding value of sin**2(theta(W)) = 0.2274.  They use CS(W)/CS(Z) = 3.26+-0.07+-0.05 and Gamma(Z) = 2.487+-0.010 GeV.


pdgid: S043W
text:
ALBAJAR 1991 measured R = 9.5+1.1-1.0 (stat. + syst.). CS(W)/CS(Z) is calculated in QCD at the parton level using mass(W) = 80.18+-0.28 GeV and mass(Z) = 91.172+-0.031 GeV along with sin**2(theta(W)) = 0.2322+-0.0014. They use CS(W)/CS(Z) = 3.23+-0.05 and Gamma(Z) = 2.498+-0.020 GeV. This measurement is obtained combining both the electron and muon channels.


pdgid: S043WIN
text:
BARATE 1999I measure this quantity using the dependence of the total cross section sigma(W W) upon a change in the total width.  The fit is performed to the W W measured cross sections at 161, 172, and 183 GeV.  This partial width is <139 MeV at 95%CL.


pdgid: S043WIN
text:
BARATE 1999L use W-pair production to search for effectively invisible W decays, tagging with the decay of the other Wboson to Standard Model particles.  The partial width for effectively invisible decay is <27MeV at 95%CL.


pdgid: S043R10
text:
ABBOTT 1999H measure R == [sigma(W) B(W --> lepton nu_lepton)]/[sigma(Z) B(Z --> lepton lepton)] = 10.90+-0.52 combining electron and muon channels. They use M(W) = 80.39+-0.06 GeV and the SM theoretical predictions for sigma(W)/sigma(Z) and B(Z --> lepton lepton).


pdgid: S043R10
text:
1216+-38+27-31 W --> mu nu events from ABE 1992I and 2426W --> e nu events of ABE 1991C. ABE 1992I give the inverse quantity as 9.6+-0.7 and we have inverted.


pdgid: S043R1
text:
ABAZOV 2004D take into account all correlations to properly combine the CDF  (ABE 1995W) and D0 (ABBOTT 2000B) measurements of the ratio R in the electron channel. The ratio R is defined as [sigma_{{W}}.B(W --> e nu_e)] / [sigma_{{Z}}.B(Z --> e e)]. The combination gives R**Tevatron = 10.59+-0.23.  / sigma_{{Z}} is calculated at next-to-next-to-leading order  (3.360+-0.051). The branching fraction  B(Z --> e e) is taken from this Review as (3.363+-0.004)%.


pdgid: S043R3
text:
AAD 2024CG analyse t tbar production rates in the e e, e mu and mu mu  dilepton final states. Using the ratio of B(Z --> mu mu)/B(Z --> e e) measured  precisely at e+ e- colliders, the ratio B(W --> mu nu)/B(W --> e nu) is determined.


pdgid: S043R3
text:
AABOUD 2017Q make a precise determination of W --> e nu and W --> mu nu production in  the follwoing fiducial phase space: lepton pseudo-rapidity range |eta| < 2.5, lepton  and neutrino transverse momenta larger than 25 GeV each, and W transverse mass larger than 25  GeV. They determine the ratio of the W branching fractions B(W --> e nu)/B(W --> mu nu) =  0.9967+-0.0004+-0.0101 = 0.997+-0.010.


pdgid: S043R3
text:
AAIJ 2016AJ make precise measurements of forward W --> e nu and W --> mu nu  production in proton-proton collisions at 8 TeV and determine the ratio of the W branching  fractions B(W --> e nu)/B(W --> mu nu) = 1.020+-0.002+-0.019.


pdgid: S043R3
text:
ABACHI 1995D obtain this result from the measured sigma(W)B(W --> mu nu)= 2.09+-0.23+-0.11nb and sigma(W)B(W --> e nu)= 2.36+-0.07+-0.13nb in which the first error is the combined statistical and systematic uncertainty, the second reflects the uncertainty in the luminosity.


pdgid: S043R3
text:
ABE 1992I obtain sigma(W)B(W --> mu nu)= 2.21+-0.07+-0.21 and combine with ABE 1991C sigma(W) B((W --> e nu)) to give a ratio of the couplings from which we derive this measurement.


pdgid: S043R7
text:
ABBOTT 2000D measure sigma(W)*B(W --> tau nu_tau) = 2.22+-0.09+-0.10+-0.10nb.  Using the ABBOTT 2000B result sigma(W)*B(W --> e nu_e) = 2.31+-0.01+-0.05+-0.10nb, they quote the ratio of the couplings from which we derive this measurement.


pdgid: S043R7
text:
ABE 1992E use two procedures for selecting W --> tau nu_tau events. The missing E(T) trigger leads to 132+-14+-8 events and the tau trigger to 47+-9+-4 events. Proper statistical and systematic correlations are taken into account to arrive at sigmaB(W --> tau nu) = 2.05+-0.27 nb. Combined with ABE 1991C result on sigmaB(W --> e nu), ABE 1992E quote a ratio of the couplings from which we derive this measurement.


pdgid: S043R16
text:
AAD 2021AN study t tbar production, with the W bosons in top-quark decay decaying to  electrons or taus, with the tau decaying further into a muon. Analyzing the muon impact parameter  and its transverse momentum, the contributions from prompt muons (arising from W decay) and  non-prompt muons (arising from tau decay) are separated, allowing a measurement of the ratio of the  W branching fractions into taus and muons, R(tau/mu) = 0.992+-0.007+-0.011 where  the first error is statistical and the second systematic.


pdgid: S043R01
text:
AAD 2024BO search for exclusive hadronic decays of the W boson into a charged meson plus  a photon, where the meson is a pi+-, K+- or rho+-. The meson-photon invariant mass  distribution is used to set the limit on the branching fraction.


pdgid: S043R01
text:
SIRUNYAN 2021I search for the rare decay of a W boson into a charged pion accompanied by  a photon. A signal is not observed, and an upper limit on the branching fraction B(W --> pi gamma)  < 1.50E-5 is obtained at 95% C.L.


pdgid: S043R04
text:
AAD 2024BO search for exclusive hadronic decays of the W boson into a charged meson plus a  photon, where the meson is a pi+-, K+- or rho+-. The meson-photon invariant mass  distribution is used to set the limit on the branching fraction.


pdgid: S043R02
text:
AAIJ 2023AM also quotes the branching fraction limit B(W+ --> D_s()+ gamma) <  6.5E-4, using the known W --> mu nu branching fraction.


pdgid: S043R15
text:
ABBIENDI 2000V tag W --> c X decays using measured jet properties, lifetime information, and leptons produced in charm decays. From this result, and using the additional measurements of Gamma(W) and B(W --> hadrons), |V(c s)| is determined to be 0.969+-0.045+-0.036.


pdgid: S043R15
text:
BARATE 1999M tag cjets using a neural network algorithm. From this measurement |V(c s)| is determined to be 1.00+-0.11+-0.07.


pdgid: S043R14
text:
ABREU 1998N tag c and sjets by identifying a charged kaon as the highest momentum particle in a hadronic jet.  They also use a lifetime tag to independently identify a cjet, based on the impact parameter distribution of charged particles in a jet. From this measurement |V(c s)| is determined to be 0.94+0.32-0.26+-0.13.


pdgid: S043R00
text:
SIRUNYAN 2019BG search for the rare decay of a W boson into three charged pions. Three pion  candidates are required in each event, with transverse momentum larger than 35 GeV, 35 GeV, 18 GeV,  respectively, while the transverse momentum of the three-pion system is required to be larger than  40 GeV.  Analyzing the three-pion invariant mass, no excess is observed in the W mass region,  leading to the 95% C.L. upper limit on the branching fraction.


pdgid: S043PIC
text:
ABREU,P 2000F measure <N(pi+-)> = 31.65+-0.48+-0.76 and 15.51+-0.38+-0.40 in the fully hadronic and semileptonic final states respectively. The value quoted is a weighted average without assuming any correlations.


pdgid: S043KC
text:
ABREU,P 2000F measure <N(K+-)> = 4.38+-0.42+-0.12 and 2.23+-0.32+-0.17 in the fully hadronic and semileptonic final states respectively. The value quoted is a weighted average without assuming any correlations.


pdgid: S043PRO
text:
ABREU,P 2000F measure <N(p)> = 1.82+-0.29+-0.16 and 0.94+-0.23+-0.06 in the fully hadronic and semileptonic final states respectively. The value quoted is a weighted average without assuming any correlations.


pdgid: S043CHG
text:
ABBIENDI 2006A measure <N(charged)> = 38.74+-0.12+-0.26 when both W bosons decay hadronically and <N(charged)> = 19.39+-0.11+-0.09 when one W boson decays semileptonically.  The value quoted here is obtained under the assumption that there is no color reconnection between W bosons; the value is a weighted average taking into account correlations in the systematic uncertainties.


pdgid: S043CHG
text:
ABREU,P 2000F measure <N(charged)> = 39.12+-0.33+-0.36 and 38.11+-0.57+-0.44 in the fully hadronic final states at 189 and 183 GeV respectively, and <N(charged)> = 19.49+-0.31+-0.27 and 19.78+-0.49+-0.43 in the semileptonic final states. The value quoted is a weighted average without assuming any correlations.


pdgid: S043CHG
text:
ABREU 1998C combine results from both the fully hadronic as well semileptonic W W final states after demonstrating that the W decay charged multiplicity is independent of the topology within errors.


pdgid: S043DG1
text:
ABDALLAH 2010 use data on the final states e+ e- --> j j lepton nu, j j j j, j j X, lepton X,  at center-of-mass energies between 189 -- 209 GeV at LEP2, where j = jet, lepton = lepton, and X  represents missing momentum. The fit is carried out keeping all other parameters fixed at their SM values.


pdgid: S043DG1
text:
SCHAEL 2005A study single-photon, single-W, and WW-pair production from 183 to 209 GeV. The result quoted here is derived from the WW-pair production sample. Each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values.


pdgid: S043DG1
text:
ABBIENDI 2004D combine results from W+ W- in all decay channels. Only CP-conserving couplings are considered and each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values. The 95% confidence interval is 0.923<g^Z_1<1.054.


pdgid: S043DG1
text:
ACHARD 2004D study WW-pair production, single-W production and single-photon production with missing energy from 189 to 209 GeV. The result quoted here is obtained from the WW-pair production sample including data from 161 to 183 GeV, ACCIARRI 1999Q. Each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values.


pdgid: S043DG1
text:
SIRUNYAN 2020BA study electroweak production of a W boson in association with two jets,  using W decays in the electron or muon channel. The isolated muons (electrons) are required to  have a transverse momentum larger than 25 (30) GeV, while the transverse momentum of the two jets  has to be larger than 50 and 30 GeV. A total of 2.382 (1.051) million events are selected in the  muon (electron) channel, with a Standard Model expectation of 2.39+-0.17 (1.054+-0.058)  million events. Analyzing the transverse momentum distribution of the charged leptons from W  decay, the following 95% C.L. limit is obtained: 0.971 < g_{{1}}^Z < 1.044.  Combining this result with that from the closely-related electroweak Z-jet-jet production  SIRUNYAN 2018BZ, the limit becomes: 0.979 < g_{{1}}^Z < 1.034.


pdgid: S043DG1
text:
SIRUNYAN 2019CL study W W and W Z production in lepton + jet events, with one W  boson decaying leptonically (electron or muon), and another W or Z boson decaying  hadronically, reconstructed as a single massive large-radius jet. In the electron channel 2,456  (2,235) events are selected in the W W(W Z) category, while in the muon channel 3,996  (3572) events are selected in the W W(W Z) category. Analysing the di-boson invariant mass  distribution, the following 95% C.L. limit is obtained: 0.9939 < g_{{1}}^Z <  1.0074.


pdgid: S043DG1
text:
SIRUNYAN 2018BZ study p p --> Zjet jet events at 13 TeV where Z --> e+ e- / mu+ mu-.  Isolated electrons and muons are selected with pT of the leading/sub-leading lepton >  30/20 GeV and |eta| < 2.4, with the di-lepton invariant  mass within 15 GeV of the  Z mass. The two highest pT jets are selected with pT of the leading/sub-leading jet  > 50/30 GeV respectively and dijet invariant mass > 200 GeV. Templates in the  transverse momentum of the Z are utilized to set limits on the triple gauge couplings in the  EFT and the LEP parametrizations. The following 95% C.L. limit is obtained: 0.965 <  g^Z_1 < 1.042.


pdgid: S043DG1
text:
AABOUD 2017S analyze electroweak production of a W boson in association with two jets at  high dijet invariant mass, with the W boson decaying to electron or muon plus neutrino. In the  signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600  GeV, 30 events are observed in the data with 39+-4 events expected in the Standard Model,  yielding the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: 0.87<g^Z_1<1.12.


pdgid: S043DG1
text:
AABOUD 2017U analyze production of W W or W Z boson pairs with one W boson  decaying to electron or muon plus neutrino, and the other W or Z boson decaying  hadronically. The hadronic decay system is reconstructed as either a resolved two-jet system or as  a single large jet. Analysing the transverse momentum distribution of the hadronic system above 100  GeV yields the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: 0.979 < g^Z_1 < 1.024.


pdgid: S043DG1
text:
KHACHATRYAN 2017O analyse W Z production where each boson decays into electrons or muons.  Events are required to have a tri-lepton invariant mass larger than 100 GeV, with one of the lepton  pairs having an invariant mass within 20 GeV of the Z boson mass. The Z transverse momentum  spectrum is analyzed to set a 95% C.L. limit of: 0.982 < g^Z_1 <  1.035.


pdgid: S043DG1
text:
SIRUNYAN 2017X study p p --> W W/W Z --> lepton nu q qbar production at 8 TeV where  lepton is an electron or muon with pT > 30 or 25 GeV respectively. Suitable cuts  are put on the pT of the dijet system and the missing E(T) of the event yielding a total  of 285 and 204 W V events observed in the electron and muon channels. The following 95%  C.L. limit is obtained: 0.9913 < g_{{1}}^Z < 1.024.


pdgid: S043DG1
text:
AAD 2016AR study W W production in p p collisions and select 6636 W W candidates in decay modes  with electrons or muons with an expected background of 1546+-157 events.  Assuming the LEP  formulation and setting the form-factor Lambda to infinity, a fit to the transverse momentum  distribution of the leading charged lepton, leads to a 95% C.L. range of 0.984  < g^Z_1< 1.027.


pdgid: S043DG1
text:
AAD 2016P study W Z production in p p collisions and select 2091 W Z candidates in 4 decay modes  with electrons and muons, with an expected background of 1825+-7 events. Analyzing the W Z  transverse momentum distribution, the resulting 95% C.L. limit is:  0.981<g^Z_1< 1.029.


pdgid: S043DG1
text:
AAD 2014Y determine the electroweak Z-dijet cross section in 8 TeV p p collisions. Z --> e e and Z --> mu mu decays are selected with the di-lepton pT> 20 GeV and mass in the 81 -- 101 GeV range. Minimum two jets are required with pT> 55 and 45 GeV and no additional jets with pT> 25 GeV in the rapidity interval between them. The normalized pT balance between the Z and the two jets is required to be < 0.15. This leads to a selection of 900 events with dijet mass > 1 TeV. The number of signal and background events expected is 261 and 592 respectively. A Poisson likelihood method is used on an event by event basis to obtain the 95% CL limit 0.5 <g_{{1}}^Z()< 1.26 for a form factor value Lambda = inf.


pdgid: S043DG1
text:
AAD 2013AL study W W production in p p collisions and select 1325 W W candidates in decay modes with electrons or muons with an expected background of 369+-61 events. Assuming the LEP formulation and setting the form-factor Lambda = infinity, a fit to the transverse momentum distribution of the leading charged lepton, leads to a 95% C.L. range of 0.961 < g^Z_1 < 1.052. Supersedes AAD 2012AC.


pdgid: S043DG1
text:
CHATRCHYAN 2013BF determine the W+ W- production cross section using unlike sign di-lepton (e or mu) events with high notpT. The leptons have pT> 20 GeV/c and are isolated. 1134 candidate events are observed with an expected SM background of 247+-34. The pT distribution of the leading lepton is fitted to obtain 95% C.L. limits of 0.905 <= g_{{1}}^Z <= 1.095.


pdgid: S043DG1
text:
AAD 2012CD study W Z production in p p collisions and select 317 W Z candidates in three lepton nu decay modes with an expected background of 68.0+-10.0 events. The resulting 95% C.L. range is: 0.943 < g^Z_1()< 1.093. Supersedes AAD 2012V.


pdgid: S043DG1
text:
AALTONEN 2012AC study W Z production in p pbar collisions and select 63 W Z candidates in three lepton nu decay modes with an expected background of 7.9+-1.0 events. Based on the cross section and shape of the Z transverse momentum spectrum, the following 95% C.L. range is reported: 0.92 < g_{{1}}^Z() < 1.20 for a form factor of Lambda = 2 TeV.


pdgid: S043DG1
text:
ABAZOV 2012AG combine new results with already published results on W gamma, W W and W Z production in order to determine the couplings with increased precision, superseding ABAZOV 2008R, ABAZOV 2011AC, ABAZOV 2009AJ, ABAZOV 2009AD. The 68% C.L. result for a formfactor cutoff of Lambda = 2 TeV is g_{{1}}^Z = 1.022+0.032-0.030.


pdgid: S043DG1
text:
ABAZOV 2011 study the p pbar --> 3 lepton nu process arising in W Z production. They observe 34 W Z candidates with an estimated background of 6 events.  An analysis of the pT spectrum of the Z boson leads to a 95% C.L. limit of 0.944 < g_{{1}}^Z() < 1.154, for a form factor Lambda = 2 TeV.


pdgid: S043DG1
text:
AALTONEN 10K study p pbar --> W+ W- with W --> e/mu nu. The pT of the leading (second) lepton is required to be > 20 (10) GeV. The final number of events selected is 654 of which 320+-47 are estimated to be background. The 95% C.L. interval is 0.76 < g^Z_1()< 1.34 for Lambda = 1.5 TeV and  0.78 < g^Z_1()< 1.30 for Lambda = 2 TeV.


pdgid: S043DG1
text:
ABAZOV 2009AD study the p pbar --> lepton nu2jet process arising in W W and W Z production. They select 12,473 (14,392) events in the electron (muon) channel with an expected di-boson  signal of 436 (527) events. The results on the anomalous couplings are derived from an analysis of the pT spectrum of the 2-jet system and quoted at 68% C.L. and for a form factor of 2 TeV. This measurement is not used for obtaining the mean as it is for a specific form factor. The 95% confidence interval is 0.88 < g_{{1}}^Z()< 1.20.


pdgid: S043DG1
text:
ABAZOV 2009AJ study the p pbar --> 2lepton 2nu process arising in W W production. They select 100 events with an expected W W signal of 65 events. An analysis of the pT spectrum of the two charged leptons leads to 95% C.L. limits of 0.86 < g_{{1}}^Z< 1.3, for a form factor Lambda = 2 TeV.


pdgid: S043DG1
text:
ABDALLAH 2008C determine this triple gauge coupling from the measurement of the spin density  matrix elements in e+ e- --> W+ W- --> ( q q ) ( lepton nu ), where lepton = e or mu. Values of all other couplings are fixed to their standard model values.


pdgid: S043DG1
text:
ABAZOV 2007Z set limits on anomalous TGCs using the measured cross section and pT(Z) distribution in W Z production with both the W and the Z decaying leptonically into electrons and muons. Setting the other couplings to their standard model values, the 95% C.L. limit for a form factor scale Lambda = 2 TeV is 0.86 <g_{{1}}^Z()< 1.35.


pdgid: S043DG1
text:
ABAZOV 2005S study pbar p --> W Z production with a subsequent trilepton decay to lepton nu lepton^' leptonbar^' (lepton and lepton^' = e or mu). Three events (estimated background 0.71+-0.08 events) with WZ decay characteristics are observed from which they derive limits on the anomalous WWZ couplings. The 95% CL limit for a form factor scale Lambda = 1.5 TeV is 0.51 < g^Z_1 < 1.66, fixing lambda_{{Z}}  and kappa_{{Z}} to their Standard Model values.


pdgid: S043DG1
text:
ABREU 2001I combine results from e+ e- interactions at 189 GeV leading to W+ W-  and W e nu_e final states with results from ABREU 1999L at 183 GeV.  The 95% confidence interval is 0.84<g^Z_1<1.13.


pdgid: S043DG1
text:
ABBOTT 1999I perform a simultaneous fit to the W gamma, W W --> dilepton, W W/W Z --> e nu j j,  W W/W Z --> mu nu j j, and W Z --> trilepton data samples. For Lambda = 2.0 TeV, the 95%CL limits are 0.63<g^Z_1<1.57, fixing lambda_{{Z}} and kappa_{{Z}} to their Standard Model values, and assuming Standard Model values for the W W gamma couplings.


pdgid: S043DKG
text:
SCHAEL 2005A study single-photon, single-W, and WW-pair production from 183 to 209 GeV. Each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values.


pdgid: S043DKG
text:
ABBIENDI 2004D combine results from W+ W- in all decay channels. Only CP-conserving couplings are considered and each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values. The 95% confidence interval is 0.73<kappa(gamma)<1.07.


pdgid: S043DKG
text:
ACHARD 2004D study WW-pair production, single-W production and single-photon production with missing energy from 189 to 209 GeV. The result quoted here is obtained including data from 161 to 183 GeV, ACCIARRI 1999Q. Each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values.


pdgid: S043DKG
text:
AABOUD 2017U analyze production of W W or W Z boson pairs with one W boson  decaying to electron or muon plus neutrino, and the other W or Z boson decaying  hadronically. The hadronic decay system is reconstructed as either a resolved two-jet system or as  a single large jet. Analysing the transverse momentum distribution of the hadronic system above 100  GeV yields the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: 0.939 < kappa(gamma) < 1.064.


pdgid: S043DKG
text:
SIRUNYAN 2017X study p p --> W W/W Z --> lepton nu q qbar production at 8 TeV where  lepton is an electron or muon with pT > 30 or 25 GeV respectively. Suitable cuts  are put on the pT of the dijet system and the missing E(T) of the event yielding a total  of 285 and 204 W V events observed in the electron and muon channels. The following 95%  C.L. limit is obtained: 0.956 < kappa_{{gamma}} < 1.063.


pdgid: S043DKG
text:
CHATRCHYAN 2014AB measure W gamma production cross section for p(T)**gamma> 15 GeV and R(lepton gamma) > 0.7, which is the separation between the gamma and the final state charged lepton (e or mu) in the azimuthal angle-pseudorapidity (phi-eta) plane. After background subtraction the number of e nu gamma and mu nu gamma events is determined to be 3200+-325 and 4970+-543 respectively, compatible with expectations from the SM. This leads to a 95% CL limit of 0.62 <kappa(gamma)< 1.29, assuming other parameters have SM values.


pdgid: S043DKG
text:
AAD 2013AN study W gamma production in p p collisions. In events with no additional  jet, 4449 (6578) W decays to electron (muon) are selected, with an expected background of 1662+-262  (2538+-362) events. Analysing the photon pT spectrum above 100 GeV yields a 95%  C.L. limit of 0.59 < kappa(gamma) < 1.46. Supersedes AAD 2012BX.


pdgid: S043DKG
text:
CHATRCHYAN 2013BF determine the W+ W- production cross section using unlike sign di-lepton (e or mu) events with high notpT. The leptons have pT> 20 GeV/c and are isolated. 1134 candidate events are observed with an expected SM background of 247+-34. The pT distribution of the leading lepton is fitted to obtain 95% C.L. limits of 0.79 <= k(gamma) <= 1.22.


pdgid: S043DKG
text:
ABAZOV 2012AG combine new results with already published results on W gamma, W W and W Z production in order to determine the couplings with increased precision, superseding ABAZOV 2008R, ABAZOV 2011AC, ABAZOV 2009AJ, ABAZOV 2009AD. The 68% C.L. result for a formfactor cutoff of Lambda = 2 TeV is kappa(gamma) = 1.048+0.106-0.105.


pdgid: S043DKG
text:
ABAZOV 2011AC study W gamma production in p pbar collisions at 1.96 TeV, with the W decay products containing an electron or a muon. They select 196 (363) events in the electron (muon) mode, with a SM expectation of 190 (372) events. A likelihood fit to the photon E(T) spectrum above 15 GeV yields at 95% C.L. the result: 0.6 <kappa_{{gamma}}< 1.4 for a formfactor Lambda = 2 TeV.


pdgid: S043DKG
text:
CHATRCHYAN 2011M study W gamma production in p p collisions at sqrt(s) = 7 TeV using 36pb**-1 p p data with the W decaying to electron and muon. The total cross section is measured for photon transverse energy E(T)**gamma> 10 GeV and spatial  separation from charged leptons in the plane of pseudo rapidity and azimuthal angle DeltaR(lepton,gamma)> 0.7.  The number of candidate (background) events is 452 (228+-21) for the electron channel and 520 (277+-25) for the muon channel.  Setting other couplings to their standard model value, they derive a 95% CL limit of -0.11 < kappa_{{gamma}}< 2.04.


pdgid: S043DKG
text:
AALTONEN 10K study p pbar --> W+ W- with W --> e/mu nu. The pT of the leading (second) lepton is required to be > 20 (10) GeV. The final number of events selected is 654 of which 320+-47 are estimated to be background. The 95% C.L. interval is 0.37 < kappa(gamma)< 1.72 for Lambda = 1.5 TeV and  0.43 < kappa(gamma)< 1.65 for Lambda = 2 TeV.


pdgid: S043DKG
text:
AARON 2009B study single-W production in e p collisions at 0.3 TeV C.M. energy. They select 53 W --> e / mu events with a standard model expectation of 54.1+-7.4 events. Fitting the transverse momentum spectrum of the hadronic recoil system they obtain a 95% C.L. limit of -3.7<kappa_{{gamma}}<-1.5 or 0.3<kappa_{{gamma}}<1.5, where the ambiguity is due to the quadratic dependence of the cross section to the coupling parameter.


pdgid: S043DKG
text:
ABAZOV 2009AD study the p pbar --> lepton nu2jet process arising in W W and W Z production. They select 12,473 (14,392) events in the electron (muon) channel with an expected di-boson  signal of 436 (527) events. The results on the anomalous couplings are derived from an analysis of the pT spectrum of the 2-jet system and quoted at 68% C.L. and for a form factor of 2 TeV. This measurement is not used for obtaining the mean as it is for a specific form factor. The 95% confidence interval is 0.56 < kappa_{{gamma}}()< 1.55.


