SCALE LIMITS for Contact Interactions: $\Lambda\mathrm {( {{\mathit \mu}} {{\mathit \mu}} {{\mathit q}} {{\mathit q}} )}$

$\Lambda_{LL}^+({\mathrm {TeV}}$) $\Lambda_{LL}^-({\mathrm {TeV}}$) CL% DOCUMENT ID TECN  COMMENT
$> 22.3$ > 32.7 95 1
 2021 Q
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$> 23.3$ $\mathbf {> 40.0}