pdgid: S043DKG
text:
ABAZOV 2009AJ study the p pbar --> 2lepton 2nu process arising in W W production. They select 100 events with an expected W W signal of 65 events. An analysis of the pT spectrum of the two charged leptons leads to 95% C.L. limits of 0.46 < kappa_{{gamma}}< 1.83, for a form factor Lambda = 2 TeV.


pdgid: S043DKG
text:
ABAZOV 2008R use 0.7 fb**-1 p pbar data at sqrt(s) = 1.96 TeV to select 263 W gamma + X events, of which 187 constitute signal, with the W decaying into an electron or a muon, which is required to be well separated from a photon with E(T)> 9 GeV. A likelihood fit to the photon E(T) spectrum yields a 95% CL limit 0.49 <kappa(gamma)< 1.51 with other couplings fixed to their Standard Model values.


pdgid: S043DKG
text:
AALTONEN 2007L set limits on anomalous TGCs using the pT(W) distribution in W W and W Z  production with the W decaying to an electron or muon and the Z to 2 jets. Setting other couplings  to their standard model value, the 95% C.L. limits are 0.54 <kappa_{{gamma}}< 1.39 for a form factor scale Lambda = 1.5 TeV.


pdgid: S043DKG
text:
ABAZOV 2006H study pbar p --> W W production with a subsequent decay  W W --> e+ nu_e e- nubar_e, W W --> e+- nu_e mu-+ nu_mu  or W W --> mu+ nu_mu mu- nubar_mu. The 95% C.L. limit for a form factor scale Lambda = 1 TeV is - 0.05<kappa(gamma)<2.29, fixing lambda(gamma)=0. With the assumption that the W W gamma and W W Z couplings are equal the 95% C.L. one-dimensional limit (Lambda = 2 TeV) is 0.68 <kappa< 1.45.


pdgid: S043DKG
text:
ABAZOV 2005J perform a likelihood fit to the photon E(T) spectrum of W gamma + X events, where the W decays to an electron or muon which is required to be well separated from the photon.  For Lambda = 2.0 TeV the 95% CL limits are 0.12 < kappa_{{gamma}} < 1.96. In the fit lambda(gamma) is kept fixed to its Standard Model value.


pdgid: S043DKG
text:
ABREU 2001I combine results from e+ e- interactions at 189 GeV leading to W+ W-, W e nu_e, and nu nubar gamma final states with results from ABREU 1999L at 183 GeV.  The 95% confidence interval is 0.87<kappa_{{gamma}}<1.68.


pdgid: S043DKG
text:
BREITWEG 2000 search for W production in events with large hadronic pT.  For pT>20 GeV, the upper limit on the cross section gives the 95%CL limit -3.7<kappa_{{gamma}}<2.5 (for lambda(gamma)=0).


pdgid: S043DKG
text:
ABBOTT 1999I perform a simultaneous fit to the W gamma, W W --> dilepton, W W/W Z --> e nu j j,  W W/W Z --> mu nu j j, and W Z --> trilepton data samples. For Lambda = 2.0 TeV, the 95%CL limits are 0.75<kappa_{{gamma}}<1.39.


pdgid: S043LG
text:
ABBIENDI 2004D combine results from W+ W- in all decay channels. Only CP-conserving couplings are considered and each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values. The 95% confidence interval is -0.13<lambda(gamma)<0.01.


pdgid: S043LG
text:
CHATRCHYAN 2014AB measure W gamma production cross section for p(T)**gamma> 15 GeV and R(lepton gamma) > 0.7, which is the separation between the gamma and the final state charged lepton (e or mu) in the azimuthal angle-pseudorapidity (phi-eta) plane. After background subtraction the number of e nu gamma and mu nu gamma events is determined to be 3200+-325 and 4970+-543 respectively, compatible with expectations from the SM. This leads to a 95% CL limit of -0.050 <lambda(gamma)< 0.037, assuming all other parameters have SM values.


pdgid: S043LG
text:
AAD 2013AN study W gamma production in p p collisions. In events with no additional jet, 4449 (6578) W decays to electron (muon) are selected, with an expected background of 1662+-262 (2538+-362) events. Analysing the photon pT spectrum above 100 GeV yields a 95% C.L. limit of -0.065 < lambda(gamma) < 0.061. Supersedes AAD 2012BX.


pdgid: S043LG
text:
ABAZOV 2012AG combine new results with already published results on W gamma, W W and W Z production in order to determine the couplings with increased precision, superseding ABAZOV 2008R, ABAZOV 2011AC, ABAZOV 2009AJ, ABAZOV 2009AD. The 68% C.L. result for a formfactor cutoff of Lambda = 2 TeV is lambda(gamma) = 0.007+0.021-0.022.


pdgid: S043LG
text:
ABAZOV 2011AC study W gamma production in p pbar collisions at 1.96 TeV, with the W decay products containing an electron or a muon. They select 196 (363) events in the electron (muon) mode, with a SM expectation of 190 (372) events. A likelihood fit to the photon E(T) spectrum above 15 GeV yields at 95% C.L. the result: -0.08 < lambda_{{gamma}} < 0.07 for a formfactor Lambda = 2 TeV.


pdgid: S043LG
text:
CHATRCHYAN 2011M study W gamma production in p p collisions at sqrt(s) = 7 TeV using 36pb**-1 p p data with the W decaying to electron and muon. The total cross section is measured for photon transverse energy E(T)**gamma> 10 GeV and spatial separation from charged leptons in the plane of pseudo rapidity and azimuthal angle DeltaR(lepton,gamma)> 0.7.  The number of candidate (background) events is 452 (228+-21) for the electron channel and 520 (277+-25) for the muon channel.  Setting other couplings to their standard model value, they derive a 95% CL limit of -0.18 < lambda_{{gamma}}< 0.17.


pdgid: S043LG
text:
AARON 2009B study single-W production in e p collisions at 0.3 TeV C.M. energy. They select 53 W --> e / mu events with a standard model expectation of 54.1+-7.4 events. Fitting the transverse momentum spectrum of the hadronic recoil system they obtain a 95% C.L. limit of -2.5<lambda_{{gamma}}< 2.5.


pdgid: S043LG
text:
ABAZOV 2009AD study the p pbar --> lepton nu2jet process arising in W W and W Z production. They select 12,473 (14,392) events in the electron (muon) channel with an expected di-boson  signal of 436 (527) events. The results on the anomalous couplings are derived from an analysis of the pT spectrum of the 2-jet system and quoted at 68% C.L. and for a form factor of 2 TeV. This measurement is not used for obtaining the mean as it is for a specific form factor. The 95% confidence interval is -0.10< lambda_{{gamma}}()< 0.11.


pdgid: S043LG
text:
ABAZOV 2009AJ study the p pbar --> 2lepton 2nu process arising in W W production. They select 100 events with an expected W W signal of 65 events. An analysis of the pT spectrum of the two charged leptons leads to 95% C.L. limits of -0.14< lambda_{{gamma}}< 0.18, for a form factor Lambda = 2 TeV.


pdgid: S043LG
text:
ABAZOV 2008R use 0.7 fb**-1 p pbar data at sqrt(s) = 1.96 TeV to select 263 W gamma + X events, of which 187 constitute signal, with the W decaying into an electron or a muon, which is required to be well separated from a photon with E(T)> 9 GeV. A likelihood fit to the photon E(T) spectrum yields a 95% CL limit - 0.12<lambda(gamma)< 0.13 with other couplings fixed to their Standard Model values.


pdgid: S043LG
text:
AALTONEN 2007L set limits on anomalous TGCs using the pT(W) distribution in W W and W Z production with the W decaying to an electron or muon and the Z to 2 jets. Setting other couplings to their standard model value, the 95% C.L. limits are -0.18<lambda_{{gamma}}< 0.17 for a form factor scale Lambda = 1.5 TeV.


pdgid: S043LG
text:
ABAZOV 2006H study pbar p --> W W production with a subsequent decay W W --> e+ nu_e e- nubar_e, W W --> e+- nu_e mu-+ nu_mu or W W --> mu+ nu_mu mu- nubar_mu. The 95% C.L. limit for a form factor scale Lambda = 1 TeV is - 0.97<lambda(gamma)< 1.04, fixing kappa(gamma)=1. With the assumption that the W W gamma and W W Z couplings are equal the 95% C.L. one-dimensional limit (Lambda = 2 TeV) is -0.29<lambda< 0.30.


pdgid: S043LG
text:
ABAZOV 2005J perform a likelihood fit to the photon E(T) spectrum of W gamma + X events, where the W decays to an electron or muon which is required to be well separated from the photon. For Lambda = 2.0 TeV the 95% CL limits are -0.20 < lambda(gamma) < 0.20. In the fit kappa_{{gamma}} is kept fixed to its Standard Model value.


pdgid: S043LG
text:
ABREU 2001I combine results from e+ e- interactions at 189 GeV leading to W+ W-, W e nu_e, and nu nubar gamma final states with results from ABREU 1999L at 183 GeV.  The 95% confidence interval is -0.11<lambda_gamma<0.23.


pdgid: S043LG
text:
BREITWEG 2000 search for W production in events with large hadronic pT.  For pT>20 GeV, the upper limit on the cross section gives the 95%CL limit -3.2<lambda(gamma)<3.2 for kappa_{{gamma}} fixed to its Standard Model value.


pdgid: S043LG
text:
ABBOTT 1999I perform a simultaneous fit to the W gamma, W W --> dilepton, W W/W Z --> e nu j j,  W W/W Z --> mu nu j j, and W Z --> trilepton data samples. For Lambda = 2.0 TeV, the 95%CL limits are -0.18<lambda(gamma)<0.19.


pdgid: S043DKZ
text:
ACHARD 2004D study WW-pair production, single-W production and single-photon production with missing energy from 189 to 209 GeV. The result quoted here is obtained using the WW-pair production sample. Each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values.


pdgid: S043DKZ
text:
SIRUNYAN 2020BA study electroweak production of a W boson in association with two jets,  using W decays in the electron or muon channel. The isolated muons (electrons) are required to  have a transverse momentum larger than 25 (30) GeV, while the transverse momentum of the two jets  has to be larger than 50 and 30 GeV. A total of 2.382 (1.051) million events are selected in the  muon (electron) channel, with a Standard Model expectation of 2.39+-0.17 (1.054+-0.058)  million events. Analysing the transverse momentum distribution of the charged leptons from W  decay, the following 95% C.L. limit is obtained: 0.956 < kappa_{{Z}} < 1.044.  Combining this result with that from the closely-related electroweak Z-jet-jet production  SIRUNYAN 2018BZ, the limit becomes: 0.957 < kappa_{{Z}} < 1.042.


pdgid: S043DKZ
text:
SIRUNYAN 2019CL study W W and W Z production in lepton + jet events, with one W  boson decaying leptonically (electron or muon), and another W or Z boson decaying  hadronically, reconstructed as a single massive large-radius jet. In the electron channel 2,456  (2,235) events are selected in the W W(W Z) category, while in the muon channel 3,996  (3572) events are selected in the W W(W Z) category. Analysing the di-boson invariant mass  distribution, the following 95% C.L. limit is obtained: 0.9921 < kappa_{{Z}} <  1.0082.


pdgid: S043DKZ
text:
AABOUD 2017S analyze electroweak production of a W boson in association with two jets at  high dijet invariant mass, with the W boson decaying to electron or muon plus neutrino. In the  signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600  GeV, 30 events are observed in the data with 39+-4 events expected in the Standard Model,  yielding the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: 0.85<kappa_{{Z}}<1.16.


pdgid: S043DKZ
text:
KHACHATRYAN 2017O analyse W Z production where each boson decays into electrons or muons.  Events are required to have a tri-lepton invariant mass larger than 100 GeV, with one of the lepton  pairs having an invariant mass within 20 GeV of the Z boson mass. The Z transverse momentum  spectrum is analyzed to set a 95% C.L. limit of: 0.79 < kappa_{{Z}} <  1.25.


pdgid: S043DKZ
text:
AAD 2016AR study W W production in pp collisions and select 6636 WW candidates in decay modes  with electrons or muons with an expected background of 1546+-157 events.  Assuming the LEP  formulation and setting the form-factor Lambda to infinity, a fit to the transverse  momentum distribution of the leading charged lepton, leads to a 95% C.L. range of 0.975  <kappa_{{Z}}< 1.020.


pdgid: S043DKZ
text:
AAD 2016P study W Z production in p p collisions and select 2091 W Z candidates in 4 decay modes  with electrons and muons, with an expected background of 1825+-7 events. Analyzing the W Z transverse momentum distribution, the resulting 95% C.L. limit is:  0.81 <kappa_{{Z}}< 1.30.


pdgid: S043DKZ
text:
AAD 2013AL study W W production in p p collisions and select 1325 W W candidates in decay modes with electrons or muons with an expected background of 369+-61 events. Assuming the LEP formulation and setting the form-factor Lambda = infinity, a fit to the transverse momentum distribution of the leading charged lepton, leads to a 95% C.L. range of 0.957 < kappa_{{Z}} < 1.043. Supersedes AAD 2012AC.


pdgid: S043DKZ
text:
AAD 2012CD study W Z production in p p collisions and select 317 W Z candidates in three lepton nu decay modes with an expected background of 68.0+-10.0 events. The resulting 95% C.L. range is: 0.63 < kappa_{{Z}}()< 1.57. Supersedes AAD 2012V.


pdgid: S043DKZ
text:
AALTONEN 2012AC study W Z production in p pbar collisions and select 63 W Z candidates in three lepton nu decay modes with an expected background of 7.9+-1.0 events. Based on the cross section and shape of the Z transverse momentum spectrum, the following 95% C.L. range is reported: 0.61 < kappa_{{Z}}() < 1.90 for a form factor of Lambda = 2 TeV.


pdgid: S043DKZ
text:
ABAZOV 2011 study the p pbar --> 3 lepton nu process arising in W Z production. They observe 34 W Z candidates with an estimated background of 6 events. An analysis of the pT spectrum of the Z boson leads to a 95% C.L. limit of 0.600 <kappa_{{Z}}()< 1.675, for a form factor Lambda = 2 TeV.


pdgid: S043DKZ
text:
ABAZOV 2006H study pbar p --> W W production with a subsequent decay W W --> e+ nu_e e- nubar_e, W W --> e+- nu_e mu-+ nu_mu or W W --> mu+ nu_mu mu- nubar_mu. The 95% C.L. limit for a form factor scale Lambda = 2 TeV is 0.55 <kappa(Z)< 1.55, fixing lambda(Z)=0. With the assumption that the W W gamma and W W Z couplings are equal the 95% C.L. one-dimensional limit (Lambda = 2 TeV) is 0.68 <kappa< 1.45.


pdgid: S043DKZ
text:
ABAZOV 2005S study pbar p --> W Z production with a subsequent trilepton decay to lepton nu lepton^' leptonbar^' (lepton and lepton^' = e or mu). Three events (estimated background 0.71+-0.08 events) with WZ decay characteristics are observed from which they derive limits on the anomalous WWZ couplings. The 95% CL limit for a form factor scale Lambda = 1 TeV is -1.0 < kappa_{{Z}} < 3.4, fixing lambda_{{Z}} and g^Z_1 to their Standard Model values.


pdgid: S043LZ
text:
SIRUNYAN 2020BA study electroweak production of a W boson in association with two jets,  using W decays in the electron or muon channel. The isolated muons (electrons) are required to  have a transverse momentum larger than 25 (30) GeV, while the transverse momentum of the two jets  has to be larger than 50 and 30 GeV. A total of 2.382 (1.051) million events are selected in the  muon (electron) channel, with a Standard Model expectation of 2.39+-0.17 (1.054+-0.058)  million events. Analysing the transverse momentum distribution of the charged leptons from W  decay, the following 95% C.L. limit is obtained: -0.0088 < lambda_{{Z}} < 0.0095.  Combining this result with that from the closely-related electroweak Z-jet-jet production  SIRUNYAN 2018BZ, the limit becomes: $-0.0071 < lambda_Z < 0.0076$.


pdgid: S043LZ
text:
SIRUNYAN 2019CL study W W and W Z production in lepton + jet events, with one W  boson decaying leptonically (electron or muon), and another W or Z boson decaying  hadronically, reconstructed as a single massive large-radius jet. In the electron channel 2,456  (2,235) events are selected in the W W(W Z) category, while in the muon channel 3,996  (3572) events are selected in the W W(W Z) category. Analysing the di-boson invariant mass  distribution, the following 95% C.L. limit is obtained: -0.0065 < lambda_{{Z}}  < 0.0066.


pdgid: S043LZ
text:
SIRUNYAN 2018BZ study p p --> Zjet jet events at 13 TeV where Z --> e+ e- / mu+ mu-.  Isolated electrons and muons are selected with pT of the leading/sub-leading lepton >  30/20 GeV and |eta| < 2.4, with the di-lepton invariant  mass within 15 GeV of the  Z mass. The two highest pT jets are selected with pT of the leading/sub-leading jet  > 50/30 GeV respectively and dijet invariant mass > 200 GeV. Templates in the  transverse momentum of the Z are utilized to set limits on the triple gauge couplings in the  EFT and the LEP parametrizations. The following 95% C.L. limit is obtained -0.010  <lambda_{{Z}}< 0.010.


pdgid: S043LZ
text:
AABOUD 2017S analyze electroweak production of a W boson in association with two jets at  high dijet invariant mass, with the W boson decaying to electron or muon plus neutrino. In the  signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600  GeV, 30 events are observed in the data with 39+-4 events expected in the Standard Model,  yielding the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: -0.053 <lambda_{{Z}}< 0.042.


pdgid: S043LZ
text:
AABOUD 2017U analyze production of W W or W Z boson pairs with one W boson  decaying to electron or muon plus neutrino, and the other W or Z boson decaying  hadronically. The hadronic decay system is reconstructed as either a resolved two-jet system or as  a single large jet. Analysing the transverse momentum distribution of the hadronic system above 100  GeV yields the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: -0.013 < lambda_{{Z}} < 0.013.


pdgid: S043LZ
text:
KHACHATRYAN 2017O analyse W Z production where each boson decays into electrons or muons.  Events are required to have a tri-lepton invariant mass larger than 100 GeV, with one of the lepton  pairs having an invariant mass within 20 GeV of the Z boson mass. The Z transverse momentum  spectrum is analyzed to set a 95% C.L. limit of: -0.018 < lambda_{{Z}} <  0.016.


pdgid: S043LZ
text:
SIRUNYAN 2017X study p p --> W W/W Z --> lepton nu q qbar production at 8 TeV where  lepton is an electron or muon with pT > 30 or 25 GeV respectively. Suitable cuts  are put on the pT of the dijet system and the missing E(T) of the event yielding a total  of 285 and 204 W V events observed in the electron and muon channels. The following 95%  C.L. limit is obtained: -0.011 < lambda_{{Z}} < 0.011.


pdgid: S043LZ
text:
AAD 2016AR study WW production in p p collisions and select 6636 W W candidates in decay modes  with electrons or muons with an expected background of 1546+-157 events.  Assuming the LEP  formulation and setting the form-factor Lambda to infinity, a fit to the transverse momentum  distribution of the leading charged lepton, leads to a 95% C.L. range of -0.019  <lambda_{{Z}}< 0.019.


pdgid: S043LZ
text:
AAD 2016P study W Z production in p p collisions and select 2091 W Z candidates in 4 decay modes with electrons and muons, with an expected background of 1825+-7 events. Analyzing the W Z transverse momentum distribution, the resulting 95% C.L. limit is: -0.016  <lambda_{{Z}}< 0.016.


pdgid: S043LZ
text:
AAD 2014Y determine the electroweak Z-dijet cross section in 8 TeV p p collisions. Z --> e e and Z --> mu mu decays are selected with the di-lepton pT> 20 GeV and mass in the 81 -- 101 GeV range. Minimum two jets are required with pT> 55 and 45 GeV and no additional jets with pT> 25 GeV in the rapidity interval between them. The normalized pT balance between the Z and the two jets is required to be < 0.15. This leads to a selection of 900 events with dijet mass > 1 TeV. The number of signal and background events expected is 261 and 592 respectively. A Poisson likelihood method is used on an event by event basis to obtain the 95% CL limit -0.15 <lambda_{{Z}}() < 0.13 for a form factor value Lambda = inf.


pdgid: S043LZ
text:
AAD 2013AL study W W production in p p collisions and select 1325 W W candidates in decay modes with electrons or muons with an expected background of 369+-61 events. Assuming the LEP formulation and setting the form-factor Lambda = infinity, a fit to the transverse momentum distribution of the leading charged lepton, leads to a 95% C.L. range of -0.062 < lambda_{{Z}} < 0.059. Supersedes AAD 2012AC.


pdgid: S043LZ
text:
CHATRCHYAN 2013BF determine the W+ W- production cross section using unlike sign  di-lepton (e or mu) events with high notpT. The leptons have pT> 20  GeV/c and are isolated. 1134 candidate events are observed with an expected SM background of 247+-34.  The pT distribution of the leading lepton is fitted to obtain 95% C.L. limits of  -0.048 <= lambda_{{Z}} <= 0.048.


pdgid: S043LZ
text:
AAD 2012CD study W Z production in p p collisions and select 317 W Z candidates in three lepton nu decay modes with an expected background of 68.0+-10.0 events. The resulting 95% C.L. range is: -0.046 < lambda_{{Z}}()< 0.047. Supersedes AAD 2012V.


pdgid: S043LZ
text:
AALTONEN 2012AC study W Z production in p pbar collisions and select 63 W Z candidates in three lepton nu decay modes with an expected background of 7.9+-1.0 events. Based on the cross section and shape of the Z transverse momentum spectrum, the following 95% C.L. range is reported: -0.08 < lambda_{{Z}}() < 0.10 for a form factor of Lambda = 2 TeV.


pdgid: S043LZ
text:
ABAZOV 2011 study the p pbar --> 3 lepton nu process arising in W Z production. They observe 34 W Z candidates with an estimated background of 6 events.  An analysis of the pT spectrum of the Z boson leads to a 95% C.L. limit of -0.077< lambda_{{Z}}()< 0.093, for a form factor Lambda = 2 TeV.


pdgid: S043LZ
text:
AALTONEN 10K study p pbar --> W+ W- with W --> e/mu nu. The pT of the leading (second) lepton is required to be > 20 (10) GeV. The final number of events selected is 654 of which 320+-47 are estimated to be background. The 95% C.L. interval is -0.16 < lambda_{{Z}}()< 0.16 for Lambda = 1.5 TeV and  -0.14 < lambda_{{Z}}()< 0.15 for Lambda = 2 TeV.


pdgid: S043LZ
text:
ABAZOV 2007Z set limits on anomalous TGCs using the measured cross section and pT(Z) distribution in W Z production with both the W and the Z decaying leptonically into electrons and muons. Setting the other couplings to their standard model values, the 95% C.L. limit for a form factor scale Lambda = 2TeV is -0.17 <lambda_{{Z}}< 0.21.


pdgid: S043LZ
text:
ABAZOV 2006H study pbar p --> W W production with a subsequent decay W W --> e+ nu_e e- nubar_e, W W --> e+- nu_e mu-+ nu_mu or W W --> mu+ nu_mu mu- nubar_mu. The 95% C.L. limit for a form factor scale Lambda = 2 TeV is -0.39 <lambda(Z)< 0.39, fixing kappa(Z)=1. With the assumption that the W W gamma and W W Z couplings are equal the 95% C.L. one-dimensional limit (Lambda = 2 TeV) is -0.29 <lambda< 0.30.


pdgid: S043LZ
text:
ABAZOV 2005S study pbar p --> W Z production with a subsequent trilepton decay to lepton nu lepton^' leptonbar^' (lepton and lepton^' = e or mu). Three events (estimated background 0.71+-0.08 events) with WZ decay characteristics are observed from which they derive limits on the anomalous WWZ couplings. The 95% CL limit for a form factor scale Lambda = 1.5 TeV is -0.48 < lambda_{{Z}} < 0.48, fixing g^Z_1 and kappa_{{Z}} to their Standard Model values.


pdgid: S043DG5
text:
ABBIENDI 2004D combine results from W+ W- in all decay channels. Only CP-conserving couplings are considered and each parameter is determined from a single-parameter fit in which the other parameters assume their Standard Model values. The 95% confidence interval is -0.28 < g(5)**Z<+0.21.


pdgid: S043DG5
text:
EBOLI 2000 extract this indirect value of the coupling studying the non-universal one-loop contributions to the experimental value of the Z --> b bbar width (Lambda=1 TeV is assumed).


pdgid: S043GZ4
text:
ABBIENDI 2001H study W-pair events, with one leptonically and one hadronically decaying W.  The coupling is extracted using information from the W production angle together with decay angles from the leptonically decaying W.


pdgid: S043KAZ
text:
AABOUD 2017S analyze electroweak production of a W boson in association with two jets at  high dijet invariant mass, with the W boson decaying to electron or muon plus neutrino. In the  signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600  GeV, 30 events are observed in the data with 39+-4 events expected in the Standard Model,  yielding the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: -0.56 <kappatilde_{{Z}}< 0.56.


pdgid: S043KAZ
text:
BLINOV 2011 use the LEP-average e+ e- --> W+ W- cross section data for sqrt(s) = 183 -- 207 GeV to determine an upper limit on the TGC kappatilde_{{Z}}. The average values of the cross sections as well as their correlation matrix, and standard model expectations of the cross sections are taken from the LEPEWWG note hep-ex/0612034. At 95% confidence level |kappatilde_{{Z}}| < 0.13.


pdgid: S043LAZ
text:
AABOUD 2017S analyze electroweak production of a W boson in association with two jets at  high dijet invariant mass, with the W boson decaying to electron or muon plus neutrino. In the  signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600  GeV, 30 events are observed in the data with 39+-4 events expected in the Standard Model,  yielding the following limit at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: -0.047 <lambdatilde_{{Z}}< 0.046.


pdgid: S043LAZ
text:
BLINOV 2011 use the LEP-average e+ e- --> W+ W- cross section data for sqrt(s) = 183 -- 207 GeV to determine an upper limit on the TGC lambdatilde_{{Z}}. The average values of the cross sections as well as their correlation matrix, and standard model expectations of the cross sections are taken from the LEPEWWG note hep-ex/0612034. At 95% confidence level |lambdatilde_{{Z}}| < 0.31.


pdgid: S043WMG
text:
ABREU 2001I combine results from e+ e- interactions at 189 GeV leading to W+ W-, W e nu_e, and nu nubar gamma final states with results from ABREU 1999L at 183 GeV to determine Delta g^Z_1, Delta kappa_gamma, and lambda_gamma. Delta kappa_gamma and lambda_gamma are simultaneously floated in the fit to determine mu(W).


pdgid: S043WMG
text:
ABE 1995G report -1.3<kappa<3.2 for lambda=0 and -0.7<lambda<0.7 for kappa=1 in p pbar --> e nu_e gamma X and mu nu_mu gamma X at sqrt(s) = 1.8 TeV.


pdgid: S043WMG
text:
ALITTI 1992C measure kappa = 1+2.6-2.2 and lambda = 0+1.7-1.8 in p pbar --> e nu gamma + X at sqrt(s) = 630 GeV.  At 95%CL they report -3.5<kappa<5.9 and -3.6<lambda<3.5.


pdgid: S043WMG
text:
SAMUEL 1992 use preliminary CDF and UA2 data and find -2.4<kappa<3.7 at 96%CL and -3.1<kappa<4.2 at 95%CL respectively.  They use data for W gamma production and radiative W decay.


pdgid: S043WMG
text:
SAMUEL 1991 use preliminary CDF data for p pbar --> W gamma X to obtain -11.3 <= Deltakappa <= 10.9.  Note that their kappa = 1-Deltakappa.


pdgid: S043WMG
text:
GROTCH 1987 finds the limit -37 < Deltakappa < 73.5 (90% CL) from the experimental limits on e+ e- --> nu nubar gamma assuming three neutrino generations and -19.5 < Deltakappa < 56 for four generations.  Note their Deltakappa has the opposite sign as our definition.


pdgid: S043WMG
text:
VANDERBIJ 1987 uses existing limits to the photon structure to obtain |Deltakappa| < 33 (mass(W)/Lambda).  In addition VANDERBIJ 1987 discusses problems with using the rho parameter of the Standard Model to determine Deltakappa.


pdgid: S043WMG
text:
GRAU 1985 uses the muon anomaly to derive a coupled limit on the anomalous magnetic dipole and electric quadrupole (lambda) moments 1.05 >Deltakappa ln(Lambda/mass(W)) + lambda/2 >-2.77.  In the Standard Model lambda = 0.


pdgid: S043WMG
text:
SUZUKI 1985 uses partial-wave unitarity at high energies to obtain |Deltakappa| ~< 190 (mass(W)/Lambda)**2. From the anomalous magnetic moment of the muon, SUZUKI 1985 obtains |Deltakappa| ~< 2.2/ln(Lambda/mass(W)). Finally SUZUKI 1985 uses deviations from the rho parameter and obtains a very qualitative, order-of-magnitude limit |Deltakappa| ~< 150 (mass(W)/Lambda)**4 if |Deltakappa| <<1.


pdgid: S043WMG
text:
HERZOG 1984 consider the contribution of W-boson to muon magnetic moment including anomalous coupling of W W gamma.  Obtain a limit -1 < Deltakappa < 3 for Lambda ~> 1 TeV.


pdgid: S043A00
text:
TUMASYAN 2022AB study W Z  production, measuring cross sections and various  distributions. Analysing the W Z invariant  mass distribution, the following 95% C.L.  limits are derived in units of TeV**-2:  -2.5 < c(W)/Lambda**2 < 0.3,  -1.0 < c(WWW)/Lambda**2 <  1.2, -43 < c(b)/Lambda**2 <  113, -0.62 < ctilde(WWW)/Lambda**2  < 0.53, -32 <  ctilde(W)/Lambda**2 < 32.


pdgid: S043A00
text:
TUMASYAN 2022E measure W gamma production where the W boson decays to electrons or  muons. Analysing the photon transverse momentum distribution in bins of lepton azimuth, the  following 95% C.L. limit is derived in units of TeV**-2: -0.062 <  c(3W)/Lambda**2 < 0.052. This limit is derived including the non-SM, SM and their  interference effects.


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AAD 2021AC study the differential cross-section for the electroweak production of dijets in   association with a Z boson, where the Z boson decays to electrons or muons. The number of   events selected in the data is 10,870 (12,125) in the electron (muon) channel. Analyzing the   distribution of the azimuthal separation of the two jets, the following 95% C.L. limits are   derived in units of TeV**-2: -2.7 < c(W W W)/Lambda**2 < 5.8, -1.6   < ctilde(W W W)/Lambda**2 < 2.0, -0.19 < c(W)/Lambda**2   < 0.41, -0.11 < ctilde(W)/Lambda**2 < 0.14, -6.31 <   c(H W B)/Lambda**2 < 1.01, 0.23 < ctilde(H W B)/Lambda**2 <   2.35.


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AAD 2021W analyze W+ W- production in association with at least one jet. Events with  exactly one oppositely-charged electron-muon pair and at least one hadronic jet of transverse  momentum larger than 30 GeV (120 GeV) are selected. In the data, 89,239 (5,825) events are found,  with a total Standard-Model expectation of 91600+-2500 (5980+-150). Analyzing the  electron-muon invariant mass distribution, the following limit at 95% C.L. is obtained:  -0.33 < c(W)/Lambda**2 < 0.33 (-0.60 < c(W)/Lambda**2 <  0.58), for a fixed choice of Lambda = 1 TeV.


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SIRUNYAN 2021G measure W gamma production where the W decays into electrons or muons.  In the data, 385,224 (395,818) events are selected in the electron (muon) channel, with a total  Standard-Model expectation of 396913+-54686 (396257+-22837) events. Analysing the photon  transverse momentum distribution, the following 95% C.L. limits are derived in units of  TeV**-2: -0.90 < c(W W W)/Lambda**2 < 0.91, -40 <  c(B)/Lambda**2 < 41, -0.45 < c(Wbar W W)/Lambda**2 < 0.45,  -20 < c(Wbar)/Lambda**2 < 20.


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SIRUNYAN 2020BA study electroweak production of a W boson in association with two jets,  using W decays in the electron or muon channel. The isolated muons (electrons) are required to  have a transverse momentum larger than 25 (30) GeV, while the transverse momentum of the two jets  has to be larger than 50 and 30 GeV. A total of 2.382 (1.051) million events are selected in the  muon (electron) channel, with a Standard Model expectation of 2.39+-0.17 (1.054+-0.058)  million events. Analysing the transverse momentum distribution of the charged leptons from W  decay, the following 95% C.L. limits are obtained in units of TeV**-2: -2.3 <  c_{{WWW}}/Lambda**2 < 2.5, -8.8 < c_{{W}}/Lambda**2 <  16, -45 < c_{{B}}/Lambda**2 < 46.  Combining these results with those from the closely-related electroweak Z-jet-jet production  SIRUNYAN 2018BZ, the limits become:  -1.8 < c_{{WWW}}/Lambda**2 < 2.0,  -5.8 < c_{{W}}/Lambda**2 < 10, -43 < c_{{B}}/Lambda**2 < 45.


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SIRUNYAN 2020BF study W+ W- production with the W bosons decaying to electrons or  muons. The leading (subleading) lepton is required to have a transverse momentum larger than 25  (20) GeV. Events with a same-flavor di-lepton invariant mass within 15 GeV of the Z mass are  rejected, as are event with a third lepton of transverse momentum larger than 10 GeV. In the same-  (different-) flavor category a total of 9,604 (20,270) events are selected while the number of  expected events is 9640+-490 (20280+-430). Analyzing the different-flavor di-lepton  invariant mass distribution, the following 95% C.L. limits are obtained in units of  TeV**-2: -1.8 < c_{{WWW}}/Lambda**2 < 1.8, -3.6 < c_{{W}}/Lambda**2  < 2.8, -9.4 < c_{{B}}/Lambda**2 < 8.5.


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AABOUD 2019BA study W W production in decay modes with an electron and a muon. The  charged leptons are each required to have a transverse momentum larger than 27 GeV and rapidity  less than 2.5. The electron-muon system is required to have a mass larger than 55 GeV and a  transverse momentum larger than 30 GeV. The missing transverse energy must be larger than 20 GeV.   Events containing a jet with transverse momentum exceeding 35 GeV and rapidity smaller than 4.5 are  rejected. A total of 12,659 events are selected in the data, with an expected background of 4240+-477  events. Analysing the transverse momentum spectrum of the leading charged lepton, the following  95% C.L. limits are derived in units of TeV**-2: -3.4 < c_{{WWW}}/Lambda**2  < 3.3, -7.4 < c_{{W}}/Lambda**2 < 4.1, -21 < c_{{B}}/Lambda**2  < 18, -1.6 < c(Wbar W W)/Lambda**2 < 1.6, -76 <  c(Wbar)/Lambda**2 < 76.


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SIRUNYAN 2019AD study inclusive W Z production, with W and Z decaying to  electrons or muons. The leading (subleading) charged lepton candidate from the Z boson decay is  required to have a transverse momentum larger than 25 GeV (10 GeV). The charged lepton candidate  from the W boson decay is required to have a transverse momentum larger than 25 GeV. The  invariant mass of the two leptons from Z decay is required to be within 15 GeV of the Z  mass, while the invariant mass of the tri-lepton system is required to exceed 100 GeV. A total of  3,831 tri-lepton events are observed, with a fitted SM W Z signal of 3166+-62 events and a  fitted background of 666+-45 events. The approximated W Z invariant mass distribution is  analyzed to set 95% C.L. limits as follows: -4.1 < c_{{W}}/Lambda**2 < 1.1,  -2.0 < c_{{WWW}}/Lambda**2 < 2.1, -100 < c_{{B}}/Lambda**2 < 160,  in units of TeV**-2.


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SIRUNYAN 2019CL study W W and W Z production in lepton + jet events, with one W  boson decaying leptonically (electron or muon), and another W or Z boson decaying  hadronically, reconstructed as a single massive large-radius jet. In the electron channel 2,456  (2,235) events are selected in the W W(W Z) category, while in the muon channel 3,996  (3572) events are selected in the W W(W Z) category. Analysing the di-boson invariant mass  distribution, the following 95% C.L. limits are obtained in units of TeV**-2: -1.58  < c_{{WWW}}/Lambda**2 < 1.59, -2.00 < c_{{W}}/Lambda**2 < 2.65,  -8.78 < c_{{B}}/Lambda**2 < 8.54.


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AABOUD 2018Q study p p --> Z Z events at sqrt(s) = 13 TeV with Z --> e+ e- or Z --> mu+ mu-. The  number of events observed in the 4e, 2e 2mu, and 4mu channels is 249, 465, and 303  respectively. Analysing the pT spectrum of the leading Z boson, the following the  following 95% C.L. limits are derived in units of TeV**-4: -5.9 <  c(Btilde W)/Lambda**4 < 5.9, -3.0 < c_{{WW}}/Lambda**4 <  3.0, -3.3 < c_{{BW}}/Lambda**4 < 3.3, -2.7 < c_{{BB}}/Lambda**4  < 2.8.


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SIRUNYAN 2018BZ study p p --> Zjet jet events at 13 TeV where Z --> e+ e- / mu+ mu-.  Isolated electrons and muons are selected with pT of the leading/sub-leading lepton >  30/20 GeV and |eta| < 2.4, with the di-lepton invariant  mass within 15 GeV of the  Z mass. The two highest pT jets are selected with pT of the leading/sub-leading jet  > 50/30 GeV respectively and dijet invariant mass > 200 GeV. Templates in the  transverse momentum of the Z are utilized to set limits on the triple gauge couplings in the  EFT and the LEP parametrizations. The following 95% C.L. limits are obtained in units of  TeV**-2: -2.6<c_{{WWW}}/Lambda**2< 2.6 and  -8.4<c_{{W}}/Lambda**2< 10.1.


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AABOUD 2017S analyze electroweak production of a W boson in association with two jets at  high dijet invariant mass, with the W boson decaying to electron or muon plus neutrino. In the  signal region of dijet mass larger than 1 TeV and leading-jet transverse momentum larger than 600  GeV, 30 events are observed in the data with 39+-4 events expected in the Standard Model,  yielding the following limits at 95% CL for the form factor cut-off scale  Lambda_{{FF}}-->inf: -33 < c_{{W}}/Lambda**2 < 30, -170  < c_{{B}}/Lambda**2 < 160, -13 < c_{{WWW}}/Lambda**2 < 9,  -580 < c(Wtilde)/Lambda**2 < 580, -11 <  c(WtildeWW)/Lambda**2 < 11, in units of TeV**-2.


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AABOUD 2017U analyze production of W W or W Z boson pairs with one W boson  decaying to electron or muon plus neutrino, and the other W or Z boson decaying  hadronically. The hadronic decay system is reconstructed as either a resolved two-jet system or as  a single large jet. Analysing the transverse momentum distribution of the hadronic system above 100  GeV yields the following limits at 95% CL for the form factor cut-off scale Lambda_{{FF}}  --> inf: -3.1 < c_{{WWW}}/Lambda**2 < 3.1, -19 <  c_{{B}}/Lambda**2 < 20, -5.1 < c_{{W}}/Lambda**2 < 5.8, in units of  TeV**-2.


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KHACHATRYAN 2017O analyse W Z production where each boson decays into electrons or muons.  Events are required to have a tri-lepton invariant mass larger than 100 GeV, with one of the lepton  pairs having an invariant mass within 20 GeV of the Z boson mass. The Z transverse momentum  spectrum is analyzed to set 95% C.L. limits of: -260 < c_{{B}}/Lambda**2 <  210, -4.2 < c_{{W}}/Lambda**2 < 8.0, -4.6 <  c_{{WWW}}/Lambda**2 < 4.2, in units of TeV**-2.


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SIRUNYAN 2017X study p p --> W W/W Z --> lepton nu q qbar production at 8 TeV where  lepton is an electron or muon with pT > 30 or 25 GeV respectively. Suitable cuts  are put on the pT of the dijet system and the missing E(T) of the event yielding a total  of 285 and 204 W V events observed in the electron and muon channels. The following 95%  C.L. limits in units of TeV**-2 are obtained: -2.7 < c_{{W W W}}/Lambda**2 <  2.7, -14 < c_{{B}}/Lambda**2 < 17, -2.0 < c_{{W}}/Lambda**2 < 5.7.


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AAD 2016AR study W W production in p p collisions and select 6636 W W candidates in decay modes with electrons or muons with an expected background of 1546+-157 events.  Assuming an EFT  formulation, a fit to the transverse momentum distribution of the leading charged lepton, leads to  95% C.L. ranges of: -4.61<c_{{WWW}}/Lambda**2< 4.60,  -5.87<c_{{W}}/Lambda**2< 10.54 and  -20.9<c_{{B}}/Lambda**2< 26.3,in units of TeV**-2.


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AAD 2016P study W Z production in p p collisions and select 2091 W Z candidates in 4 decay modes with electrons and muons, with an expected background of 1825+-7 events. Analyzing the W Z transverse momentum distribution, the resulting 95% C.L. limits are:  -3.9<c_{{WWW}}/Lambda**2< 4.0,  -4.3<c_{{W}}/Lambda**2< 6.8, and  -320<c_{{B}}/Lambda**2< 210, in units of TeV**-2.


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KHACHATRYAN 2016BI determine the W+ W- production cross section using unlike sign di-lepton (e or mu) events with high pT. The leptons have pT > 20 GeV/c and are isolated. Events are required to have no jets above pT of 30 GeV/c. 4847 (2233) events are selected with different (same) flavor leptons, with an expected total background of 1179+-123 (643+-73) events. Analysing the di-lepton invariant mass spectrum, the following values are obtained:  c_{{WWW}}/Lambda**2 = 0.1+-3.2, c_{{W}}/Lambda**2 = -3.6+5.0-4.5 and  c_{{B}}/Lambda**2= -3.2+15.0-14.5, in units of TeV**-2. The limits at 95% C.L. are:  -5.7<c_{{WWW}}/Lambda**2<5.9, -11.4<c_{{W}}/Lambda**2<5.4 and  -29.2<c_{{B}}/Lambda**2<23.9, in units of TeV**-2.


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AAD 2024AD tag same-sign W W production, with the W bosons decaying into electrons or  muons, in association with at least two jets with large invariant mass and rapidity difference. The  di-lepton invariant mass distribution is used to extract the following 95% C.L. limits:  -4.1 < f(M,0)/Lambda**4 < 4.1, -6.8 < f(M,1)/Lambda**4 <  7.0, -9.8 < f(M,7)/Lambda**4 < 9.5, -5.9 < f(S02)/Lambda**4  < 5.9, -23.5 < f(S,1)/Lambda**4 < 23.6, -0.36 <  f(T,0)/Lambda**4 < 0.36, -0.174< f(T,1)/Lambda**4 < 0.186,  -0.63 < f(T,2)/Lambda**4 < 0.74, in units of TeV**-4.


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AAD 2024AM tag W Z production, with the bosons decaying into electrons or muons, in  association with two jets. The transverse mass of the W Z system is used to extract the  following 95% C.L. limits: -0.57 < f(T,0)/Lambda**4 < 0.56, -0.39  < f(T,1)/Lambda**4 < 0.35, -1.2 < f(T,2)/Lambda**4 < 1.0,  -5.8 < f(M,0)/Lambda**4 < 5.6, -8.6 < f(M,1)/Lambda**4 <  8.5, -11.3 < f(M,7)/Lambda**4 < 11.3, -10.4 < f(S02)/Lambda**4  < 10.4, -30 < f(S,1)/Lambda**4 < 30, in units of TeV**-4.


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AAD 2024C study the production of four charged leptons (electrons or muons) in association  with two jets. Analysing the 4-lepton invariant mass distribution and the di-jet invarinat mass  distribution leads to the following 95% C.L. limits: -0.98 < f(T,0)/Lambda**4  < 0.93, -1.2 < f(T,1)/Lambda**4 < 1.2, -2.5 <  f(T,2)/Lambda**4 < 2.4, -2.5 < f(T,5)/Lambda**4 < 2.4, -3.9  < f(T,6)/Lambda**4 < 3.9, -8.5 < f(T,7)/Lambda**4 < 8.1,  -2.1 < f(T,8)/Lambda**4 < 2.1, -4.5 < f(T,9)/Lambda**4 <  4.5, in units of TeV**-4. The article also reports limits on these couplings by cutting the EFT  expansion at various values of the cut-off scale.


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AAD 2024CH study electroweak W gamma production in association with two jets. The  distribution of the transverse momentum of the two-jet system or of the lepton is analysed to set  the following 95% C.L. limits: -1.8 < f(T,0)/Lambda**4 < 1.8,  -1.1 < f(T,1)/Lambda**4 < 1.2, -3.1 < f(T,2)/Lambda**4  < 3.5, -2.4 < f(T,3)/Lambda**4 < 2.6, -2.2 <  f(T,4)/Lambda**4 < 2.2, -1.2 < f(T,5)/Lambda**4 < 1.3,  -1.0 < f(T,6)/Lambda**4 < 1.1, -2.7 < f(T,7)/Lambda**4  < 2.8, -24 < f(M,0)/Lambda**4 < 24, -37 <  f(M,1)/Lambda**4 < 38, -8.6 < f(M,2)/Lambda**4 < 8.5,  -13 < f(M,3)/Lambda**4 < 14, -15 < f(M,4)/Lambda**4  < 15, -14 < f(M,5)/Lambda**4 < 12, -66 <  f(M,7)/Lambda**4 < 65, in units of TeV**-4.


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AAD 2023BH study p p --> Z gamma gamma events with the Z boson decaying to electron  or muon pairs. The number of observed data events is 148 for the electron mode and 171 for the muon  mode. The respective number of (data-background) events is 105.5+-12.2(stat)+-8.1(syst)  and 120.4+-13.1(stat)+-9.4(syst). The corresponding number of predicted signal events is  91.5+-0.9 and 119.5+-1.0 using SHERPA (NLO), and 91.0+-1.0 and 118.1+-1.2 using  MADGRAPH 5 AMC (NLO), where the error is statistical only. Analysing the transverse momentum  distribution of the dilepton system, the following 95% C.L. limits are derived: -9.87  < f(T,0)/Lambda**4 < 9.33, -9.88 < f(T,1)/Lambda**4 <  9.34, -20.31 < f(T,2)/Lambda**4 < 18.68, -4.64 <  f(T,5)/Lambda**4 < 4.54, -7.04 < f(T,6)/Lambda**4 < 6.94,  -15.55< f(T,7)/Lambda**4 < 15.04, -1.64 < f(T,8)/Lambda**4  < 1.61, -3.26 < f(T,9)/Lambda**4 < 3.26, in units of TeV**-4.


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AAD 2023K measure Z production in association with a photon and two jets in proton-proton  collisions at 13 TeV CM energy, where the Z boson decays into neutrinos. Within a sensitive  fiducial phase-space region, 356 signal events are selected, with an expectation of 357+-30.  Analysing the photon transverse energy distribution, the following 95% C.L. limits are  derived in units of TeV**-4: -0.094 < f(T,0)/Lambda**4 < 0.084,  -0.088 < f(T,5)/Lambda**4 < 0.099, -0.059 <  f(T,8)/Lambda**4 < 0.059, -0.13 < f(T,9)/Lambda**4 < 0.13,  -4.6 < f(M,0)/Lambda**4 < 4.6, -7.7 < f(M,1)/Lambda**4  < 7.7, -1.9 < f(M,2)/Lambda**4 < 1.9.


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TUMASYAN 2023AK study electroweak W gamma production in association with 2 jets. The  events selected for the couplings analysis are required to have a dijet invariant mass in excess of  800 GeV, jet-jet separation of at least 2.5 in rapidity, invariant mass of the W gamma system  larger than 150 GeV and transverse photon momentum larger than 100 GeV. Analysing the W gamma  invariant mass distribution, varying one coupling at a time while fixing the others to their  Standard Model value, leads to the following 95% C.L. limits: -5.6 <  f(M,0)/Lambda**4 < 5.5, -7.8 < f(M,1)/Lambda**4 < 8.1,  -1.9 < f(M,2)/Lambda**4 < 1.9, -2.7 < f(M,3)/Lambda**4  < 2.7, -3.7 < f(M,4)/Lambda**4 < 3.6, -3.9 <  f(M,5)/Lambda**4 < 3.9, -14 < f(M,7)/Lambda**4 < 14,  -0.47 < f(T,0)/Lambda**4 < 0.51, -0.31 < f(T,1)/Lambda**4  < 0.34, -0.85 < f(T,2)/Lambda**4 < 1.0, -0.31 <  f(T,5)/Lambda**4 < 0.33, -0.25 < f(T,6)/Lambda**4 < 0.27,  -0.67 < f(T,7)/Lambda**4 < 0.73, in units of TeV**-4.


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TUMASYAN 2023AM use the combined CMS-TOTEM detector system to study exclusive gamma gamma --> W W  and gamma gamma --> Z Z production in p p collisions at 13 TeV. The W and Z are  identified through their hadronic decays with the added requirements of the invariant mass of the  di-boson pair to be larger than 1 TeV, and the relative beam proton momentum loss between 0.04 and  0.20. The following limits are obtained at 95% C.L.: (i) on the dimension-6 (LEP like)  couplings, in units of GeV**-2: |a_{{0}}^W/Lambda**2| < 4.3E-6,  |a^W_C/Lambda**2| < 1.6E-5, |a_{{0}}^Z/Lambda**2| < 0.9E-5,  |a^Z_C/Lambda**2| < 4.0E-5. (ii) on the dimension-8 operators, in units of  TeV**-4: |f(M,0)/Lambda**4| < 66.0, |f(M,1)/Lambda**4| <  245.5, |f(M,2)/Lambda**4| < 9.8, |f(M,3)/Lambda**4| <  73.0, |f(M,4)/Lambda**4| < 36.0, |f(M,5)/Lambda**4| <  67.0, |f(M,7)/Lambda**4| < 490.9.


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SIRUNYAN 2021 study electroweak Z-pair production in association with two jets, with the  Z bosons decaying to oppositely-charged electron or muon pairs. Leptons with high transverse  momentum are selected, with the di-lepton invariant mass of the two Z boson candidates between  60 GeV and 120 GeV, and the four-lepton invariant mass larger than 180 GeV. A total of 365 events  are selected in the data, while the number of expected events is 370+-48. Analyzing the  four-lepton invariant mass distribution, the following 95% C.L. limits are derived: -0.24  < f(T,0)/Lambda**4 < 0.22, -0.31 < f(T,1)/Lambda**4 < 0.31,  -0.63 < f(T,2)/Lambda**4 < 0.59, -0.43 < f(T,8)/Lambda**4  < 0.43, -0.92 < f(T,9)/Lambda**4 < 0.92, in units of TeV**-4.


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TUMASYAN 2021A study electroweak Z gamma production in association with two jets, where   the Z boson decays to electron or muon pairs and the pair of two jets has high invariant mass,   superseeding SIRUNYAN 2020AL. The number of observed (expected) electron events in the  barrel  and endcap regions are 375 (349+-9) and 174 (166+-6) events, respectively, while  for muon events  the respective numbers are 584 (612+-13) and 320 (303+-8). Analysing the  Z gamma  invariant mass distribution, the following 95% C.L. limits are derived:  -15.8 <  f(M,0)/Lambda**4 < 16.0, -35.0 < f(M,1)/Lambda**4  < 34.7, -6.55  < f(M,2)/Lambda**4 < 6.49, -13.0 <  f(M,3)/Lambda**4 < 13.0,  -13.0 < f(M,4)/Lambda**4 < 12.7,  -22.2 < f(M,5)/Lambda**4  < 21.3, -56.6 < f(M,7)/Lambda**4  < 55.9, -0.64 <  f(T,0)/Lambda**4 < 0.57, -0.81 <  f(T,1)/Lambda**4 < 0.90, -1.68  < f(T,2)/Lambda**4 < 1.54,  -0.58 < f(T,5)/Lambda**4 < 0.64,  -1.30 < f(T,6)/Lambda**4  < 1.33, -2.15 < f(T,7)/Lambda**4  < 2.43, -0.47 <  f(T,8)/Lambda**4 < 0.47, -0.91 <  f(T,9)/Lambda**4 < 0.91, in units  of TeV**-4.


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TUMASYAN 2021B measure W or Z boson production in association with two photons, using     the leptonic decays modes of W and Z with electrons or muons. The number of selected  W --> e ( mu ) nu    events is 1987 (2384) and the number of selected Z --> e e ( mu mu )  events is 110 (272)    respectively. Analyzing the transverse momentum of the di-photon system, the  following 95 %    C.L.  limits are derived in  units of TeV**-4: In the W production  channel, the observed    limits are: -39.9 <  f(M,2)/Lambda**4 < 39.5,  -63.8 <   f(M,3)/Lambda**4 < 65.0,  -1.30 < f(T,0)/Lambda**4  < 1.30, -1.70    < f(T,1)/Lambda**4  < 1.66, -3.64 <  f(T,2)/Lambda**4 < 3.64,    -0.52 <  f(T,5)/Lambda**4 < 0.60,  -0.60 < f(T,6)/Lambda**4    < 0.68,  -1.16 < f(T,7)/Lambda**4  < 1.16. In the Z production    channel, the    observed limits are: -5.70 <  f(T,0)/Lambda**4 < 5.46, -5.70    <  f(T,1)/Lambda**4 < 5.46,  -11.4 < f(T,2)/Lambda**4 < 10.9,    -2.92 < f(T,5)/Lambda**4  < 2.92, -3.80 < f(T,6)/Lambda**4    < 3.88, -7.88 <  f(T,7)/Lambda**4 < 7.72, -1.06 <    f(T,8)/Lambda**4 < 1.10,  -1.82 < f(T,9)/Lambda**4 < 1.82, in  units  of TeV**-4.


pdgid: S043AQC
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SIRUNAYN 2020 study W Z and same-sign W W production in association with two jets,  using the leptonic decays modes of the W and Z bosons with electrons or muons. Overall, 524  W W events and 229 W Z events are selected, with a Standard Model expectation of 535+-52 and  216+-21 events, respectively. Analyzing the transverse mass spectrum of the di-boson system  and the di-jet invariant mass, the following 95% C.L. limits are derived, not using any  unitarization procedure:  -0.25 < f(T,0)/Lambda**4 < 0.28,  -0.12  < f(T,1)/Lambda**4 < 0.14,  -0.35 < f(T,2)/Lambda**4 <  0.48,  -2.7 < f(M,0)/Lambda**4 < 2.9, -4.1 <  f(M,1)/Lambda**4 < 4.2,  -5.4 < f(M,6)/Lambda**4 < 5.8,  -5.7 < f(M,7)/Lambda**4 < 6.0, -5.7 < f(S,0)/Lambda**4  < 6.1, -16 < f(S,1)/Lambda**4 < 17, in units of TeV**-4. The  article also reports limits on these couplings by cutting the EFT expansion at the unitarity limit.


pdgid: S043AQC
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SIRUNYAN 2020AL study electroweak production of a Z boson and a photon in association  with two jets in the electron and muon decay modes of the Z. A signal with a significance of  3.9 standard deviations is observed, compared to a Standard Model expectation of 5.2 standard  deviations. Combining with KHACHATRYAN 2017AA data at 8 TeV the final observed and expected  signal significance is 4.7 and 5.5 standard deviations. Analyzing the Z-photon invariant mass  distribution, the following 95% C.L. limits are derived: -19.5 <  f(M,0)/Lambda**4 < 20.3, -40.5 < f(M,1)/Lambda**4 < 39.5,  -8.22 < f(M,2)/Lambda**4 < 8.10, -17.7 < f(M,3)/Lambda**4  < 17.9, -15.3 < f(M,4)/Lambda**4 < 15.8, -25.1 <  f(M,5)/Lambda**4 < 24.5, -38.9 < f(M,6)/Lambda**4 < 40.6,  -60.3 < f(M,7)/Lambda**4 < 62.5, -0.74 < f(T,0)/Lambda**4  < 0.69, -0.98 < f(T,1)/Lambda**4 < 0.96, -1.97 <  f(T,2)/Lambda**4 < 1.86, -0.70 < f(T,5)/Lambda**4 < 0.75,  -1.64 < f(T,6)/Lambda**4 < 1.68, -2.59 < f(T,7)/Lambda**4  < 2.82, -0.47 < f(T,8)/Lambda**4 < 0.47, -1.27 <  f(T,9)/Lambda**4 < 1.27, in units of TeV**-4.


pdgid: S043AQC
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SIRUNYAN 2020BD study electroweak W gamma production in association with two jets, where  the W boson decays to electron or muon and the two jets have high invariant mass. The number of  observed (expected) electron events with the photon in the barrel and endcap regions are 393  (397.1+-18.5) and 159 (145.2+-10.0) respectively, while for muon events the respective  numbers are 565 (537.9+-21.4) and 201 (188.2+-10.5). Analyzing the W gamma invariant  mass distribution, the following 95% C.L. limits are derived: -8.1 <  f(M,0)/Lambda**4 < 8.0, -12 < f(M,1)/Lambda**4 < 12, -2.8  < f(M,2)/Lambda**4 < 2.8, -4.4 < f(M,3)/Lambda**4 < 4.4,  -5.0 < f(M,4)/Lambda**4 < 5.0, -8.3 < f(M,5)/Lambda**4 <  8.3, -16 < f(M,6)/Lambda**4 < 16, -21 < f(M,7)/Lambda**4  < 20, -0.6 < f(T,0)/Lambda**4 < 0.6, -0.4 <  f(T,1)/Lambda**4 < 0.4, -1.0 < f(T,2)/Lambda**4 < 1.2, -0.5  < f(T,5)/Lambda**4 < 0.5, -0.4 < f(T,6)/Lambda**4 < 0.4,  -0.9 < f(T,7)/Lambda**4 < 0.9, in units of TeV**-4.


pdgid: S043AQC
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SIRUNYAN 2019BM search for the final state W+ W- W+- using W decays to electrons or  muons. Two event samples are considered, events with three leptons, or events with two oppositely  charged leptons accompanied by two jets. In a kinematic region selected to enhance the effect of  anomalous couplings, no events are selected in the data, and 95% C.L. upper limits are  obtained as follows: -1.2 < f(T,0)/Lambda**4 < 1.2, -3.3 <  f(T,1)/Lambda**4 < 3.3, -2.7 < f(T,2)/Lambda**4 < 2.6, in  units of TeV$^{-4}$ and without application of a form factor.


pdgid: S043AQC
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SIRUNYAN 2019BP study W Z plus 2 jets production, using W and Z decay channels  with electrons or muons. In the data, 75 events are selected, with a fitted SM signal of 15.1+-1.6  events and a fitted background of 62.4+-2.8 events. The transverse mass distribution of the  W Z system is analyzed to set the following limits  at 95% C.L., in units of TeV**-4:   -9.15 < f(M,0)/Lambda**4 < 9.15, -9.15 < f(M,1)/Lambda**4  < 9.45, -26.5 < f(S,0)/Lambda**4 < 27.5,  -41.2 <  f(S,1)/Lambda**4 < 42.8, -0.75 < f(T,0)/Lambda**4 < 0.81, -0.49  < f(T,1)/Lambda**4 < 0.55, -1.49 < f(T,2)/Lambda**4 < 1.85.


pdgid: S043AQC
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SIRUNYAN 2019CQ search for anomalous electroweak production of vector boson pairs in  association with two jets. Events are selected by requiring two jets with a large invariant mass  and rapidity separation, one or two leptons (electrons or muons), and a W or Z boson  decaying hadronically. In the W V (Z V) channel, 347 (47) events are selected in the data,  with a total expected background of 352+-19 (50.3+-5.8) events. Analysing the mass  distribution of the W V or Z V system, the following 95% C.L. limits are obtained:  -2.7< f(S,0)/Lambda**4 < 2.7, -3.4 < f(S,1)/Lambda**4 <  3.4, -0.69 < f(M,0)/Lambda**4 < 0.70, -2.0 < f(M,1)/Lambda**4  < 2.1, -1.3 < f(M,6)/Lambda**4 < 1.3, -3.4 <  f(M,7)/Lambda**4 < 3.4, -0.12 < f(T,0)/Lambda**4 < 0.11, -0.12  < f(T,1)/Lambda**4 < 0.13, -0.28 < f(T,2)/Lambda**4 < 0.28,  in units of TeV**-4.


pdgid: S043AQC
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SIRUNYAN 2018CC  study p p collisions at sqrt(s) = 13 TeV leading to a pair of same-sign  W pairs decaying leptonically (e or mu) associated with a pair of jets. Isolated  leptons with pT > 25 (20) GeV for the leading (trailing) lepton, with |eta|  < 2.5 (2.4) for e (mu) and jets with pT > 30 GeV, |eta| <  5.0, |Deltaeta_{{jj}}()| > 2.5 and m_{{jj}}() > 500 GeV is required.  Further cuts are applied to minimize Z --> e e events, non-prompt leptons and hadronically  decaying taus. The number of selected events is 201, with an expected SM signal of 66.9+-2.4  and background of 138+-13 events. Analysing the dilepton invariant mass spectrum the following  95% C.L. limits are derived: -7.7< f(S,0)/Lambda**4 < 7.7, -21.6  < f(S,1)/Lambda**4 <21.8, -6.0 < f(M,0)/Lambda**4 <  5.9, -8.7 < f(M,1)/Lambda**4 < 9.1,  -11.9 <  f(M,6)/Lambda**4 < 11.8,  -13.3 < f(M,7)/Lambda**4 < 12.9, -0.62 < f(T,0)/Lambda**4 < 0.65,  -0.28 < f(T,1)/Lambda**4  <0.31,  -0.89 < f(T,2)/Lambda**4 <1.02.


pdgid: S043AQC
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AABOUD 2017AA analyze W+- W+- production in association  with two jets and W decay  modes with electrons or muons.  In the  kinematic region of VBS the effect of anomalous QGCs is  enhanced by  requiring the transverse mass of the W W system to be larger than 400 GeV. In the  data, 8 events are selected with a total  background expected from SM processes of 3.8+-0.6  events. Assuming the other QGC coupling to have the SM value of zero, the  observed event yield is  used to determine 95% CL limits on the QGCs: -0.14<alpha_{{4}}()< 0.15 and  -0.22<alpha_{{5}}()< 0.22. Supersedes AAD 2014AM.


pdgid: S043AQC
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AABOUD 2017AG determine the W W gamma and W Z gamma cross sections in 8 TeV p p  interactions by studying the final states e nu mu nu gamma and e nu j j gamma or mu nu j j gamma.  Upper limits on the production cross sections are derived in a fiducial region optimized for BSM  physics. These are used to derive the following 95% C.L. upper limits for quartic couplings  assuming the form scale factor, Lambda(FF) = inf (all in units of E3  TeV**-4): -0.3 < f(M,0)/Lambda**4 < 0.3, -0.5 <  f(M,1)/Lambda**4 < 0.5, -1.8 < f(M,2)/Lambda**4 < 1.8, -1.1  < f(M,4)/Lambda**4 < 1.1, -1.7 < f(M,5)/Lambda**4 < 1.7,  -0.6 < f(M,6)/Lambda**4 < 0.6, -1.1 <  f(M,7)/Lambda**4 < 1.1, -0.1 < f(T,0)/Lambda**4 < 0.1, -0.2  < f(T,1)/Lambda**4 < 0.2, -0.4 < f(T,4)/Lambda**4 < 0.4,  -1.5 < f(T,5)/Lambda**4 < 1.6, -1.9 < f(T,6)/Lambda**4 <  1.9, -4.3 < f(T,7)/Lambda**4 < 4.3.


pdgid: S043AQC
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AABOUD 2017D analyze electroweak diboson (W V, V = W, Z) production in  association with a high-mass dijet system. In the data, 32 events are selected with an expected  total background of 32+-12 events. Analysing the transverse mass distribution of the W V  system, the following limits are set at 95% C.L.: -0.024 < alpha_{{4}} <  0.030 and -0.028 < alpha_{{5}} < 0.033.


pdgid: S043AQC
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AABOUD 2017J analyze the Z gamma production in association with a high-mass dijet system,  with the Z boson decaying into a pair of electrons, muons, or neutrinos. In the charged lepton  (neutrino) channel, events are selected with a dijet mass larger than 500 (600) GeV and a  transverse photon energy larger than 250 (150) GeV, with 2 (4) events selected in the data and  0.30+-0.08 (1.6+-0.5) expected background events. The observed event yield is used to  determine 95% CL limits as follows: -4.1E3 < f(T,9)/Lambda**4 < 4.2E3,  -1.9E3 < f(T,8)/Lambda**4 < 2.1E3, -1.9E1 <  f(T,0)/Lambda**4 < 1.6E1, -1.6E2 < f(M,0)/Lambda**4 < 1.8E2,  -3.5E2 < f(M,1)/Lambda**4 < 3.4E2, -8.9E2 <  f(M,2)/Lambda**4 < 8.9E2, -1.7E3 < f(M,3)/Lambda**4 < 1.7E3, in  units of TeV**-4 and without application of a form factor.


pdgid: S043AQC
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AABOUD 2017M analyze tri-boson W+- W+- W-+ production in decay channels with three  charged leptons or two like-sign charged leptons with two jets, where the lepton can be an electron  or muon. In the data, 24 tri-lepton events and 21 di-lepton plus jets events are selected, compared  to a total event yield expected in the SM of 30.8+-3.0 and 21.9+-2.0, respectively.  Analysing the tri-lepton transverse mass or the transverse momentum sum of the two leptons, two  jets and the missing transverse energy, the following limits at 95% CL are derived for the  form factor cut-off scale Lambda(FF)-->inf: -0.13 <  f(S,0)/Lambda**4 < 0.18, -0.21 < f(S,1)/Lambda**4 < 0.27,  in units of 10**4 TeV**-4, which are converted into the following limits: -0.49 <  alpha_{{4}}() < 0.75 and -0.48 < alpha_{{5}} < 0.62.


pdgid: S043AQC
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KHACHATRYAN 2017AA analyse electroweak production of Z gamma  in association with two  hadronic jets, with the Z boson decaying  to electron or muon pairs. Events with photon  transverse momentum  larger than 60 GeV and di-jet invariant mass larger than 400 GeV are   selected. The Z gamma inavariant mass spectrum is analysed to set  95% C.L. limits as  follows:  -71 < f(M,0)/Lambda**4 < 75,   -190 <  f(M,1)/Lambda**4 < 182,   -32 < f(M,2)/Lambda**4 < 31, -58 < f(M,3)/Lambda**4 < 59,   -3.8 < f(T,0)/Lambda**4  < 3.4,   -4.4 < f(T,1)/Lambda**4 < 4.4,   -9.9 <  f(T,2)/Lambda**4 < 9.0,   -1.8 < f(T,8)/Lambda**4 < 1.8, -4.0 < f(T,9)/Lambda**4 < 4.0,   in units of TeV**-4 and without  application of a form factor.


pdgid: S043AQC
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KHACHATRYAN 2017M analyse electroweak production of W gamma  in association with two  hadronic jets, with the W boson decaying  to electrons or muons. Events with photon transverse  momentum larger  than 200 GeV and di-jet invariant mass larger than 200 GeV are selected.  The W transverse momentum spectrum is analysed to set  95% C.L. limits as follows:  -77  < f(M,0)/Lambda**4 < 74,   -125 < f(M,1)/Lambda**4 <  129,   -26 < f(M,2)/Lambda**4 < 26,   -43 <  f(M,3)/Lambda**4 < 44,   -40 < f(M,4)/Lambda**4 < 40, -65 < f(M,5)/Lambda**4 < 65,   -129 < f(M,6)/Lambda**4  < 129,   -164 < f(M,7)/Lambda**4 < 162,   -5.4 <  f(T,0)/Lambda**4 < 5.6,   -3.7 < f(T,1)/Lambda**4 < 4.0, -11 < f(T,2)/Lambda**4 < 12,   -3.8 < f(T,5)/Lambda**4  < 3.8,   -2.8 < f(T,6)/Lambda**4 < 3.0,   -7.3 <  f(T,7)/Lambda**4 < 7.7,   in units of TeV**-4 and without application of a form  factor.


pdgid: S043AQC
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SIRUNYAN 2017AD study p p collisions at sqrt(s) = 13 TeV to determine the cross section  of Z Z j j with the Z decaying to e e or mu mu. The Z Z mass distribution is  used to set upper limits on the anomalous quartic couplings. The 95% upper limits for the  relevant quartic couplings in units of TeV**-4 are: -0.46 < f(T,0)/Lambda**4  < 0.44, -0.61 < f(T,1)/Lambda**4 < 0.61, -1.2 <  f(T,2)/Lambda**4 < 1.2, -0.84 < f(T,8)/Lambda**4 < 0.84, -1.8  < f(T,9)/Lambda**4 < 1.8.


pdgid: S043AQC
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SIRUNYAN 2017AR study p p collisions at sqrt(s) = 8 TeV to determine the cross section  of p p --> W gamma gamma and p p --> Z gamma gamma where W --> lepton nu and Z --> lepton+ lepton-,  lepton being an electron or a muon. The number of W events in the e and mu channels  is 63 and 108 respectively, and the number of Z events in the e and mu channels is 117  and 141. To increase sensitivity, the transverse momentum of the leading photon is required to be  larger than 70 GeV. The 95% C.L. upper limits in units of TeV**-4 are -701 <  f(M,2)/Lambda**4 < 683, -1170 < f(M,3)/Lambda**4 < 1220, -33.5  < f(T,0)/Lambda**4 < 34.0, -44.3 < f(T,1)/Lambda**4 < 44.8,  -93.8 < f(T,2)/Lambda**4 < 93.2.


pdgid: S043AQC
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AABOUD 2016E study W W production in two-photon mediated p p collisions at 8 TeV where the W boson decays into an electron or muon, probing the gamma gamma W W vertex for anomalous quartic gauge couplings. The lepton pT is required to be larger than 30 GeV. Limits on anomalous couplings are determined from events with pT larger than 120 GeV where the aQGC effect is enhanced and the SM background reduced; in the data corresponding to an integrated luminosity of 20.2fb^{-1}, 1 event is selected with an expected SM background of 0.37+-0.13 events. The 95% C.L. limits without a form-factor cutoff (Lambda(cutoff)-->inf) are as follows: -1.7 < a^W_0()/Lambda**2 < 1.7 and -6.4 < a^W_C/Lambda**2 < 6.3 in units of 10**-6 GeV**-2.  In terms of another set of variables: -6.6 < f(M,0)/Lambda**4 < 6.6 and -24 < f(M,1)/Lambda**4 < 25 in units of 10**-11 GeV**-4.


pdgid: S043AQC
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AAD 2016Q study Z gamma gamma production in p p collisions. In events with no additional jets, 29 (22) Z decays to electron (muon) pairs are selected, with an expected background of 3.3+-1.1 (6.5+-2.0) events, as well as 19 Z decays to netrino pairs with an expected background of 8.3+-4.4 events. Analysing the photon transverse momentum distribution for mass(gamma gamma) above 200 GeV (300 GeV) for lepton (neutrino) events, yields the 95% C.L. limits: -1.6E4 < f(M,2)/Lambda**4 < 1.6E4, -2.9E4 < f(M,3)/Lambda**4 < 2.7E4, -0.86E2 < f(T,0)/Lambda**4 < 1.03E2, -0.69E3 < f(T,5)/Lambda**4 < 0.68E3, -0.74E4 < f(T,9)/Lambda**4 < 0.74E4 in units of TeV**-4 and without application of a form factor Lambda(FF).


pdgid: S043AQC
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KHACHATRYAN 2016AX searches for anomalous W W gamma gamma quartic gauge couplings in the two-photon-mediated process p p --> p p W W, assuming the W W gamma triple gauge boson couplings to be at their Standard Model values. 13 events containing an e+-  mu-+ pair with pT(e, mu) > 30 GeV are selected in a total luminosity of 19.7 fb^{-1}, with an expected gamma gamma --> W W signal of 5.3+-0.1 events and an expected background of 3.9+-0.5 events. When combining with the data collected at 7 TeV (CHATRCHYAN 2013AA), and not assuming a form factor, the following 1-parameter limits at 95% C.L. are obtained from the pT(e, mu) spectrum: |a^W_0()/Lambda**2| < 1.1E-6 GeV**-2 (a^W_C = 0), and |a^W_C/Lambda**2| < 4.1E-6 GeV**-2 (a^W_0() = 0). In terms of another set of variables: |f(M,0)/Lambda**4| < 4.2E-12 GeV**-4, |f(M,1)/Lambda**4| < 16E-12 GeV**-4, |f(M,2)/Lambda**4| < 2.1E-12 GeV**-4,  |f(M,3)/Lambda**4| < 7.8E-12 GeV**-4.


pdgid: S043AQC
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AAD 2015N study W gamma gamma events in 8 TeV p p interactions, where the W  decays into an electron or a muon. The events are characterized by an isolated lepton, a missing  transverse energy due to the decay neutrino, and two isolated photons, with the pT of the  lepton and the photons being > 20 GeV. The number of candidate events observed in the  electron channel for N(jet) >= 0 and N(jet) = 0 is 47 and 15, the corresponding numbers for  the muon channel being 110 and 53. The backgrounds expected are 30.2+-7.4, 8.7+-3.0,  52.1+-12.2, and 24.4+-8.3 respectively. The 95% C.L. limits on the values of the  parameters f(T,0)/Lambda^4(), f(M,2)/Lambda^4() and  f(M,3)/Lambda^4() are -0.9 -- 0.9E2, -0.8 -- 0.8E4, and -1.5 -- 1.4E4  respectively, without application of a form factor Lambda(FF).


pdgid: S043AQC
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KHACHATRYAN 2015D study vector-boson-scattering tagged by two jets, requiring two same-sign   charged leptons arising from W+- W+- production and decay. The two jets must have a   transverse momentum larger than 30 GeV, while the leptons, electrons or muons, must have a   transverse momentum > 20 GeV. The dijet mass is required to be > 500 GeV, the dilepton   mass > 50 GeV, with additional requirement of differing from the Z mass by > 15   GeV. In the two categories W+ W+ and W- W-, 10 and 2 data events are observed in a data   sample corresponding to an integrated luminosity of 19.4 fb**-1, with an expected background of   3.1+-0.6 and 2.6+-0.5 events. Analysing the distribution of the dilepton invariant mass,   the following limits at 95% C.L. are obtained, in units of TeV**-4: -38 < F(S,0)/Lambda**4 < 40, -118 < F(S,1)/Lambda**4   < 120, -33 <  F(M,0)/Lambda**4 < 32, -44 < F(M,1)/Lambda**4 < 47, -65 <  F(M,6)/Lambda**4   < 63, -70 <  F(M,7)/Lambda**4 < 66, -4.2 <   F(T,0)/Lambda**4 < 4.6, -1.9 < F(T,1)/Lambda**4   < 2.2, -5.2 < F(T,2)/Lambda**4 < 6.4.


pdgid: S043AQC
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AAD 2014AM analyze electroweak production of W W jet jet same-charge diboson plus two jets production, with the W bosons decaying to electron or muon, to study the quartic W W W W coupling. In a kinematic region enhancing the electroweak production over the strong production, 34 events are observed in the data while 29.8+-2.4 events are expected with a backgound of 15.9+-1.9 events. Assuming the other QGC coupling to have the SM value of zero, the observed event yield is used to determine 95% CL limits on the quartic gauge couplings: -0.14<alpha_{{4}}()< 0.16 and -0.23<alpha_{{5}}()< 0.24.


pdgid: S043AQC
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CHATRCHYAN 2014Q study W V gamma production in 8 TeV p p collisions, in the single lepton final state, with W --> lepton nu, Z --> dijet or W --> lepton nu, W --> dijet, the dijet mass resolution precluding differentiation between the W and Z. pT and pseudo-rapidity cuts are put on the lepton, the photon and the two jets to minimize backgrounds. The dijet mass is required to be between 70 -- 100 GeV and |Deltaeta_{{jj}}()| < 1.4. The selected number of muon (electron) events are 183 (139), with SM expectation being 194.2+-11.5 (147.9+-10.7) including signal and background. The photon E(T) distribution is used to set limits on the anomalous quartic couplings. The following 95% CL limits are deduced (all in units of TeV**-2 or TeV**-4): -21 <a_{{0}}^W()/Lambda^2()< 20, -34 <a_{{c}}^W()/Lambda^2()< 32, -12 <kappa_{{0}}^W()/Lambda^2()< 10 and -18 <kappa_{{c}}^W()/Lambda^2()< 17; and -25 <f(T,0)/Lambda^4()< 24 TeV**-4.


pdgid: S043AQC
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ABAZOV 2013D searches for anomalous W W gamma gamma quartic gauge couplings in the   two-photon-mediated process p p --> p p W W, assuming the W W gamma triple gauge boson couplings to be at their Standard Model values. 946 events containing an e+ e- pair with missing energy are selected in a total luminosity of 9.7 fb**-1, with an expectation of 983+-108 events from Standard-Model processes. The following 1-parameter limits at 95% CL are otained:   |a_{{0}}^W/Lambda**2| < 4.3E-4 GeV**-2 (a_{{c}}^W = 0), |a_{{c}}^W/Lambda**2| < 1.5E-3 GeV**-2 (a_{{0}}^W = 0).


pdgid: S043AQC
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CHATRCHYAN 2013AA searches for anomalous W W gamma gamma quartic gauge couplings in the two-photon-mediated process p p --> p p W W, assuming the W W gamma triple gauge boson couplings to be at their Standard Model values. 2 events containing an e+- mu-+ pair with pT(e, mu) > 30 GeV are selected in a total luminosity of 5.05 fb**-1, with an expected p p W W signal of 2.2+-0.4 events and an expected background of 0.84+-0.15 events. The following 1-parameter limits at 95% CL are otained from the pT(e, mu) spectrum: |a_{{0}}^W/Lambda**2| < 4.0E-6 GeV**-2 (a_{{c}}^W = 0), |a_{{c}}^W/Lambda**2| < 1.5E-5 GeV**-2 (a_{{0}}^W = 0).


pdgid: S043AQC
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ABBIENDI 2004B select 187 e+ e- --> W+ W- gamma events in the C.M. energy range 180 -- 209 GeV, where E(gamma)>2.5 GeV, the photon has a polar angle |cos(theta(gamma)) |< 0.975 and is well isolated from the nearest jet and charged lepton, and the effective masses of both fermion-antifermion systems agree with the W mass within 3 Gamma(W). The measured differential cross section as a function of the photon energy and photon polar angle is used to extract the 95% CL limits: -0.020 GeV**-2<a(0)/Lambda**2<0.020 GeV**-2, -0.053~GeV**-2<a(c)/Lambda**2<0.037 GeV**-2 and -0.16 GeV**-2<a(n)/Lambda**2<0.15 GeV**-2.


pdgid: S043AQC
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ABBIENDI 2004L select 20 e+ e- --> nu nubar gamma gamma  acoplanar events in the energy range 180 -- 209 GeV and 176 e+ e- --> q qbar gamma gamma events in the energy range 130 -- 209 GeV. These samples are used to constrain possible anomalous W+ W- gamma gamma and Z Z  gamma  gamma quartic couplings. Further combining with the W+ W- gamma sample of ABBIENDI 2004B  the following one--parameter 95% CL limits are obtained: -0.007 <a_{{0}}^Z/Lambda**2< 0.023 GeV**-2, -0.029 <a_{{c}}^Z/Lambda**2< 0.029 GeV**-2, -0.020 <a_{{0}}^W/Lambda**2< 0.020 GeV**-2, -0.052 <a_{{c}}^W/Lambda**2< 0.037 GeV**-2.


pdgid: S043AQC
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In the CM energy range 183 to 209 GeV HEISTER 2004A select 30 e+ e- --> nu nubar gamma gamma events with two acoplanar, high energy and high transverse momentum photons. The photon-photon acoplanarity is required to be > 5degree, E(gamma)/sqrt(s) > 0.025 (the more energetic photon having energy > 0.2 sqrt(s)), p(T(gamma))/E(beam)  > 0.05 and |cos( theta(gamma))| < 0.94. A likelihood fit to the photon energy and recoil missing mass yields the following one--parameter 95% CL limits: -0.012 < a_{{0}}^Z/Lambda**2 < 0.019 GeV**-2, -0.041 < a_{{c}}^Z/Lambda**2 < 0.044 GeV**-2, -0.060 < a_{{0}}^W/Lambda**2 < 0.055 GeV**-2, -0.099 < a_{{c}}^W/Lambda**2 < 0.093 GeV**-2.


pdgid: S043AQC
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ABDALLAH 2003I select 122 e+ e- --> W+ W- gamma events in the C.M. energy range 189 -- 209 GeV, where E(gamma)>5 GeV, the photon has a polar angle |cos(theta(gamma))|<0.95 and is well isolated from the nearest charged fermion. A fit to the photon energy spectra yields a(c)/Lambda**2= 0.000+0.019-0.040 GeV**-2, a(0)/Lambda**2= -0.004+0.018-0.010 GeV**-2, atilde(0)/Lambda**2= -0.007+0.019-0.008 GeV**-2, a(n)/Lambda**2= -0.09+0.16-0.05 GeV**-2, and atilde(n)/Lambda**2= +0.05+0.07-0.15 GeV**-2, keeping the other parameters fixed to their Standard Model values(0). The 95% CL limits are: -0.063 GeV**-2<a(c)/Lambda**2<+0.032 GeV**-2, -0.020 GeV**-2<a(0)/Lambda**2<+0.020 GeV**-2, -0.020 GeV**-2<atilde(0)/Lambda**2<+0.020 GeV**-2, -0.18 GeV**-2<a(n)/Lambda**2<+0.14 GeV**-2, -0.16 GeV**-2<atilde(n)/Lambda**2<+0.17 GeV**-2.


pdgid: S043AQC
text:
ACHARD 2002F select 86 e+ e- --> W+ W- gamma events at 192 -- 207 GeV, where E(gamma)>5 GeV and the photon is well isolated.  They also select 43 acoplanar e+ e- --> nu nubar gamma gamma events in this energy range, where the photon energies are >5GeV and >1GeV and the photon polar angles are between 14degrees and 166degrees. All these 43 events are in the recoil mass region corresponding to the Z (75 -- 110 GeV). Using the shape and normalization of the photon spectra in the W+ W- gamma events, and combining with the 42 event sample from 189 GeV data (ACCIARRI 2000T), they obtain: a(0)/Lambda**2= 0.000+-0.010 GeV**-2, a(c)/Lambda**2= -0.013+-0.023 GeV**-2, and a(n)/Lambda**2= -0.002+-0.076 GeV**-2. Further combining the analyses of W+ W- gamma events with the low recoil mass region of  nu nubar gamma gamma events (including samples collected at 183+189 GeV), they obtain the following one-parameter 95% CL limits: -0.015 GeV**-2<a(0)/Lambda**2<0.015 GeV**-2, -0.048 GeV**-2<a(c)/Lambda**2<0.026 GeV**-2, and -0.14 GeV**-2<a(n)/Lambda**2<0.13 GeV**-2.


pdgid: S044M
text:
AALTONEN 2022 analyse Z decays in the di-muon and di-electron channels using their full  Run-II data set. They obtain Z mass values of 91192.0+-6.4(stat.)+-4.0(syst.) MeV and  91194.3+-13.8(stat.)+-7.6(syst.) MeV, respectively. Combining these results using the  systematic uncertainty contributions and their correlations as given in AALTONEN 2022, we  obtain an average of 91192.3+-5.8(stat.)+-4.1(syst.) MeV.


pdgid: S044M
text:
This result combines ABBIENDI 2001A, ABREU 2000F, ACCIARRI 2000C, BARATE 2000C,  taking correlated uncertainties into account.


pdgid: S044M
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ABBIENDI 2004G obtain this result using the S-matrix formalism for a combined fit to their cross section and asymmetry data at the Z peak and their data at 130 -- 209 GeV. The authors have corrected the measurement for the 34 MeV shift with respect to the Breit-Wigner fits.


pdgid: S044M
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ACHARD 2004C select e+ e- --> Z gamma events with hard initial-state radiation. Z decays to q qbar and muon pairs are considered. The fit results obtained in the two samples are found consistent to each other and combined considering the uncertainty due to ISR modelling as fully correlated.


pdgid: S044M
text:
ABBIENDI 2001A error includes approximately 2.3 MeV due to statistics and 1.8 MeV due to LEP  energy uncertainty. This result is included in the LEP average LEP-SLC 2006.


pdgid: S044M
text:
The error includes 1.6 MeV due to LEP energy uncertainty. This result is included in the LEP  average LEP-SLC 2006.


pdgid: S044M
text:
The error includes 1.8 MeV due to LEP energy uncertainty. This result is included in the LEP  average LEP-SLC 2006.


pdgid: S044M
text:
ACCIARRI 2000Q interpret the s-dependence of the cross sections and lepton forward-backward asymmetries in the framework of the S-matrix formalism.  They fit to their cross section and asymmetry data at high energies, using the results of S-matrix fits to Z-peak data (ACCIARRI 2000C) as constraints.  The 130 -- 189 GeV data constrains the gamma/Z interference term.  The authors have corrected the measurement for the 34.1 MeV shift with respect to the Breit-Wigner fits. The error contains a contribution of +-2.3 MeV due to the uncertainty on the gamma Z interference.


pdgid: S044M
text:
BARATE 2000C error includes approximately 2.4 MeV due to statistics, 0.2MeV due to  experimental systematics, and 1.7MeV due to LEP energy uncertainty. This result is  included in the LEP average LEP-SLC 2006.


pdgid: S044M
text:
MIYABAYASHI 1995 combine their low energy total hadronic cross-section measurement with the ACTON 1993D data and perform a fit using an S-matrix formalism.  As expected, this result is below the mass values obtained with the standard Breit-Wigner parametrization.


pdgid: S044M
text:
Enters fit through W/Z mass ratio given in the W Particle Listings. The ALITTI 1992B systematic error (+-0.93) has two contributions: one (+-0.92) cancels in mass(W)/mass(Z) and one (+-0.12) is noncancelling.  These were added in quadrature.


pdgid: S044M
text:
First error of ABE 1989 is combination of statistical and systematic contributions; second is mass scale uncertainty.


pdgid: S044W
text:
JANOT 2020 applies a correction to LEP-SLC 2006 using an  updated Bhabha cross section  calculation. This result also includes a  correction to account for correlated luminosity bias as  presented in  VOUTSINAS 2020.


pdgid: S044W
text:
ABBIENDI 2004G obtain this result using the S-matrix formalism for a combined fit to their cross section and asymmetry data at the Z peak and their data at 130 -- 209 GeV. The authors have corrected the measurement for the 1 MeV shift with respect to the Breit-Wigner fits.


pdgid: S044W
text:
ABBIENDI 2001A error includes approximately 3.6 MeV due to statistics, 1MeV due to event selection systematics, and 1.3 MeV due to LEP energy uncertainty.


pdgid: S044W
text:
ACCIARRI 2000Q interpret the s-dependence of the cross sections and lepton forward-backward asymmetries in the framework of the S-matrix formalism.  They fit to their cross section and asymmetry data at high energies, using the results of S-matrix fits to Z-peak data (ACCIARRI 2000C) as constraints.  The 130 -- 189 GeV data constrains the gamma/Z interference term.  The authors have corrected the measurement for the 0.9 MeV shift with respect to the Breit-Wigner fits.


pdgid: S044W
text:
BARATE 2000C error includes approximately 3.8 MeV due to statistics, 0.9MeV due to experimental systematics, and 1.3MeV due to LEP energy uncertainty.


pdgid: S044W
text:
ABREU 1996R obtain this value from a study of the interference between initial and final state radiation in the process e+ e- --> Z --> mu+ mu-.


pdgid: S044W
text:
Quoted values of ANSARI 1987 are from direct fit. Ratio of Z and W production gives either Gamma(Z) < (1.09+-0.07) * Gamma(W), CL = 90% or Gamma(Z) = (0.82+0.19-0.14+-0.06) * Gamma(W). Assuming Standard-Model value Gamma(W) = 2.65 GeV then gives Gamma(Z) < 2.89+-0.19 or = 2.17+0.50-0.37+-0.16.


pdgid: S044W1
text:
ABE 1995J obtain this measurement from Bhabha events in a restricted fiducial region to improve systematics. They use the values 91.187 and 2.489 GeV for the Z mass and total decay width to extract this partial width.


pdgid: S044W6
text:
AAD 2024L use the measured ratio of invisible Z decays and leptonic Z decays to  derive the width of the Z decaying to invisible particles. Events with transverse momentum of  the Z larger than 130 GeV and at least one central jet with transverse momentum larger than 110  GeV are selected.


pdgid: S044W6
text:
TUMASYAN 2023E analyses leptonic Z decay modes, with the invisible Z decay identified  by missing momentum.


pdgid: S044W6
text:
The LEP Collaborations perform a combined fit to their line-shape results and determine this  quantity as a difference between the total width and the sum of all the visible widths, assuming  lepton universality. This result combines ABBIENDI 2001A, ABREU 2000F, ACCIARRI 2000C,  BARATE 2000C, taking correlated uncertainties into account.


pdgid: S044W6
text:
This is an indirect determination of Gamma(invisible) from a fit to the visible Zdecay modes. It is included in the determination of the LEP average  LEP-SLC 2006 reported above.


pdgid: S044R3
text:
AABOUD 2017Q make a precise determination of Z --> e e and Z --> mu mu production in  the lepton pseudo-rapidity range |eta| < 2.5 and determine the ratio of the Z  branching fractions B(Z --> e e)/B(Z --> mu mu) = 1.0026+-0.0013+-0.0048 =  1.0026+-0.0050.


pdgid: S044R3
text:
This parameter is not directly used in the overall fit but is derived using the fit results; see  the note ``The Z boson'' and ref. LEP-SLC 2006.


pdgid: S044R19
text:
AAIJ 2018AR obtain the result from the ratio of the measured p p --> Z + X cross sections  in the corresponding Z decay channels.


pdgid: S044R01
text:
AAD 2021AQ analyze differential cross-sections in four-lepton events. Based on the measured  cross section in the  channel, a branching fraction of B() =  4.41+-0.13+-0.23+-0.09+-0.12E-6 is obtained, where the uncertainties are statistical,  systematic, theory and luminosity, respectively.


pdgid: S044R01
text:
AABOUD 2019N reports 4.70+-0.32+-0.21+-0.14E-6, where the uncertainties are  statistical, systematic, and  luminosity. We have combined the latter two in quadrature.


pdgid: S044R01
text:
SIRUNYAN 2018BT report the  branching fraction = 4.83+0.23-0.22+0.32-0.29+-0.08+-0.12E-6, where  the uncertainties are statistical, systematic, due to theory, and luminosity. The last three have  been added in quadrature to obtain the total systematic error.


pdgid: S044R01
text:
KHACHATRYAN 2016CC reports 4.9+0.8-0.7+0.3-0.2+0.2-0.1+0.1-0.1E-6 value, where the  uncertainties are statistical, systematic, theory, and due to luminosity. We have combined  uncertainties in quadrature.


pdgid: S044R01
text:
CHATRCHYAN 2012BN reports 4.2+0.9-0.8+-0.2E-6 value. Their result (both central value and uncertainties) is scaled up by 10% to account for the different phase-space definition used here (see RAINBOLT 2019).


pdgid: S044R11
text:
ABBIENDI 2001A error includes approximately 0.067 due to statistics, 0.040 due to event selection systematics, 0.027 due to the theoretical uncertainty in t-channel prediction, and 0.014 due to LEP energy uncertainty.


pdgid: S044R11
text:
BARATE 2000C error includes approximately 0.062 due to statistics, 0.033 due to experimental systematics, and 0.026 due to the theoretical uncertainty in t-channel prediction.


pdgid: S044R9
text:
ABBIENDI 2001A error includes approximately 0.050 due to statistics and 0.027 due to event selection systematics.


pdgid: S044R9
text:
BARATE 2000C error includes approximately 0.053  due to statistics and 0.021 due to experimental systematics.


pdgid: S044R12
text:
ABBIENDI 2001A error includes approximately 0.055 due to statistics and 0.071 due to event selection systematics.


pdgid: S044R12
text:
BARATE 2000C error includes approximately 0.054 due to statistics and 0.033 due to experimental systematics.


pdgid: S044R20
text:
ABBIENDI 2001A error includes approximately 0.034 due to statistics and 0.027 due to event selection systematics.


pdgid: S044R20
text:
BARATE 2000C error includes approximately 0.033 due to statistics, 0.020 due to experimental systematics, and 0.005 due to the theoretical uncertainty in t-channel prediction.


pdgid: S044R21
text:
ABBIENDI 2004E select photons with energy > 7 GeV and use Gamma(hadrons) = 1744.4+-2.0 MeV and alpha_{{s}} = 0.1172+-0.002 to obtain Gamma(u) = 300+19-18 MeV.


pdgid: S044R21
text:
ACKERSTAFF 1997T measure Gamma(u ubar)/(Gamma(d dbar)+Gamma(u ubar)+Gamma(s sbar)) = 0.258+-0.031+-0.032. To obtain this branching ratio authors use R(c)+R(b) = 0.380+-0.010. This measurement is fully negatively correlated with the measurement of Gamma(d dbar,s sbar)/(Gamma(d dbar)+Gamma(u ubar)+Gamma(s sbar)) given in the next data block.


pdgid: S044R21
text:
ABREU 1995X use M(Z) = 91.187+-0.009 GeV, Gamma(hadrons) = 1725+-12 MeV and alpha(s) = 0.123+-0.005.  To obtain this branching ratio we divide their value of C(2/3) = 0.91+0.25-0.36 by their value of (3C(1/3) + 2C(2/3)) = 6.66+-0.05.


pdgid: S044R21
text:
ADRIANI 1993 use M(Z) = 91.181+-0.022 GeV, Gamma(hadrons) = 1742+-19 MeV and alpha(s) = 0.125+-0.009.  To obtain this branching ratio we divide their value of C(2/3) = 0.92+-0.22 by their value of (3C(1/3) + 2C(2/3)) = 6.720+-0.076.


pdgid: S044R22
text:
ABBIENDI 2004E select photons with energy > 7 GeV and use Gamma(hadrons) = 1744.4+-2.0 MeV and alpha_{{s}} = 0.1172+-0.002 to obtain Gamma(d) = 381+-12 MeV.


pdgid: S044R22
text:
ACKERSTAFF 1997T measure Gamma(d dbar,s sbar)/(Gamma(d dbar)+Gamma(u ubar)+Gamma(s sbar)) = 0.371+-0.016+-0.016. To obtain this branching ratio authors use R(c)+R(b) = 0.380+-0.010. This measurement is fully negatively correlated with the measurement of Gamma(u ubar)/(Gamma(d dbar)+Gamma(u ubar)+Gamma(s sbar)) presented in the previous data block.


pdgid: S044R22
text:
ABREU 1995X use M(Z) = 91.187+-0.009 GeV, Gamma(hadrons) = 1725+-12 MeV and alpha(s) = 0.123+-0.005.  To obtain this branching ratio we divide their value of C(1/3) = 1.62+0.24-0.17 by their value of (3C(1/3) + 2C(2/3)) = 6.66+-0.05.


pdgid: S044R22
text:
ADRIANI 1993 use M(Z) = 91.181+-0.022 GeV, Gamma(hadrons) = 1742+-19 MeV and alpha(s) = 0.125+-0.009.  To obtain this branching ratio we divide their value of C(1/3) = 1.63+-0.15 by their value of (3C(1/3) + 2C(2/3)) = 6.720+-0.076.


pdgid: S044R29
text:
ABE 2005F use hadronic Z decays collected during 1996--98 to obtain an enriched sample of c cbar events using a double tag method. The single c--tag is obtained with a neural network trained to perform flavor discrimination using as input several signatures (corrected secondary vertex mass, vertex decay length, multiplicity and total momentum of the hemisphere). A multitag approach is used, defining 4 regions of the output value of the neural network and R(c) is extracted from a simultaneous fit to the count rates of the 4 different tags. The quoted systematic error includes an uncertainty of +-0.0006 due to the uncertainty on R(b).


pdgid: S044R29
text:
ABREU 2000 obtain this result properly combining the measurement from the D^*()+ production rate (R(c)= 0.1610+-0.0104+-0.0077+-0.0043 (BR)) with that from the overall charm counting (R(c)= 0.1692+-0.0047+-0.0063+-0.0074 (BR)) in c cbar events.  The systematic error includes an uncertainty of +-0.0054 due to the uncertainty on the charmed hadron branching fractions.


pdgid: S044R29
text:
BARATE 2000B use exclusive decay modes to independently determine the quantities R(c)*f(c --> X), X=D0, D+, D_{{s}}()+, and Lambda_{{c}}.  Estimating R(c)*f(c --> Xi_cslashOmega_c)= 0.0034, they simply sum over all the charm decays to obtain R(c)= 0.1738+-0.0047+-0.0088+-0.0075(BR).  This is combined with all previous ALEPH measurements (BARATE 1998T and BUSKULIC 1994G, R(c)= 0.1681+-0.0054+-0.0062) to obtain the quoted value.


pdgid: S044R29
text:
ACKERSTAFF 1998E use an inclusive/exclusive double tag.  In one jet D^*()+- mesons are exclusively reconstructed in several decay channels and in the opposite jet a slow pion (opposite charge inclusive D^*()+-) tag is used.  The b content of this sample is measured by the simultaneous detection of a lepton in one jet and an inclusively reconstructed D^*()+-meson in the opposite jet.  The systematic error includes an uncertainty of +-0.006 due to the external branching ratios.


pdgid: S044R29
text:
ALEXANDER 1996R obtain this value via direct charm counting, summing the partial contributions from D0, D+, D_{{s}}()+, and Lambda_{{c}}()+, and assuming that strange-charmed baryons account for the 15% of the Lambda_{{c}}()+ production. An uncertainty of +-0.005 due to the uncertainties in the charm hadron branching ratios is included in the overall systematics.


pdgid: S044R29
text:
ABREU 1995D perform a maximum likelihood fit to the combined p and pT distributions of single and dilepton samples.  The second error includes an uncertainty of +-0.0124 due to models and branching ratios.


pdgid: S044R18
text:
ABE 2005F use hadronic Z decays collected during 1996--98 to obtain an enriched sample of b bbar events using a double tag method. The single b--tag is obtained with a neural network trained to perform flavor discrimination using as input several signatures (corrected secondary vertex mass, vertex decay length, multiplicity and total momentum of the hemisphere; the key tag is obtained requiring the secondary vertex corrected mass to be above the D--meson mass). ABE 2005F obtain R(b) =0.21604+-0.00098+-0.00074 where the systematic error includes an uncertainty of +-0.00012 due to the uncertainty on R(c). The value reported here is obtained properly combining with ABE 1998D. The quoted systematic error includes an uncertainty of +-0.00012 due to the uncertainty on~R(c).


pdgid: S044R18
text:
ACCIARRI 2000 obtain this result using a double-tagging technique, with a high pT lepton tag and an impact parameter tag in opposite hemispheres.


pdgid: S044R18
text:
ABBIENDI 1999B tag Z --> b bbar decays using leptons and/or separated decay vertices.  The b-tagging efficiency is measured directly from the data using a double-tagging technique.


pdgid: S044R18
text:
ABREU 1999B obtain this result combining in a multivariate analysis several tagging methods (impact parameter and secondary vertex reconstruction, complemented by event shape variables).  For R(c) different from its Standard Model value of 0.172, R(b) varies as -0.024*(R(c)-0.172).


pdgid: S044R18
text:
BARATE 1997F combine the lifetime-mass hemisphere tag (BARATE 1997E) with event shape information and lepton tag to identify Z --> b bbar candidates.  They further use c- and u d s-selection tags    to identify the background.  For R(c) different from its Standard Model value of 0.172, R(b) varies as -0.019x(R(c)-0.172).


pdgid: S044R18
text:
ABREU 1995D perform a maximum likelihood fit to the combined p and pT distributions of single and dilepton samples.  The second error includes an uncertainty of +-0.0023 due to models and branching ratios.


pdgid: S044R18
text:
BUSKULIC 1994G perform a simultaneous fit to the p and pT spectra of both single and dilepton events.


pdgid: S044R18
text:
JACOBSEN 1991 tagged b bbar events by requiring coincidence of >=3 tracks with significant impact parameters using vertex detector. Systematic error includes lifetime and decay uncertainties (+-0.014).


pdgid: S044B4
text:
ABBIENDI 2001G use a sample of four-jet events from hadronic Zdecays.  To enhance the b bbar b bbar signal, at least three of the four jets are required to have a significantly detached secondary vertex.


pdgid: S044B4
text:
ABREU 1999U force hadronic Zdecays into 3jets to use all the available phase space and require a btag for every jet.  This decay mode includes primary and secondary 4b production, e.g, from gluon splitting to b bbar.


pdgid: S044R63
text:
This branching ratio is slightly dependent on the jet-finder algorithm. The value we quote is obtained using the JADE algorithm, while using the DURHAM algorithm ABREU 1996S obtain an upper limit of 1.5E-2.


pdgid: S044R13
text:
This limit is for both decay modes Z --> pi0 gamma/gamma gamma which are indistinguishable in ACCIARRI 1995G.


pdgid: S044R00
text:
AABOUD 2018AU search for the Z --> rho gamma decay mode where the rho is identified  through its decay rho --> pi+ pi-. In the data corresponding to 32.3 fb**-1, 12,583 events  are selected for 635 < m(pi+ pi-) < 915 MeV.  See erratum AABOUD 2023A.


pdgid: S044R04
text:
AABOUD 2018AU search for the Z --> phi gamma decay mode where the phi is identified  through its decay phi --> K+ K-. In the data corresponding to 32.3 fb**-1, 3,364 events are  selected for 1012 < m(K+ K-) < 1028 MeV.  See erratum AABOUD 2023A.


pdgid: S044R04
text:
AABOUD 2016K search for the Z --> phi gamma decay mode where the phi is identified  through its decay into K+ K-. In the data corresponding to a total luminosity of 2.7  fb^{-1}, 1065 events are selected and their K+ K- gamma invariant mass spectrum is analyzed.


pdgid: S044R23
text:
ACCIARRI 1999F combine mu+ mu- and e+ e- J/psi(1S) decay channels.  The branching ratio for prompt J/psi(1S) production is measured to be (2.1+-0.6+-0.4(-0.2)**+0.4(theor.))*10**-4.


pdgid: S044R23
text:
ALEXANDER 1996B identify J/psi(1S) from the decays into lepton pairs. (4.8+-2.4)% of this branching ratio is due to prompt J/psi(1S) production (ALEXANDER 1996N).


pdgid: S044R23
text:
Combining mu+ mu- and e+ e- channels and taking into account the common systematic errors. (7.7+6.3-5.4)% of this branching ratio is due to prompt J/psi(1S) production.


pdgid: S044R03
text:
SIRUNYAN 2019AJ study  Z --> J/psi gamma with J/psi --> mu+  mu-. Candidate events  are selected by requiring a pair of oppositely charged muons and a well isolated photon. The  leading (subleading) muon is require to have a transverse momentum larger than 20 GeV (4 GeV),  while the photon must have a transverse energy larger than 33 GeV. Requiring the invariant mass of  the mu mu (mu mu gamma) system in the range 3.0 to 3.2 (81 to 101) GeV, selects 183 data  events which is consistent with the expected background. The 95% C.L. limit on the Z  branching fraction is obtained assuming the J/psi to be unpolarized.


pdgid: S044R03
text:
AABOUD 2018BL study Z --> J/psi gamma in 13 TeV p p interactions. Two triggers were  used: isolated photon of pT > 35(25) GeV and a muon with pT > 18(24) GeV.  The J/psi is detected via its dimuon decay and it is required that the azimuthal angle between  the photon and the J/psi in the plane transverse to the beam direction is > pi/2.  The number of observed/expected background events is 92/89+-6 in the dimuon mass range  2.9 -- 3.3 GeV leading to the quoted 95% C.L. limit.


pdgid: S044R03
text:
AAD 2015I use events with the highest pT muon in the pair required to have pT  > 20 GeV, the dimuon mass required to be within 0.2 GeV of the J/psi(1S) mass and it's  transverse momentum required to be > 36 GeV. The photon is also required to have it's  pT > 36 GeV.


pdgid: S044R60
text:
ACCIARRI 1997J measure this branching ratio via the decay channel psi(2S) --> lepton+ lepton- (lepton = mu, e).


pdgid: S044R60
text:
ALEXANDER 1996B measure this branching ratio via the decay channel psi(2S) --> J/psi pi+ pi-, with J/psi --> lepton+ lepton-.


pdgid: S044R60
text:
ABREU 1994P measure this branching ratio via decay channel psi(2S) --> J/psi pi+ pi-, with J/psi --> mu+ mu-.


pdgid: S044R05
text:
AABOUD 2018BL study Z --> psi(2S) gamma in 13 TeV p p interactions. Two triggers were  used: isolated photon of pT > 35(25) GeV and a muon with pT > 18(24) GeV.  The psi(2S) is detected via its dimuon decay and it is required that the azimuthal angle  between the photon and the psi(2S) in the plane transverse to the beam direction is >  pi/2. The number of observed/expected background events is 43/42+-5 in the dimuon  mass range 3.5 -- 3.9 GeV leading to the quoted 95% C.L. limit.


pdgid: S044R09
text:
SIRUNYAN 2018DZ observe the decay Z --> Psi lepton+ lepton- in p p collisions at  sqrt(s) = 13 TeV, where Psi includes J/psi as well as psi(2S) --> J/psi X, and  lepton+ lepton- represents an electron or muon pair while the J/psi is detected via its  mu+ mu- decay channel. To reduce systematic errors they determine the ratio of the branching  fraction of this decay to that of Z --> mu+ mu- mu+ mu- within phase-space cuts imposed on  lepton transverse momentum and pseudo rapidity, dilepton invariant mass, and J/psi transverse  momentum. The number of selected Psi mu+ mu- (Psi e+ e-) candidate events is 29 (18).  Analyzing the mu+ mu- and mu+ mu- lepton+ lepton- invariant mass distributions, a yield of  13.0+-3.9 (11.2+-3.4) events for the Psi mu+ mu- (Psi e+ e-) mode is obtained.  The ratio of the branching fractions is determined as 0.67+-0.18+-0.05 within the selected  phase-space cuts. Assuming extrapolation to full phase space cancels in the ratio, and using their  measured value of B(Z --> mu+ mu- mu+ mu-) = 1.20+-0.08E-6, they estimate B(Z --> J/psi lepton+ lepton-) = 8E-7.


pdgid: S044R38
text:
SIRUNYAN 2019BR search for Z decays to a pair of J/psi mesons in the channel J/psi --> mu+ mu-. The  invariant masses of the higher/lower-pT J/psi candidates have to be within 0.1/0.15 GeV  of the nominal J/psi mass. A total of 189 events are selected in the 40 -- 140 GeV  4-muon invariant mass range. An un-binned extended maximum likelihood fit leads to the 95%  C.L. upper limit, obtained assuming the J/psi mesons to be unpolarised.


pdgid: S044R42
text:
ACCIARRI 1997J measure this branching ratio via the decay channel chi_c1() --> J/psi + gamma, with J/psi --> lepton+ lepton- (lepton = mu, e). The M(lepton+ lepton- gamma)-M(lepton+ lepton-) mass difference spectrum is fitted with two gaussian shapes for chi_{{c1}}() and chi_{{c2}}().


pdgid: S044R42
text:
This branching ratio is measured via the decay channel chi_c1() --> J/psi + gamma, with J/psi --> mu+ mu-.


pdgid: S044R65
text:
ACCIARRI 1997J derive this limit via the decay channel chi_c2() --> J/psi + gamma, with J/psi --> lepton+ lepton- (lepton = mu, e). The M(lepton+ lepton- gamma)-M(lepton+ lepton-) mass difference spectrum is fitted with two gaussian shapes for chi_{{c1}}() and chi_{{c2}}().


pdgid: S044R62
text:
ALEXANDER 1996F identify the Upsilon (which refers to any of the three lowest bound states) through its decay into e+ e- and mu+ mu-. The systematic error includes an uncertainty of +-0.2 due to the production mechanism.


pdgid: S044R06
text:
AABOUD 2018BL study Z --> Upsilon(1S) gamma in 13 TeV p p interactions. Two triggers  were used: isolated photon of pT > 35(25) GeV and a muon with pT > 18(24)  GeV. The Upsilon(1S) is detected via its dimuon decay and it is required that the azimuthal  angle between the photon and the Upsilon(1S) in the plane transverse to the beam direction is  > pi/2. The number of observed/expected background events is 115/126+-8 in  the dimuon mass range 9.0 -- 10.0 GeV leading to the quoted 95% C.L. limit.


pdgid: S044R06
text:
AAD 2015I use events with the highest pT muon in the pair required to have pT  > 20 GeV, the dimuon mass required to be in the range 8 -- 12 GeV and it's transverse  momentum required to be > 36 GeV. The photon is also required to have it's pT >  36 GeV.


pdgid: S044R07
text:
AABOUD 2018BL study Z --> Upsilon(2S) gamma in 13 TeV p p interactions. Two triggers  were used: isolated photon of pT > 35(25) GeV and a muon with pT > 18(24)  GeV. The Upsilon(2S) is detected via its dimuon decay and it is required that the azimuthal  angle between the photon and the Upsilon(2S) in the plane transverse to the beam direction is  > pi/2. The number of observed/expected background events is 106/121+-8 in  the dimuon mass range 9.5 -- 10.5 GeV leading to the quoted 95% C.L. limit.


pdgid: S044R08
text:
AABOUD 2018BL study Z --> Upsilon(3S) gamma in 13 TeV p p interactions. Two triggers  were used: isolated photon of pT > 35(25) GeV and a muon with pT > 18(24)  GeV. The Upsilon(3S) is detected via its dimuon decay and it is required that the azimuthal  angle between the photon and the Upsilon(3S) in the plane transverse to the beam direction is  > pi/2. The number of observed/expected background events is 112/113+-8 in  the dimuon mass range 10.0 -- 11.0 GeV leading to the quoted 95% C.L. limit.


pdgid: S044R39
text:
SIRUNYAN 2019BR search for Z decays to a pair of Upsilon mesons in the channel  Upsilon --> mu+ mu-. The invariant mass of the Upsilon candidates has to be in the range of  8.5 to 11 GeV. A total of 106 events are selected in the 20 -- 140 GeV 4-muon invariant mass  range. An un-binned extended maximum likelihood fit leads to the 95% C.L. upper limit,  obtained assuming the Upsilon mesons to be unpolarised.


pdgid: S044R73
text:
AAD 2024R identify the K(S)0 via its decay to pi+ pi-. The transverse momentum of the  photon is required to be larger than 25 GeV or 35 GeV for different periods of data taking.


pdgid: S044R72
text:
AAD 2024R identify the D0 via its decay to K- pi+. The transverse momentum of the  photon is required to be larger than 25 GeV or 35 GeV for different periods of data taking.


pdgid: S044R64
text:
AAIJ 2023AM also quotes the branching fraction limit B(Z --> D0 gamma) < 2.1E-3, using  the known Z --> mu mu branching fraction.


pdgid: S044R43
text:
The (D0/Dbar0) states in ABREU 1993I are detected by the K pi decay mode. This is a corrected result (see the erratum of ABREU 1993I).


pdgid: S044R44
text:
The D()+- states in ABREU 1993I are detected by the K pi pi decay mode. This is a corrected result (see the erratum of ABREU 1993I).


pdgid: S044R24
text:
D^*(2010)+- in ABREU 1993I are reconstructed from D0 pi+-, with D0 --> K- pi+. The new CLEO II measurement of B(D^*()+- --> D0 pi+-) = (68.1+-1.6) % is used. This is a corrected result (see the erratum of ABREU 1993I).


pdgid: S044R24
text:
DECAMP 1991J report B(D^*(2010)+ --> D0 pi+) B(D0 --> K- pi+) Gamma(D^*(2010)+- X) / Gamma(hadrons) = 5.11+-0.34E-3.  They obtained the above number assuming B(D0 --> K- pi+) = (3.62+-0.34+-0.44)% and B(D^*(2010)+ --> D0 pi+) = (55+-4)%.


pdgid: S044R70
text:
HEISTER 2002B reconstruct this meson in the decay modes D_s1(2536)+- --> D^*()+- K0 and D_s1(2536)+- --> D^*()0 K+-. The quoted branching ratio assumes that the decay width of the  is saturated by the two measured decay modes.


pdgid: S044R71
text:
HEISTER 2002B reconstruct this meson in the decay mode D_s2^*(2573)+- --> D0 K+-. The quoted branching ratio assumes that the detected decay mode represents 45% of the full decay width.


pdgid: S044R69
text:
ABBIENDI 2001N searched for the decay mode D^*'(2629)+- --> D^*()+- pi+ pi- with D^*()+ --> D0 pi+, and D0 --> K- pi+.  They quote a 95% CL limit for Z --> D^*'(2629)+-xB(D^*'(2629)+ --> D^*()+ pi+ pi-) <3.1E-3.


pdgid: S044R61
text:
ACKERSTAFF 1997M use an inclusive B reconstruction method and assume a (13.2+-4.1)% b-baryon contribution.  The value refers to a b-flavored meson mixture of B_{{u}}, B_{{d}}, and B_{{s}}.


pdgid: S044R61
text:
BUSKULIC 1996D use an inclusive reconstruction of B hadrons and assume a (12.2+-4.3)% b-baryon contribution.  The value refers to a b-flavored mixture of B_{{u}}, B_{{d}}, and B_{{s}}.


pdgid: S044R61
text:
ABREU 1995R use an inclusive B-reconstruction method and assume a (10+-4)% b-baryon contribution.  The value refers to a b-flavored meson mixture of B_{{u}}, B_{{d}}, and B_{{s}}.


pdgid: S044R61
text:
ACCIARRI 1995B assume a 9.4% b-baryon contribution.  The value refers to a b-flavored mixture of B_{{u}}, B_{{d}}, and B_{{s}}.


pdgid: S044B+X
text:
ABDALLAH 2003K measure the production fraction of B+ mesons in hadronic Z decays f(B+) = (40.99+-0.82+-1.11)%. The value quoted here is obtained multiplying this production fraction by our value of R(b) = Gamma(bbar b)/Gamma(hadrons).


pdgid: S044R49
text:
ABREU 1992M reported value is Gamma(B_s()0 X)*B(B_s()0 --> D_s mu nu_mu X) *B(D_s --> phi pi)/Gamma(hadrons) = 18+-8E-5.


pdgid: S044R49
text:
ACTON 1992N find evidence for B_{{s}}()0 production using D_{{s}}-lepton correlations, with D_s()+ --> phi pi+ and K^*(892) K+. Assuming R(b) from the Standard Model and averaging over the e and mu channels, authors measure the product branching fraction to be f(bbar --> B_s()0)xB(B_s()0 --> D_s()- lepton+ nu_lepton X)xB(D_s()- --> phi pi-) = 3.9+-1.1+-0.8E-4.


pdgid: S044R49
text:
BUSKULIC 1992E find evidence for B_{{s}}()0 production using D_{{s}}-lepton correlations, with D_s()+ --> phi pi+ and K^*(892) K+. Using B(D_s()+ --> phi pi+) = (2.7+-0.7)% and summing up the e and mu channels, the weighted average product branching fraction is measured to be B(bbar --> B_s()0)xB(B_s()0 --> D_s()- lepton+ nu_lepton X) = 0.040+-0.011+0.010-0.012.


pdgid: S044BCC
text:
ACKERSTAFF 1998O searched for the decay modes B_c --> J/psi pi+, J/psi a_1()+, and J/psi lepton+ nu_lepton, with J/psi --> lepton+ lepton-, lepton = e,mu.  The number of candidates (background) for the three decay modes is 2(0.63+-0.2), 0(1.10+-0.22), and 1(0.82+-0.19) respectively. Interpreting the 2B_c --> J/psi pi+ candidates as signal, they report Gamma(B_c()+ X)*B(B_c --> J/psi pi+)/Gamma(hadrons) =3.8+5.0-2.4+-0.5E-5.  Interpreted as background, the 90% CL bounds are Gamma(B_c()+ X)*B(B_c --> J/psi pi+)/Gamma(hadrons) <1.06E-4, Gamma(B_c()+ X)*B(B_c --> J/psi a_1()+)/Gamma(hadrons) <5.29E-4, Gamma(B_c()+ X)*B(B_c --> J/psi lepton+ nu_lepton)/Gamma(hadrons) <6.96E-5.


pdgid: S044BCC
text:
ABREU 1997E searched for the decay modes B_c --> J/psi pi+,  J/psi lepton+ nu_lepton, and J/psi (3pi)^+, with J/psi --> lepton+ lepton-, lepton = e,mu.  The number of candidates (background) for the three decay modes is 1(1.7), 0(0.3), and 1(2.3) respectively. They report the following 90% CL limits: Gamma(B_c()+ X)*B(B_c --> J/psi pi+)/Gamma(hadrons) <(1.05 -- 0.84)*10**-4, Gamma(B_c()+ X)*B(B_c --> J/psi lepton nu_lepton)/Gamma(hadrons) <(5.8 -- 5.0)*10**-5, Gamma(B_c()+ X)*B(B_c --> J/psi (3pi)^+)/Gamma(hadrons) <1.75E-4, where the ranges are due to the predicted B_{{c}} lifetime (0.4 -- 1.4)ps.


pdgid: S044BCC
text:
BARATE 1997H searched for the decay modes B_c --> J/psi pi+ and  J/psi lepton+ nu_lepton with J/psi --> lepton+ lepton-, lepton = e,mu.  The number of candidates (background) for the two decay modes is 0(0.44) and 2(0.81) respectively. They report the following 90% CL limits: Gamma(B_c()+ X)*B(B_c --> J/psi pi+)/Gamma(hadrons) <3.6E-5 and Gamma(B_c()+ X)*B(B_c --> J/psi lepton+ nu_lepton)/Gamma(hadrons) <5.2E-5.


pdgid: S044LCX
text:
ALEXANDER 1996R measure R(b) x f(b --> Lambda_c()+ X) x B(Lambda_c()+ --> p K- pi+) = (0.122+-0.023+-0.010)% in hadronic Z decays;  the value quoted here is obtained using our best value B(Lambda_c()+ --> p K- pi+) = (5.0+-1.3)%. The first error is the total experiment's error and the second error is  the systematic error due to the branching fraction uncertainty.


pdgid: S044LCX
text:
BUSKULIC 1996Y obtain the production fraction of Lambda_{{c}}()+ baryons in hadronic Z decays f(b --> Lambda_c()+ X) = 0.110+-0.014+-0.006 using B(Lambda_c()+ --> p K- pi+) = (4.4+-0.6)%; we have rescaled using our best value B(Lambda_c()+ --> p K- pi+) = (5.0+-1.3)% obtaining f(b --> Lambda_c()+ X) = 0.097+-0.013+-0.025 where the first error is their total experiment's error and the second error is the systematic error due to the branching fraction uncertainty.  The value quoted here is obtained multiplying this production fraction by our value of R(b) = Gamma(b bbar)/Gamma(hadrons).


pdgid: S044XIC
text:
ABDALLAH 2005C searched for the charmed strange baryon Xi_{{c}}()0 in the decay channel Xi_c()0 --> Xi- pi+ (Xi- --> Lambda pi-). The production rate is measured to be f(Xi_{{c}}()0) x B(Xi_c()0 --> Xi- pi+) = 4.7+-1.4+-1.1E-4 per hadronic Z decay.


pdgid: S044XIB
text:
ABDALLAH 2005C searched for the beauty strange baryon Xi_{{b}} in the inclusive semileptonic decay channel Xi_b --> Xi- lepton- nubar_lepton X. Evidence for the Xi_{{b}} production is seen from the observation of Xi()-+ production accompanied by a lepton of the same sign. From the excess of ``right-sign'' pairs Xi()-+ lepton()-+ compared to ``wrong-sign'' pairs Xi()-+ lepton()+- the production rate is measured to be B(b --> Xi_b) x B(Xi_b --> Xi- lepton- X)  = 3.0+-1.0+-0.3E-4 per lepton species, averaged over electrons and muons.


pdgid: S044XIB
text:
BUSKULIC 1996T investigate Xi-lepton correlations and find a significant excess of ``right--sign'' pairs Xi()-+ lepton()-+ compared to ``wrong--sign'' pairs Xi()-+ lepton()+-. This excess is interpreted as evidence for Xi_{{b}} semileptonic decay. The measured product branching ratio is B(b --> Xi_b) x B(Xi_b --> X_c X lepton- nubar_lepton) x B(X_c --> Xi- X^') = 5.4+-1.1+-0.8E-4 per lepton species, averaged over electrons and muons, with X_{{c}} a charmed baryon.


pdgid: S044XIB
text:
ABREU 1995V observe an excess of ``right-sign'' pairs Xi()-+ lepton()-+ compared to ``wrong-sign'' pairs Xi()-+ lepton()+- in jets: this excess is interpreted as evidence for the beauty strange baryon Xi_{{b}} production, with  Xi_b --> Xi- lepton- nubar_lepton X. They find that the probability for this signal to come from non b-baryon decays is less than 5E-4 and that Lambda_{{b}} decays can account for less than 10% of these events. The Xi_{{b}} production rate is then measured to be B(b --> Xi_b) x B(Xi_b --> Xi- lepton- X) = 5.9+-2.1+-1.0E-4 per lepton species, averaged over electrons and muons.


pdgid: S044BBR
text:
BARATE 1998V use the overall number of identified protons in b-hadron decays to measure  f(b --> b-baryon) = 0.102+-0.007+-0.027. They assume BR(b-baryonp X) =  (58+-6)% and BR(B_s()0 --> p X) = (8.0+-4.0)%. The value quoted here  is obtained multiplying this production fraction by our value of  R(b) = Gamma(b bbar)/Gamma(hadrons).


pdgid: S044R31
text:
AKRAWY 1990J report Gamma(gamma X) < 8.2 MeV at 95%CL.  They assume a three-body gamma q qbar distribution and use E(gamma)>10 GeV.


pdgid: S044PE
text:
ABBIENDI 1999I give the 95%CL limit on the partial width Gamma(Z0 --> p e)<4.6 KeV and we have transformed it into a branching ratio.


pdgid: S044PMU
text:
ABBIENDI 1999I give the 95%CL limit on the partial width Gamma(Z0 --> p mu)<4.4 KeV and we have transformed it into a branching ratio.


pdgid: S044RHC
text:
BEDDALL 2009 analyse 3.2 million hadronic Z decays as archived by ALEPH collaboration and report a value of 2.59+-0.03+-0.15+-0.04. The first error is statistical, the second systematic, and the third arises from extrapolation to full phase space. We combine the systematic errors in quadrature.


pdgid: S044ETP
text:
ACCIARRI 1997D obtain this value averaging over the two decay channels eta^' --> pi+ pi- eta and eta^' --> rho0 gamma.


pdgid: S044DSC
text:
ACKERSTAFF 1998E systematic error includes an uncertainty of +-0.0069 due to the branching ratios B(D^*()+ --> D0 pi+) = 0.683+-0.014 and B(D0 --> K- pi+) = 0.0383+-0.0012.


pdgid: S044DS1
text:
ACKERSTAFF 1997W obtain this value for x>0.6 and with the assumption that its decay width is saturated by the D^* K final states.


pdgid: S044SIC
text:
We have combined the values of <N(Sigma+)> and <N(Sigma-)> from ALEXANDER 1997E adding the statistical and systematic errors of the two final states separately in quadrature.  If isospin symmetry is assumed this value becomes 0.174+-0.010+-0.015.


pdgid: S044DBR
text:
SCHAEL 2006A obtain this anti-deuteron production rate per hadronic Z decay in the anti-deuteron momentum range from 0.62 to 1.03 GeV/c.


pdgid: S044SH
text:
ABBIENDI 2001A error includes approximately 0.031 due to statistics, 0.033 due to event selection systematics, 0.029 due to uncertainty in luminosity measurement, and 0.011 due to LEP energy uncertainty.


pdgid: S044SH
text:
BARATE 2000C error includes approximately 0.030  due to statistics, 0.026 due to experimental systematics, and 0.025 due to uncertainty in luminosity measurement.


pdgid: S044GEV
text:
ACOSTA 2005M determine the forward--backward asymmetry of e+ e- pairs produced via q qbar --> Z/gamma^* --> e+ e- in 15 M(e+ e-) effective mass bins ranging from 40~GeV to~600 GeV.  These results are used to obtain the vector and axial--vector couplings of the Z to e+ e-, assuming the quark couplings are as predicted by the standard model. Higher order radiative corrections have not been taken into account.


pdgid: S044GEV
text:
ABBIENDI 2001O use their measurement of the tau polarization in addition to the lineshape and forward-backward lepton asymmetries.


pdgid: S044GEV
text:
ACCIARRI 2000C use their measurement of the taupolarization in addition to forward-backward lepton asymmetries.


pdgid: S044GEV
text:
ABE 1995J obtain this result combining polarized Bhabha results with the A(LR) measurement of ABE 1994C.  The Bhabha results alone give -0.0507+-0.0096+-0.0020.


pdgid: S044GMV
text:
ABBIENDI 2001K obtain this from an angular analysis of the muon pair asymmetry which takes into account effects of initial state radiation on an event by event basis and of initial-final state interference.


pdgid: S044GUV
text:
ABAZOV 2011D study p pbar --> Z/gamma^* e+ e- events using 5 fb**-1 data at sqrt(s) = 1.96 TeV. The candidate  events are selected by requiring two isolated electromagnetic showers with E(T)> 25 GeV, at least one electron  in the central region and the di-electron mass in the range 50 -- 1000 GeV. From the forward-backward asymmetry, determined  as a function of the di-electron mass, they derive the axial and vector couplings of the u- and d- quarks and the value  of sin**2(theta)(eff)**lepton = 0.2309+-0.0008(stat)+-0.0006(syst).


pdgid: S044GUV
text:
LEP-SLC 2006 is a combination of the results from LEP and SLC experiments using light quark tagging.  s- and d-quark couplings are assumed to be identical.


pdgid: S044GUV
text:
ACOSTA 2005M determine the forward-backward asymmetry of e+ e- pairs produced via q qbar --> Z / gamma^*() --> e+ e- in 15 M(e+ e-) effective mass bins ranging from 40 GeV to 600 GeV. These results are used to obtain the vector and axial-vector couplings of the Z to the light quarks, assuming the electron couplings are as predicted by the Standard Model. Higher order radiative corrections have not been taken into account.


pdgid: S044GUV
text:
ABRAMOWICZ 2016A determine the Z0 couplings to u- and d-quarks using the ZEUS  polarised data from Run II together with the unpolarised data from both ZEUS and H1 Collaborations  for Run I and unpolarised H1 data from Run II.


pdgid: S044GUV
text:
ABT 2016 determine the Z0 couplings to u- and d-quarks using the same techniques  and data as ABRAMOWICZ 2016A but additionally use the published H1 polarised data.


pdgid: S044GUV
text:
AKTAS 2006 fit the neutral current (1.5<=Q**2<=30,000 GeV**2) and charged current (1.5<=Q**2<=15,000 GeV**2) differential cross sections. In the determination of the u-quark couplings the electron and d-quark couplings are fixed to their standard model values.


pdgid: S044GDV
text:
AKTAS 2006 fit the neutral current (1.5<=Q**2<=30,000 GeV**2) and charged current (1.5<=Q**2<=15,000 GeV**2) differential cross sections. In the determination of the d-quark couplings the electron and u-quark couplings are fixed to their standard model values.


pdgid: S044GEA
text:
ABE 1995J obtain this result combining polarized Bhabha results with the A(LR) measurement of ABE 1994C.  The Bhabha results alone give -0.4968+-0.0039+-0.0027.


pdgid: S044GNE
text:
VILAIN 1994 derive this value from their value of g**nu_{{mu}} and their ratio g**nu_{{e}}/g**nu_{{mu}} = 1.05+0.15-0.18.


pdgid: S044GNM
text:
VILAIN 1994 derive this value from their measurement of the couplings g(A)**e nu_mu = -0.503+-0.017 and g(V)**e nu_mu = -0.035+-0.017 obtained from nu_mu e scattering. We have re-evaluated this value using the current PDG values for g(A)**e and g(V)**e.


pdgid: S044AE
text:
ABBIENDI 2001O fit for A(e) and A(tau) from measurements of the taupolarization at varying tauproduction angles.  The correlation between A(e) and A(tau) is less than 0.03.


pdgid: S044AE
text:
ABE 2001B use the left-right production and left-right forward-backward decay asymmetries in leptonic Z decays to obtain a value of 0.1544+-0.0060. This is combined with left-right production asymmetry measurement using hadronic Z decays (ABE 2000B) to obtain the quoted value.


pdgid: S044AE
text:
HEISTER 2001 obtain this result fitting the tau polarization as a function of the polar production angle of the tau.


pdgid: S044AE
text:
ABREU 2000E obtain this result fitting the taupolarization as a function of the polar tauproduction angle.  This measurement is a combination of different analyses (exclusive taudecay modes, inclusive hadronic 1-prong reconstruction, and a neural network analysis).


pdgid: S044AE
text:
ABE 1997 obtain this result from a measurement of the observed left-right charge asymmetry, A(Q)**obs = 0.225+-0.056+-0.019, in hadronic Zdecays. If they combine this value of A(Q)**obs with their earlier measurement of A(LR)**obs they determine A(e) to be 0.1574+-0.0197+-0.0067 independent of the beam polarization.


pdgid: S044AM
text:
ABE 2001B obtain this direct measurement using the left-right production and left-right forward-backward polar angle asymmetries in mu+ mu- decays of the Z boson obtained with a polarized electron beam.


pdgid: S044AM
text:
AAD 2015BT study p p --> Z --> lepton+ lepton- events where lepton is an electron or  a muon in the dilepton mass region 70 -- 1000 GeV. The background in the Z peak region  is estimated to be < 1% for the muon channel. The muon asymmetry parameter is derived  from the measured forward-backward asymmetry assuming the value of the quark asymmetry parameter  from the SM. For this reason it is not used in the average.


pdgid: S044AT
text:
ABE 2001B obtain this direct measurement using the left-right production and left-right forward-backward polar angle asymmetries in tau+ tau- decays of the Z boson obtained with a polarized electron beam.


pdgid: S044AS
text:
ABE 2000D tag Z --> s sbar events by an absence of B or D hadrons and the presence in each hemisphere of a high momentum K+- or K(S)0.


pdgid: S044AC
text:
ABE 2005 use hadronic Z decays collected during 1996 -- 98 to obtain an enriched sample of c cbar events tagging on the invariant mass of reconstructed secondary decay vertices. The charge of the underlying c-quark is obtained with an algorithm that takes into account the net charge of the vertex as well as the charge of tracks emanating from the vertex and identified as kaons. This yields (9970 events) A_{{c}} = 0.6747+-0.0290+-0.0233. Taking into account all correlations with earlier results reported in ABE 2002G and ABE 2001C, they obtain the quoted overall SLD result.


pdgid: S044AC
text:
ABE 2002g tag b and c quarks through their semileptonic decays into electrons and muons. A maximum likelihood fit is performed to extract simultaneously A(b) and A(c).


pdgid: S044AC
text:
ABE 2001C tag Z --> c cbar events using two techniques: exclusive reconstruction of D^*()+, D+ and D0 mesons and the soft pion tag for D^*()+ --> D0 pi+. The large background from D mesons produced in b bbar events is separated efficiently from the signal using precision vertex information.  When combining the A(c) values from these two samples, care is taken to avoid double counting of events common to the two samples, and common systematic errors are properly taken into account.


pdgid: S044AB
text:
ABE 2005 use hadronic Z decays collected during 1996 -- 98 to obtain an enriched sample of b bbar events tagging on the invariant mass of reconstructed secondary decay vertices. The charge of the underlying b-quark is obtained with an algorithm that takes into account the net charge of the vertex as well as the charge of tracks emanating from the vertex and identified as kaons. This yields (25917 events) A_{{b}} = 0.9173+-0.0184+-0.0173. Taking into account all correlations with earlier results reported in ABE 2003F, ABE 2002G and ABE 1999L, they obtain the quoted overall SLD result.


pdgid: S044AB
text:
ABE 2003F obtain an enriched sample of b bbar events tagging on the invariant mass of a 3-dimensional topologically reconstructed secondary decay.  The charge of the underlying bquark is obtained using a self-calibrating track-charge method.  For the 1996--1998 data sample they measure A(b) = 0.906+-0.022+-0.023. The value quoted here is obtained combining the above with the result of ABE 1998I (1993--1995 data sample).


pdgid: S044AB
text:
ABE 2002G tag b and c quarks through their semileptonic decays into electrons and muons. A maximum likelihood fit is performed to extract simultaneously A(b) and A(c).


pdgid: S044AB
text:
ABE 1999L obtain an enriched sample of b bbar events tagging with an inclusive vertex mass cut. For distinguishing b and bbar quarks they use the charge of identified K+-.


pdgid: S044CTN
text:
BARATE 1997D combine their value of C(TN) with the world average P(tau) = -0.140+-0.007 to obtain tan(Phi(g(V)**tau)-Phi(g(A)**tau)) = -0.57+-0.97.


pdgid: S044Z01
text:
ABBIENDI 2001A error includes approximately 0.38 due to statistics, 0.16 due to event selection systematics, and 0.18 due to the theoretical uncertainty in t-channel prediction.


pdgid: S044Z01
text:
BARATE 2000C error includes approximately 0.31  due to statistics, 0.06 due to experimental systematics, and 0.13 due to the theoretical uncertainty in t-channel prediction.


pdgid: S044Z0A
text:
ABREU 1995M perform this measurement using radiative muon-pair events associated with high-energy isolated photons.


pdgid: S044Z0T
text:
ABBIENDI 2001A error includes approximately 0.26 due to statistics and 0.14 due to event selection systematics.


pdgid: S044Z0T
text:
BARATE 2000C error includes approximately 0.26 due to statistics and 0.11 due to experimental systematics.


pdgid: S044Z0L
text:
ABBIENDI 2001A error includes approximately 0.15 due to statistics, 0.06 due to event selection systematics, and 0.03 due to the theoretical uncertainty in t-channel prediction.


pdgid: S044Z0L
text:
BARATE 2000C error includes approximately 0.15  due to statistics, 0.04 due to experimental systematics, and 0.02 due to the theoretical uncertainty in t-channel prediction.


pdgid: S044Z0U
text:
ACKERSTAFF 1997T measure the forward-backward asymmetry of various fast hadrons made of light quarks. Then using SU(2) isospin symmetry and flavor independence for down and strange quarks authors solve for the different quark types.


pdgid: S044Z0S
text:
ABREU 2000B tag the presence of an squark requiring a high-momentum-identified charged kaon.  The s-quark pole asymmetry is extracted from the charged-kaon asymmetry taking the expected d- and u-quark asymmetries from the Standard Model and using the measured values for the c- and b-quark asymmetries.


pdgid: S044Z0S
text:
ACKERSTAFF 1997T measure the forward-backward asymmetry of various fast hadrons made of light quarks. Then using SU(2) isospin symmetry and flavor independence for down and strange quarks authors solve for the different quark types.  The value reported here corresponds then to the forward-backward asymmetry for ``down-type'' quarks.


pdgid: S044Z0C
text:
ABDALLAH 2004F tag b- and c-quarks using semileptonic decays combined with charge flow information from the hemisphere opposite to the lepton. Enriched samples of c cbar and b bbar  events are obtained using lifetime information.


pdgid: S044Z0C
text:
ABBIENDI 2003P tag heavy flavors using events with one or two identified leptons. This allows the simultaneous fitting of the b and cquark forward-backward asymmetries as well as the average B0-Bbar0 mixing.


pdgid: S044Z0C
text:
HEISTER 2002H measure simultaneously b and c quark forward-backward asymmetries using their semileptonic decays to tag the quark charge.  The flavor separation is obtained with a discriminating multivariate analysis.


pdgid: S044Z0C
text:
ABREU 1999Y tag Z --> b bbar and Z --> c cbar events by an exclusive reconstruction of several D meson decay modes (D^*()+, D0, and D+ with their charge-conjugate states).


pdgid: S044Z0C
text:
BARATE 1998O tag Z --> c cbar events requiring the presence of high-momentum reconstructed D^*()+, D+, or D0 mesons.


pdgid: S044Z0B
text:
ABDALLAH 2005 obtain an enriched samples of  b bbar events  using lifetime information. The quark (or antiquark) charge is determined with a neural network using the secondary vertex charge, the jet charge and particle identification.


pdgid: S044Z0B
text:
ABBIENDI 2002I tag Z0 --> b bbar decays using a combination of secondary vertex and lepton tags.  The sign of the b-quark charge is determined using an inclusive tag based on jet, vertex, and kaon charges.


pdgid: S044Z0B
text:
HEISTER 2001D tag Z --> b bbar events using the impact parameters of charged tracks complemented with information from displaced vertices, event shape variables, and lepton identification. The b-quark direction and charge is determined using the hemisphere charge method along with information from fast kaon tagging and charge estimators of primary and secondary vertices.  The change in the quoted value due to variation of A(FB)**c and R(b) is given as +0.103 (A(FB)**c - 0.0651) -0.440 (R(b) - 0.21585).


pdgid: S044Z0B
text:
ACCIARRI 1999D tag Z --> b bbar events using high p and p(T) leptons.  The analysis determines simultaneously a mixing parameter chi(b) = 0.1192+-0.0068+-0.0051 which is used to correct the observed asymmetry.


pdgid: S044Z0B
text:
ACCIARRI 1998U tag Z --> b bbar events using lifetime and measure the jet charge using the hemisphere charge.


pdgid: S044Z0Q
text:
ACTON 1992L use the weight function method on 259k selected Z --> hadrons events. The systematic error includes a contribution of 0.2 due to B0-Bbar0 mixing effect, 0.4 due to Monte Carlo (MC) fragmentation uncertainties and 0.3 due to MC statistics. ACTON 1992L derive a value of to be 0.2321+-0.0017+-0.0028.


pdgid: S044SEF
text:
AAIJ 2024AL analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to muon pairs.


pdgid: S044SEF
text:
AALTONEN 2018B is a combination of the the results from the Tevatron experiments CDF and D0  in the electron and muon channels, AALTONEN 2014C, AALTONEN 2016D, ABAZOV 2015C,  ABAZOV 2018, averaging the combined value from CDF and from D0 as also provided by the  experiments in AALTONEN 2016D and ABAZOV 2018, respectively. The average of the two  results takes correlations into account and has a chi^2 probability of 2.6%.


pdgid: S044SEF
text:
SIRUNYAN 2018CY analyse the forward-backward asymmetry in Drell-Yan production of Z  bosons decaying to muon or electron pairs.


pdgid: S044SEF
text:
AAD 2015BT analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to muon or electron pairs.


pdgid: S044SEF
text:
AAIJ 2015BF analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to muon pairs.


pdgid: S044SEF
text:
This result combines the six individual results from LEP and SLC. The average, described in  LEP-SLC 2006, has a chi^2 probability of 3.7%.


pdgid: S044SEF
text:
ABAZOV 2018 analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to muon pairs. Combining this result with the one from ABAZOV 2015C, a value of  0.23095+-0.00040 is obtained.


pdgid: S044SEF
text:
AALTONEN 2016D analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to electron pairs. Combining this result with the one from AALTONEN 2014C, a value  of 0.23221+-0.00046 is obtained.


pdgid: S044SEF
text:
ABAZOV 2015C analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to electron pairs.


pdgid: S044SEF
text:
AALTONEN 2014C analyse the forward-backward asymmetry in Drell-Yan production of Z bosons  decaying to muon pairs.


pdgid: S044SEF
text:
The result is based on the forward-backward asymmetry measured in leptonic Z decays (electrons,  muons, taus). It combines the results of the LEP experiments, ALEPH, DELPHI, L3 and OPAL, taking  correlations into account, see LEP-SLC 2006.


pdgid: S044SEF
text:
The result is based on the polarisation of tau leptons measured in Z decays to tau-lepton  pairs. It combines the results of the LEP experiments, ALEPH, DELPHI, L3 and OPAL, taking  correlations into account, see LEP-SLC 2006.


pdgid: S044SEF
text:
The result is based on the left-right and forward-backward left-right asymmetry measured in  leptonic Z decays (electrons, muons, taus). It combines the results of the SLC experiment, SLD,  taking correlations into account, see LEP-SLC 2006.


pdgid: S044SEF
text:
The result is based on the forward-backward asymmetry measured at LEP and the forward-backward  left-right asymmetry measured at SLC, in both cases using Z decays to b-quarks. It  combines the results of the LEP and SLC experiments, ALEPH, DELPHI, L3, OPAL and SLD, taking  correlations into account, see LEP-SLC 2006.


pdgid: S044SEF
text:
The result is based on the forward-backward asymmetry measured at LEP and the forward-backward  left-right asymmetry measured at SLC, in both cases using Z decays to c-quarks. It  combines the results of the LEP and SLC experiments ALEPH, DELPHI, L3, OPAL and SLD, taking  correlations into account, see LEP-SLC 2006.


pdgid: S044SEF
text:
The result is based on the inclusive hadronic charge asymmetry measured in hadronic Z decays.  It combines the results of the LEP experiments, ALEPH, DELPHI, L3 and OPAL, taking correlations  into account, see LEP-SLC 2006.


pdgid: S044ZVG
text:
AAD 2016Q study Z gamma production in p p collisions. In events with no additional  jets, 10268 (12738) Z decays to electron (muon) pairs are selected, with an expected background  of 1291+-340 (1537+-408) events, as well as 1039 Z decays to neutrino pairs with an  expected background of 450+-96 events. Analyzing the photon transverse momentum distribution  above 250 GeV (400 GeV) for lepton (neutrino) events, yields the 95% C.L. limits: -7.8E-4<h_{{3}}^Z<8.6E-4,  -3.0E-6<h_{{4}}^Z<2.9E-6, -9.5E-4<h(3)**gamma<9.9E-4,  -3.2E-6<h(4)**gamma<3.2E-6.


pdgid: S044ZVG
text:
KHACHATRYAN 2016AE determine the Z gamma --> nu nubar gamma cross section by selecting  events with a photon of E(T) > 145 GeV and notET > 140 GeV. 630 candidate  events are observed with an expected SM background of 269+-26. The E(T) spectrum of the  photon is used to set 95% C.L. limits as follows:  -1.5E-3<h_{{3}}^Z<1.6E-3,  -3.9E-6<h_{{4}}^Z<4.5E-6, -1.1E-3<h(3)**gamma<0.9E-3,  -3.8E-6<h(4)**gamma<4.3E-6.


pdgid: S044ZVG
text:
KHACHATRYAN 2015AC study Z gamma events in 8 TeV p p interactions, where the Z   decays into 2 same-flavor, opposite sign leptons (e or mu) and a photon with pT   > 15 GeV. The pT of a lepton is required to be > 20 GeV/c, their effective mass   > 50 GeV, and the photon should have a separation DeltaR > 0.7 with each   lepton. The observed pT distribution of the photons is used to extract the 95% C.L.   limits: -3.8E-3 < h(3)**Z < 3.7E-3, -3.1E-5 <   h(4)**Z < 3.0E-5, -4.6E-3 <   h(3)**gamma < 4.6E-3, -3.6E-5 <   h(4)**gamma < 3.5E-5.


pdgid: S044ZVG
text:
CHATRCHYAN 2014AB measure Z gamma production cross section for p(T)**gamma > 15 GeV and R(lepton gamma) > 0.7, which is the separation between the gamma and the final state charged lepton (e or mu) in the azimuthal angle-pseudorapidity (phi-eta) plane.  The di-lepton mass is required to be > 50 GeV. After background subtraction the number of e e gamma and mu mu gamma events is determined to be 3160+-120 and 5030+-233 respectively, compatible with expectations from the SM. This leads to a 95% CL limits of -1E-2 < h(3)**gamma < 1E-2, -9E-5 < h(4)**gamma < 9E-5, -9E-3 < h_{{3}}^Z() < 9E-3, -8E-5 < h_{{4}}^Z() < 8E-5, assuming h_{{1}}^V() and h_{{2}}^V() have SM values, V = gamma or Z.


pdgid: S044ZVG
text:
AAD 2013AN study Z gamma production in p p collisions. In events with no additional  jet, 1417 (2031) Z decays to electron (muon) pairs are selected, with an expected background of  156+-54 (244+-64) events, as well as 662 Z decays to neutrino pairs with an expected  background of 302+-42 events. Analysing the photon pT spectrum above 100 GeV yields the  95% C.L. limts: -0.013 < h_{{3}}^Z < 0.014, -8.7E-5 < h_{{4}}^Z  < 8.7E-5, -0.015 < h(3)**gamma < 0.016, -9.4E-5  < h(4)**gamma < 9.2E-5. Supersedes AAD 2012BX.


pdgid: S044ZVG
text:
CHATRCHYAN 2013BI determine the Z gamma --> nu nubar gamma cross section by selecting events with a photon of E(T)> 145 GeV and a notET> 130 GeV. 73 candidate events are observed with an expected SM background of 30.2+-6.5. The E(T) spectrum of the photon is used to set 95% C.L. limits as follows: |h_{{3}}^Z|< 2.7E-3, |h_{{4}}^Z|< 1.3E-5, |h(3)**gamma|< 2.9E-3, |h(4)**gamma|< 1.5E-5.


pdgid: S044ZVG
text:
ABAZOV 2012S study Z gamma production in p pbar collisions at sqrt(s) = 1.96 TeV using 6.2 fb**-1 of data  where the Z decays to electron (muon) pairs and the photon has at least 10 GeV of transverse momentum. In data, 304 (308)  di-electron (di-muon) events are observed with an expected background of 255+-16 (285+-24) events. Based on the photon pT spectrum, and including also earlier data and the Z --> nu nubar decay mode (from ABAZOV 2009L),  the following 95% C.L. limits are reported:  |h_{{03}}^Z()| < 0.026, |h_{{04}}^Z()| < 0.0013, |h(03)**gamma| < 0.027, |h(04)**gamma| < 0.0014 for a form factor scale of Lambda = 1.5 TeV.


pdgid: S044ZVG
text:
AALTONEN 2011S study Z gamma events in p pbar interactions at sqrt(s) = 1.96 TeV with integrated luminosity  5.1 fb**-1 for Z --> e+ e-/mu+ mu- and 4.9 fb**-1 for Z --> nu nubar. For the charged lepton case,  the two leptons must be of the same flavor with the transverse momentum/energy of one > 20 GeV and the other > 10 GeV. The isolated photon must have E(T)> 50 GeV. They observe 91 events with 87.2+-7.8 events expected from standard  model processes. For the nu nubar case they require solitary photons with E(T)> 25 GeV and missing E(T)  > 25 GeV and observe 85 events with standard model expectation of 85.9+-5.6 events. Taking the form factor Lambda = 1.5 TeV they derive 95% C.L. limits as |h(3)**gamma**,Z| < 0.022 and |h(4)**gamma**,Z| < 0.0009.


pdgid: S044ZVG
text:
CHATRCHYAN 2011M study Z gamma production in p p collisions at sqrt(s) = 7 TeV using 36 pb**-1 p p data, where the Z decays to e+ e- or mu+ mu-. The total cross sections are measured for photon transverse energy E(T)**gamma> 10 GeV and spatial separation from charged leptons in the plane of pseudo rapidity and azimuthal angle DeltaR(lepton,gamma)> 0.7 with the dilepton invariant mass requirement of M(lepton lepton)> 50 GeV. The number of e+ e- gamma and mu+ mu- gamma candidates is 81 and 90 with estimated backgrounds of 20.5+-2.5 and 27.3+-3.2 events respectively. The 95% CL limits for Z Z gamma couplings are -0.05< h_{{3}}^Z< 0.06 and -0.0005<h_{{4}}^Z< 0.0005, and for Z gamma gamma couplings are   -0.07<h(3)**gamma< 0.07 and -0.0005<h(4)**gamma< 0.0006.


pdgid: S044ZVG
text:
ABAZOV 2009L study Z gamma, Z --> nu nubar production in p pbar collisions at 1.96 TeV C.M. energy. They select 51 events with a photon of transverse energy E(T) larger than 90 GeV, with an expected background of 17 events. Based on the photon E(T) spectrum and including also Z decays to charged leptons (from ABAZOV 2007M), the following 95% CL limits are reported: |h(30)**gamma|< 0.033, |h(40)**gamma|< 0.0017, |h_{{30}}^Z()|< 0.033, |h_{{40}}^Z()|< 0.0017.


pdgid: S044ZVG
text:
ABAZOV 2007M use 968 p pbar -->e+ e- / mu+ mu- gamma X candidates, at 1.96 TeV center of mass energy, to tag p pbar --> Z gamma events by requiring E(T)(gamma)>  7 GeV,  lepton-gamma separation DeltaR(lepton gamma)> 0.7, and di-lepton invariant mass > 30 GeV. The cross section is in agreement with the SM prediction. Using these Z gamma events they obtain 95% C.L. limits on each h_{{i}}^V(), keeping all others fixed at their SM values. They report: -0.083<h_{{30}}^Z()< 0.082, -0.0053<h_{{40}}^Z()< 0.0054, -0.085<h(30)**gamma< 0.084, -0.0053<h(40)**gamma< 0.0054, for the form factor scale Lambda= 1.2 TeV.


pdgid: S044ZVG
text:
Using data collected at sqrt(s) = 183 -- 208, ABDALLAH 2007C select 1,877 e+ e- --> Z gamma events with Z --> q qbar or nu nubar, 171 e+ e- --> Z Z events with Z --> q qbar or lepton pair (except an explicit tau pair), and 74 e+ e- --> Z gamma^*() events with a q qbar mu+ mu- or q qbar e+ e- signature, to derive 95% CL limits on h_{{i}}^V(). Each limit is derived with other parameters set to zero. They report: -0.23<h_{{1}}^Z()< 0.23,  -0.30<h_{{3}}^Z()< 0.16,    -0.14<h(1)**gamma< 0.14,  -0.049<h(3)**gamma< 0.044.


pdgid: S044ZVG
text:
ACHARD 2004H select 3515 e+ e- --> Z gamma events with Z --> q qbar or nu nubar at sqrt(s) = 189 -- 209 GeV to derive 95% CL limits on h^V_i. For deriving each limit the other parameters are fixed at zero. They report: -0.153<h_{{1}}^Z<0.141, -0.087<h_{{2}}^Z<0.079, -0.220<h_{{3}}^Z<0.112, -0.068<h_{{4}}^Z<0.148, -0.057<h(1)**gamma<0.057, -0.050<h(2)**gamma<0.023, -0.059<h(3)**gamma<0.004, -0.004<h(4)**gamma<0.042.


pdgid: S044ZVG
text:
ABBIENDI,G 2000C study e+ e- --> Z gamma events (with Z --> q qbar and Z --> nu nubar) at 189 GeV to obtain the central values (and 95% CL limits) of these couplings: h(1)**Z= 0.000+-0.100 (-0.190,0.190), h(2)**Z= 0.000+-0.068 (-0.128,0.128), h(3)**Z= -0.074+0.102-0.103 (-0.269,0.119), h(4)**Z= 0.046+-0.068 (-0.084,0.175), h(1)**gamma= 0.000+-0.061 (-0.115,0.115), h(2)**gamma= 0.000+-0.041 (-0.077,0.077), h(3)**gamma= -0.080+0.039-0.041 (-0.164,-0.006), h(4)**gamma= 0.064+0.033-0.030 (+0.007,+0.134). The results are derived assuming that only one coupling at a time is different from zero.


pdgid: S044ZVG
text:
ABBOTT 1998M study p pbar --> Z gamma + X, with Z --> e+ e-, mu+ mu-, nubar nu at 1.8 TeV, to obtain 95% CL limits at Lambda= 750 GeV: |h(30)**Z|<0.36, |h(40)**Z|<0.05 (keeping h(i)**gamma=0), and |h(30)**gamma|<0.37, |h(40)**gamma|<0.05 (keeping h(i)**Z=0). Limits on the CP-violating couplings are |h(10)**Z|<0.36, |h(20)**Z|<0.05 (keeping h(i)**gamma=0), and |h(10)**gamma|<0.37, |h(20)**gamma|<0.05 (keeping h(i)**Z=0).


pdgid: S044ZVG
text:
ABREU 1998K determine a 95% CL upper limit on CS(e+ e- --> gamma + invisible particles) <2.5pb using 161 and 172 GeV data.  This is used to set 95% CL limits on |h(30)**gamma|<0.8 and |h(30)**Z|<1.3, derived at a scale Lambda=1TeV and with n=3 in the form factor representation.


pdgid: S044ZZZ
text:
AAD 2023CH measure Z Z production with the Z bosons decaying to electrons or muons.  Analysing the angular information of the final-state four-lepton system, the following limits are  derived at 95% C.L.: -0.012 < f^Z_4 < 0.012, -0.015 <  f(4)**gamma < 0.015.


pdgid: S044ZZZ
text:
SIRUNYAN 2021Q measure Z Z production where both Z bosons decay in the electron or   muon channel. Analyzing the four-lepton invariant mass distribution, the following limits are   derived at 95% C.L. in units of E-4: -6.6 < f_{{4}}^Z < 6.0, -5.5   < f_{{5}}^Z < 7.5, -7.8 < f(4)**gamma < 7.1, -6.8   < f(5)**gamma < 7.5. This set of parameters is linearly related to a set   of EFT parameters, resulting in the following limits at 95% C.L. in units of TeV**-4:   -2.3 < c(Btilde W)/Lambda**4 < 2.5, -1.4 < c(W W)/Lambda**4   < 1.2, -1.4 < c(B W)/Lambda**4 < 1.3, -1.2 < c(B B)/Lambda**4 <   1.2.


pdgid: S044ZZZ
text:
AABOUD 2019AY study Z Z production in the lepton lepton nu nu decay channel. Events  with a pair of isolated high-transverse momentum charged leptons (electron pairs or muon pairs),  and with large missing energy, are selected. In the data, 371 (416) di-electron (di-muon) events  are found, with a total expected background of 128+-8 (143+-8) events. Analysing the  transverse momentum distribution of the charged dilepton system above 150 GeV, the following  95% C.L. limits are derived in units of E-3: -1.2 < f(4)**gamma  < 1.2, -1.0 < f_{{4}}^Z < 1.0, -1.2 < f(5)**gamma  < 1.2, -1.0 < f_{{5}}^Z < 1.0.


pdgid: S044ZZZ
text:
AABOUD 2018Q study p p --> Z Z events at sqrt(s) = 13 TeV with Z --> e+ e- or Z --> mu+ mu-. The  number of events observed in the 4e, 2e 2mu, and 4mu channels is 249, 465, and 303  respectively. Analysing the pT spectrum of the leading Z boson, the following the  following 95% C.L. limits are derived in units of E-4: -1.8 <  f(4)**gamma < 1.8, -1.5 < f(4)**Z < 1.5,  -1.8 < f(5)**gamma < 1.8, -1.5 < f(5)**Z  < 1.5.


pdgid: S044ZZZ
text:
SIRUNYAN 2018BT study p p Z Z events at sqrt(s) = 13 TeV with Z --> e+ e- or Z --> mu+ mu-. The  number of events observed in the 4e, 2e 2mu, and 4mu channels is 220, 543 and 335  respectively. Analysing the 4-lepton invariant mass spectrum, the following 95% C.L. limits  are derived in units of E-3: -1.2 < f(4)**gamma < 1.3,  -1.2 < f(4)**Z < 1.0, -1.2 < f(5)**gamma  < 1.3, -1.0 < f(5)**Z < 1.3.


pdgid: S044ZZZ
text:
KHACHATRYAN 2015B study Z Z production in 8 TeV p p collisions. In the decay modes Z Z --> 4 e, 4mu, 2e 2mu, 54, 75, 148 events are observed, with an expected background of 2.2+-0.9, 1.2+-0.6, and 2.4+-1.0 events, respectively. Analysing the 4-lepton invariant mass spectrum in the range from 110 GeV to 1200 GeV, the following 95% C.L.  limits are obtained: |f(4)**Z| < 0.004, |f(5)**Z| < 0.004, |f(4)**gamma| < 0.005, |f(5)**gamma| < 0.005.


pdgid: S044ZZZ
text:
KHACHATRYAN 2015BC use the cross section measurement of the final state p p --> Z Z --> 2 lepton 2 nu,  (lepton being an electron or a muon) at 7 and 8 TeV to put limits on these triple gauge couplings. Effective mass of the charged lepton pair is required to be in the range 83.5 -- 98.5 GeV and the dilepton pT > 45 GeV. The reduced missing E(T) is required to be > 65  GeV, which takes into account the fake missing E(T) due to detector effects. The numbers of e+ e- and mu+ mu- events selected are 35 and 40 at 7 TeV and 176 and 271 at 8 TeV  respectively.   The production cross sections so obtained are in agreement with SM predictions. The  following   95% C.L. limits are set: -0.0028 < f_{{4}}^Z < 0.0032,  -0.0037 <   f(4)**gamma < 0.0033, -0.0029 < f_{{5}}^Z  < 0.0031,   -0.0033 < f(5)**gamma < 0.0037. Combining with  previous results   (KHACHATRYAN 2015B and CHATRCHYAN 2013B) which include 7 TeV and 8  TeV data on the   final states p p --> Z Z --> 2 lepton 2 lepton^' where lepton and  lepton^' are an   electron or a muon, the best limits are -0.0022 < f_{{4}}^Z <  0.0026, -0.0029   < f(4)**gamma < 0.0026, -0.0023 <  f_{{5}}^Z < 0.0023,   -0.0026 < f(5)**gamma < 0.0027.


pdgid: S044ZZZ
text:
AAD 2013Z study Z Z production in p p collisions at sqrt(s) = 7 TeV. In the Z Z --> lepton+ lepton- lepton^'()+ lepton^'()- final state they observe a total of 66 events with an expected background of 0.9+-1.3. In the Z Z --> lepton+ lepton- nu nu  final state they observe a total of 87 events with an expected background of 46.9+-5.2. The limits on anomalous TGCs are determined  using the observed and expected numbers of these Z Z events binned in p_{{T}}^Z. The 95% C.L. are as follows:  for form factor scale Lambda = inf, -0.015 < f(4)**gamma < 0.015, -0.013 < f(4)**Z < 0.013, -0.016 < f(5)**gamma < 0.015, -0.013 < f(5)**Z < 0.013; for form factor scale Lambda = 3 TeV, -0.022 < f(4)**gamma < 0.023, -0.019 < f(4)**Z < 0.019, -0.023 < f(5)**gamma < 0.023, -0.020 < f(5)**Z < 0.019.


pdgid: S044ZZZ
text:
CHATRCHYAN 2013B study Z Z production in p p collisions and select 54 Z Z candidates in the Z decay channel with electrons or muons with an expected background of 1.4+-0.5 events. The resulting 95% C.L. ranges are: -0.013 < f(4)**gamma < 0.015, -0.011 < f(4)**Z < 0.012, -0.014 < f(5)**gamma < 0.014, -0.012 < f(5)**Z < 0.012.


pdgid: S044ZZZ
text:
Using data collected in the center of mass energy range 192 -- 209 GeV, SCHAEL 2009 select 318 e+ e- --> Z Z events with 319.4 expected from the standard model. Using this data they derive the following 95% CL limits: -0.321<f(4)**gamma< 0.318, -0.534<f_{{4}}^Z()< 0.534, -0.724<f(5)**gamma< 0.733, -1.194<f_{{5}}^Z()< 1.190.


pdgid: S044ZZZ
text:
ABAZOV 2008K search for Z Z and Z gamma^*() events with 1fb**-1 p pbar data at sqrt(s) = 1.96 TeV in ( e e )( e e ), ( mu mu )( mu mu ), ( e e )( mu mu ) final states requiring the lepton pair masses to be > 30 GeV. They observe 1 event, which is consistent with an expected signal of 1.71+-0.15 events and a background of 0.13+-0.03 events. From this they derive the following limits, for a form factor (Lambda) value of 1.2 TeV: -0.28<f_{{40}}^Z()< 0.28, -0.31<f_{{50}}^Z()< 0.29, -0.26<f_{{40}}^gamma()< 0.26, -0.30<f_{{50}}^gamma()< 0.28.


pdgid: S044ZZZ
text:
Using data collected at sqrt(s) = 183 -- 208 GeV, ABDALLAH 2007C select 171 e+ e- --> Z Z events with Z --> q qbar or lepton pair (except an explicit tau pair), and 74 e+ e- --> Z gamma^*() events with a q qbar mu+ mu- or q qbar e+ e- signature, to derive 95% CL limits on f_{{i}}^V(). Each limit is derived with other parameters set to zero. They report: -0.40<f_{{4}}^Z()< 0.42,  -0.38<f_{{5}}^Z()< 0.62,    -0.23<f(4)**gamma< 0.25,  -0.52<f(5)**gamma< 0.48.


pdgid: S044ZZZ
text:
ABBIENDI 2004C study Z Z production in e+ e- collisions in the C.M. energy range 190 -- 209 GeV.  They select 340 events with an expected background of 180 events. Including the ABBIENDI 2000N data at 183 and 189 GeV (118 events with an expected background of 65 events) they report the following 95% CL limits: -0.45<f(4)**Z<0.58, -0.94<f(5)**Z<0.25, -0.32<f(4)**gamma<0.33, and -0.71<f(5)**gamma<0.59.


pdgid: S044ZZZ
text:
ACHARD 2003D study Z-boson pair production in e+ e- collisions in the C.M. energy range 200 -- 209 GeV.  They select 549 events with an expected background of 432 events.  Including the ACCIARRI 1999G and ACCIARRI 1999O data (183 and 189 GeV respectively, 286 events with an expected background of 241 events) and the 192 -- 202 GeV ACCIARRI 2001I results (656 events, expected background of 512 events), they report the following 95% CL limits: -0.48<=f(4)**Z<=0.46, -0.36<=f(5)**Z<=1.03, -0.28<=f(4)**gamma<=0.28, and -0.40<=f(5)**gamma<=0.47.


pdgid: S044AQC
text:
ABBIENDI 2004L select 20 e+ e- --> nu nubar gamma gamma  acoplanar events in the energy range 180 -- 209 GeV and 176 e+ e- --> q qbar gamma gamma events in the energy range 130 -- 209 GeV. These samples are used to constrain possible anomalous W+ W- gamma gamma and Z Z  gamma  gamma quartic couplings. Further combining with the W+ W- gamma sample of ABBIENDI 2004B  the following one--parameter 95% CL limits are obtained: -0.007 < a_{{0}}^Z/Lambda**2 < 0.023 GeV**-2, -0.029 < a_{{c}}^Z/Lambda**2 < 0.029 GeV**-2, -0.020 < a_{{0}}^W/Lambda**2 < 0.020 GeV**-2, -0.052 < a_{{c}}^W/Lambda**2 < 0.037 GeV**-2.


pdgid: S044AQC
text:
In the CM energy range 183 to 209 GeV HEISTER 2004A select 30 e+ e- --> nu nubar gamma gamma events with two acoplanar, high energy and high transverse momentum photons. The photon--photon acoplanarity is required to be > 5degree, E(gamma)/sqrt(s) > 0.025 (the more energetic photon having energy > 0.2 sqrt(s)), p(T(gamma))/E(beam)  > 0.05 and |cos( theta(gamma) )| < 0.94. A likelihood fit to the photon energy and recoil missing mass yields the following one--parameter 95% CL limits: -0.012 < a_{{0}}^Z/Lambda**2 < 0.019 GeV**-2, -0.041 < a_{{c}}^Z/Lambda**2 < 0.044 GeV**-2, -0.060 < a_{{0}}^W/Lambda**2 < 0.055 GeV**-2, -0.099 < a_{{c}}^W/Lambda**2 < 0.093 GeV**-2.


pdgid: S044AQC
text:
ACHARD 2002G study e+ e- --> Z gamma gamma --> q qbar gamma gamma events using data at center-of-mass energies from 200 to 209 GeV.  The photons are required to be isolated, each with energy >5GeV and |cos(theta)|<0.97, and the di-jet invariant mass to be compatible with that of the Zboson (74 -- 111 GeV). Cuts on Zvelocity (beta<0.73) and on the energy of the most energetic photon reduce the backgrounds due to non-resonant production of the q qbar gamma gamma state and due to ISR respectively, yielding a total of 40 candidate events of which 8.6 are expected to be due to background.  The energy spectra of the least energetic photon are fitted for all ten center-of-mass energy values from 130 GeV to 209 GeV (as obtained adding to the present analysis 130 -- 202 GeV data of ACCIARRI 2001E, for a total of 137 events with an expected background of 34.1 events) to obtain the fitted values a(0)/Lambda**2= 0.00+0.02-0.01 GeV**-2 and a(c)/Lambda**2= 0.03+0.01-0.02 GeV**-2, where the other parameter is kept fixed to its Standard Model value (0). A simultaneous fit to both parameters yields the 95% CL limits -0.02 GeV**-2<a(0)/Lambda**2<0.03 GeV**-2 and -0.07 GeV**-2<a(c)/Lambda**2<0.05 GeV**-2.


pdgid: S126M
text:
AAD 2023BP combine 13 TeV results of H --> gamma gamma (AAD 2023BU) and H --> Z Z^* --> 4 lepton  where lepton = e , mu (AAD 2023AU) using 140 fb**-1 of p p collision data.  The result is 125.10+-0.09(stat)+-0.07(syst) GeV.


pdgid: S126M
text:
SIRUNYAN 2020L result of H --> gamma gamma is combined with that of H --> Z Z^* --> 4 lepton  where lepton = e , mu (SIRUNYAN 2017AV).


pdgid: S126M
text:
AAD 2023AU use 139 fb**-1 of p p collisions at Ecm = 13 TeV with H --> Z Z^* --> 4 lepton where   lepton = e , mu.


pdgid: S126M
text:
AAD 2023BP combine 13 TeV results with 7 and 8 TeV results. The result is 125.11+-0.09(stat)+-0.06(syst)  GeV.


pdgid: S126M
text:
AABOUD 2018BM use 36.1 fb**-1 of p p collisions at Ecm = 13 TeV with H --> Z Z^* --> 4 lepton  where lepton = e , mu.


pdgid: S126M
text:
AABOUD 2018BM combine 13 TeV results with 7 and 8 TeV results. Other combined results are summarized in their Fig. 4.


pdgid: S126M
text:
SIRUNYAN 2017AV use 35.9 fb**-1 of p p collisions at Ecm = 13 TeV with H --> Z Z^* --> 4 lepton where  lepton = e , mu.


pdgid: S126M
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.


pdgid: S126M
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. Superseded by AAD 2014W.


pdgid: S126M
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. See also AAD 2012DA.


pdgid: S126M
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. See also CHATRCHYAN 2012BY and CHATRCHYAN 2013Y.


pdgid: S126CP
text:
AAD 2024AG search for CP violation in the decay kinematics and VBF production of the  Higgs boson using H --> Z Z^* --> 4 lepton decay channel (lepton = e , mu) with 139  fb**-1 at Ecm = 13 TeV. By using the optimal observables, the data constrain six  CP-odd Wilson coefficients in two effective field theory bases: the Warsaw basis and the  Higgs basis. The result is given in their Table 5 and Figs. 7 -- 11. The differential  fiducial cross sections for the four optimal observables are measured as shown in their Fig. 13.  The VBF fiducial cross sections are given in their Table 6.


pdgid: S126CP
text:
AAD 2024J measure the CP structure of the top Yukawa coupling using 139 fb**-1 of  data at Ecm = 13 TeV. The CP-mixing angle alpha for top Yukawa coupling is  measured to be (11+52-73)degree with the top Yukawa coupling strength modifier  kappa(t). See their Fig. 3. The data disfavour the pure CP-odd (alpha =  90degree) at 1.2 sigma.


pdgid: S126CP
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AAD 2023AK measure the CP structure of the tau Yukawa coupling using 139 fb**-1  of data at Ecm = 13 TeV. The CP-mixing angle alpha for tau Yukawa coupling  is measured to be 9+-16degree. The data disfavour the pure CP-odd (alpha  = 90degree) at 3.4 sigma.


pdgid: S126CP
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AAD 2023AN test CP invariance in H production via VBF using H --> gamma gamma    decay channel with 139 fb**-1 at Ecm = 13 TeV. By using the Optimal Observable method,    the data constrain parameters describing the strength of the CP-odd component in the  coupling   between Higgs and W/Z in effective field theory bases: dtilde in the HISZ  basis and   c(H Wtilde) in the Warsaw basis. The result is -0.010 <= dtilde  <=   0.040 and -0.15 <= c(H Wtilde) <= 0.67 at 68% CL. See  their Table  I,  which shows the result combined with H --> tau tau (AAD 2020N): -0.012  <=   dtilde <= 0.030 at 68% CL.


pdgid: S126CP
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TUMASYAN 2023AJ constraint anomalous couplings of the Higgs to vector bosons and fermions   using p p --> H --> tau tau at Ecm = 13 TeV with 138 fb**-1 data. The   CP-violating parameter in gluon-fusion production f_{{a3}}^ggH and the effective mixing angle   alpha^Hff are given in their Table VII with H --> tau tau and f_{{a3}}^ggH in  their Table  X with H --> tau tau and . Using the VBF production analysis, the   CP-violating parameter f_{{a3}} and the CP-conserving parameters f_{{a2}},   f(Lambda1) and f( Lambda1)**Z gamma are given in their Table   VIII with H --> tau tau and Table IX with H --> tau tau and . The   CP-violating parameter f_{{CP}}^Htt is constrained to be 0.03+0.17-0.03 using H --> tau tau,    and H --> gamma gamma.


pdgid: S126CP
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TUMASYAN 2023P constrain kappatilde_{{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 kappatilde_{{t}} is constrained to be |kappatilde_{{t}}| <= 1.4  at 95% CL by fixing kappa_{{t}} = 1 and other couplings      (kappa_{{V}} etc.) to the SM  values, see their Table 6 (see their Fig. 9 for 2-dim contours).  The fractional contribution of     the  CP-odd component |f(CP)**H t t| is  constrained to (0.24, 0.81) at      68% CL with a best fit value of 0.59. The combination with  other t tbar H decaying H --> gamma gamma      (SIRUNYAN 2020AS) and   (SIRUNYAN 2021AE) constraints to be  |kappatilde_{{t}}| <=  1.07 at 95% CL and |f(CP)**H t t|<0.55 at     68% CL  with  a best fit value of 0.28.


pdgid: S126CP
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AAD 2022V measure the CP properties of the effective Higgs-gluon interaction using  gluon fusion H --> W W^* --> e nu mu nu plus two jets with 36.1 fb**-1 of data at  Ecm = 13 TeV. The measured tangent of the CP-mixing angle tan(alpha) is 0.0+-0.4+-0.3  assuming the standard model H V V couplings. See their Fig. 6.


pdgid: S126CP
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TUMASYAN 2022Y measure the CP structure of the tau Yukawa coupling using 137  fb**-1 of data at Ecm = 13 TeV. The CP-mixing angle alpha for tau  Yukawa coupling is measured to be -1+-19degree. The data disfavour the pure  CP-odd (alpha = 90degree) at 3.0 sigma.


pdgid: S126CP
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AAD 2020N test CP invariance in H production via VBF using H --> tau tau  decay channel with 36.1 fb**-1 at Ecm = 13 TeV. By using the Optimal Observable method,  the data constrain a parameter dtilde, which is for the strength of CP violation in an  effective field theory, to be -0.090 <= dtilde <= 0.035 at 68% CL (see  their Fig. 6).


pdgid: S126CP
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AAD 2020Z exclude a CP-mixing angle alpha, |alpha| >  43degree at 95% CL, where alpha = 0 represents the Standard Model, in 139  fb**-1 of data at Ecm = 13 TeV. The pure CP-odd structure of the top Yukawa  coupling (alpha = 90degree) is excluded at 3.9 sigma.


pdgid: S126CP
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SIRUNYAN 2020AS exclude the pure CP-odd structure of the top Yukawa coupling at 3.2  sigma using t tbar H, H --> gamma gamma in 137 fb**-1 of data at Ecm =  13 TeV. The fractional contribution of the CP-odd component f(CP)**t tbar H  is measured to be 0.00+-0.33.


pdgid: S126CP
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SIRUNYAN 2019BL measure the 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. See their Tables VI and VII for anomalous H V V  couplings of CP-violating and CP-conserving parameters with on- and off-shells.


pdgid: S126CP
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SIRUNYAN 2019BZ constrain anomalous H V V couplings of the Higgs boson with data of 35.9  fb**-1 at Ecm = 13 TeV using Higgs boson candidates with two jets produced in VBF, ggF,  and V H that decay to tau tau. See their Table 2 and Fig. 10, which show 68% CL and  95% CL intervals. Combining those with the  (SIRUNYAN 2019BL,  on-shell scenario), results shown in their Tables 3, 4, and Fig. 11 are obtained. A  CP-violating parameter is set to be f_{{a3}}cos(phi_{{a3}}) = 0.00+-0.27E-3 and  CP-conserving parameters are f_{{a2}}cos(phi_{{a2}}) = 0.08+1.04-0.21E-3,  f(Lambda1)cos(phi(Lambda1)) = 0.00+0.53-0.09E-3, and  f( Lambda1)**Z gammacos(phi(Lambda1)**Z gamma) =  0.0+1.1-1.3E-3.


pdgid: S126CP
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AABOUD 2018AJ study the tensor structure of the Higgs boson couplings using an effective  Lagrangian using 36.1 fb**-1 of p p collision data at Ecm = 13 TeV. Constraints are  set on the non-Standard-Model CP-even and CP-odd couplings to Z bosons and on the  CP-odd coupling to gluons. See their Figs. 9 and 10, and Tables 10 and 11.


pdgid: S126CP
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SIRUNYAN 2017AM constrain anomalous couplings of the Higgs boson with 5.1 fb**-1 of p p  collisions at Ecm = 7 TeV, 19.7 fb**-1 at Ecm = 8 TeV, and 38.6 fb**-1 at  Ecm = 13 TeV. See their Table 3 and Fig. 3, which show 68% CL and 95% CL  intervals. A CP violation parameter f_{{a3}} is set to be  f_{{a3}}cos(phi(a3)) = [-0.38, 0.46] at 95% CL (phi(a3) =  0 or pi).


pdgid: S126CP
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AAD 2016 study H --> gamma gamma with an effective Lagrangian including CP even  and odd terms in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. The data is consistent  with the expectations for the Higgs boson of the Standard Model. Limits on anomalous couplings are  also given.


pdgid: S126CP
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AAD 2016BL study VBF H --> tau tau with an effective Lagrangian including a CP odd  term in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV. The measurement is consistent  with the expectation of the Standard Model. The CP-mixing parameter dtilde (a  dimensionless coupling dtilde=-(m^2_W/Lambda**2)f(Wtilde W))  is constrained to the interval of (-0.11, 0.05) at 68% CL under the assumption of  dtilde = dtilde_{{B}}.


pdgid: S126CP
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KHACHATRYAN 2016AB search for anomalous pseudoscalar couplings of the Higgs boson to W  and Z with 18.9 fb**-1 of p p collisions at Ecm = 8 TeV. See their Table 5 and  Figs 5 and 6 for limits on possible anomalous pseudoscalar coupling parameters.


pdgid: S126CP
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AAD 2015AX compare the J**#italic{CP}= **0**+ Standard Model assignment with other  J**#italic{CP} hypotheses in 20.3 fb**-1 of p p collisions at Ecm = 8 TeV, using the  process H --> W W^* --> e nu mu nu.  **2**+ hypotheses are excluded at 84.5 -- 99.4%CL,  **0**- at 96.5%CL, **0**+ (field strength coupling) at 70.8%CL. See their  Fig. 19 for limits on possible CP mixture parameters.


pdgid: S126CP
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AAD 2015CI compare the J**#italic{CP}= **0**+ Standard Model assignment with other  J**#italic{CP} hypotheses in 4.5 fb**-1 of p p collisions at Ecm = 7 TeV and 20.3  fb**-1 at Ecm = 8 TeV, using the processes H --> Z Z^* --> 4 lepton. H --> gamma gamma  and combine with AAD 2015AX data.  **0**+ (field strength coupling), **0**- and  several **2**+ hypotheses are excluded at more than 99.9% CL. See their Tables   7 -- 9 for limits on possible CP mixture parameters.


pdgid: S126CP
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AALTONEN 2015 combine AALTONEN 2015B and ABAZOV 2014F data. An upper limit of  0.36 of the Standard Model production rate at 95% CL is obtained both for a **0**- and  a **2**+ state. Assuming the SM event rate, the J**#italic{CP} = **0**- (**2**+)  hypothesis is excluded at the 5.0sigma (4.9sigma) level.


pdgid: S126CP
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AALTONEN 2015B compare the J**#italic{CP} = **0**+ Standard Model assignment with other  J**#italic{CP} hypotheses in 9.45 fb**-1 of p pbar collisions at Ecm = 1.96 TeV, using the   processes Z H --> lepton lepton b bbar, W H --> lepton nu b bbar, and Z H --> nu nu b bbar.  Bounds on the production rates of **0**- and **2**+ (graviton-like) states are set,  see their tables II and III.


pdgid: S126CP
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KHACHATRYAN 2015Y compare the J**#italic{CP} = **0**+ Standard Model assignment with other  J**#italic{CP} hypotheses 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, using the processes H --> 4 lepton, H --> W W^*,  and H --> gamma gamma. **0**- is excluded at 99.98% CL, and several **2**+  hypotheses are excluded at more than 99% CL. Spin 1 models are excluded at more than  99.999% CL in Z Z^* and W W^* modes. Limits on anomalous couplings and several cross  section fractions, treating the case of CP-mixed states, are also given.


pdgid: S126CP
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ABAZOV 2014F compare the J**#italic{CP}= **0**+ Standard Model assignment with J**#italic{CP}= **0**- and **2**+ (graviton-like coupling) hypotheses in up to 9.7 fb**-1 of p pbar collisions at Ecm = 1.96 TeV. They use kinematic correlations between the decay products of the vector boson and the Higgs boson in the final states Z H --> lepton lepton b bbar, W H --> lepton nu b bbar, and Z H --> nu nu b bbar. The **0**- (**2**+) hypothesis is excluded at 97.6% CL (99.0% CL). In order to treat the case of a possible mixture of a 0**+** state with another J**#italic{CP} state, the cross section fractions f_{{X}} = sigma_{{X}}/(sigma(0**+**) + sigma_{{X}}) are considered, where X = 0**-**, 2**+**. Values for f(0**-**) (f(2**+**)) above 0.80 (0.67) are excluded at 95% CL under the assumption that the total cross section is that of the SM Higgs boson.


pdgid: S126CP
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CHATRCHYAN 2014AA compare the J**#italic{CP}= **0**+ Standard Model assignment with various J**#italic{CP} hypotheses in 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. J**#italic{CP}= **0**- and 1**+- hypotheses are excluded at 99% CL, and several J = 2 hypotheses are excluded at 95% CL. In order to treat the case of a possible mixture of a **0**+ state with another J**#italic{CP} state, the cross section fraction f_{{a3}} = |a_{{3}}|**2 sigma_{{3}} / (|a_{{1}}|**2 sigma_{{1}} + |a_{{2}}|**2 sigma_{{2}}  + |a_{{3}}|**2 sigma_{{3}}) is considered, where the case a_{{3}} = 1, a_{{1}} = a_{{2}} = 0 corresponds to a pure CP-odd state. Assuming a_{{2}} = 0, a value for f_{{a3}} above 0.51 is excluded at 95% CL.


pdgid: S126CP
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CHATRCHYAN 2014G compare the J**#italic{CP}= **0**+ Standard Model assignment with J**#italic{CP}= **0**- and **2**+ (graviton-like coupling) hypotheses in 4.9 fb**-1  of p p collisions at Ecm = 7 TeV and 19.4 fb**-1 at Ecm = 8 TeV. Varying the  fraction of the production of the **2**+ state via g g and q qbar, **2**+  hypotheses are disfavored at CL between 83.7 and 99.8%. The **0**- hypothesis is  disfavored against **0**+ at the 65.3% CL.


pdgid: S126CP
text:
KHACHATRYAN 2014P compare the J**#italic{CP}= **0**+ Standard Model assignment with a **2**+ (graviton-like coupling) hypothesis in 5.1 fb**-1 of p p collisions at Ecm = 7 TeV and 19.7 fb**-1 at Ecm = 8 TeV. Varying the fraction of the production of the **2**+ state via g g and q qbar, **2**+ hypotheses are disfavored at CL between 71 and 94%.


pdgid: S126CP
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AAD 2013AJ compare the spin 0, CP-even hypothesis with specific alternative hypotheses of spin 0, CP-odd, spin 1, CP-even and CP-odd, and spin 2, CP-even models using the Higgs boson decays H --> gamma gamma, H --> Z Z^* --> 4 lepton and H --> W W^* --> lepton nu lepton nu and combinations thereof. The data are compatible with the spin 0, CP-even hypothesis, while all other tested hypotheses are excluded at confidence levels above 97.8%.


pdgid: S126CP
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CHATRCHYAN 2013J study angular distributions of the lepton pairs in the Z Z^* channel where both Z bosons decay to e or mu pairs. Under the assumption that the observed particle has spin 0, the data are found to be consistent with the pure CP-even hypothesis, while the pure CP-odd hypothesis is disfavored.


pdgid: S126W
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AAD 2023BR use 139 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, AAD 2020AQ) decay channels are used  to measure the total width. The off-shell Higgs signal strength is measured to be 1.1+0.7-0.6  assuming the same on-shell and off-shell coupling modifiers are used individually for gluon-fusion  and for gauge-boson modes. The scenario of no off-shell contribution is excluded at 3.3  sigma. Combining with the on-shell signal strength measurement, the total width normalized  to its SM expectation Gamma(H)/Gamma(H)**SM is measured to be 1.1+0.7-0.6  assuming the same on-shell and off-shell coupling modifiers are used individually for gluon-fusion  and for gauge-boson modes. The observed upper limit on the total width is 10.2 MeV at 95% CL.  See their Fig. 7. See corrected width values their erratum AAD 2024P.


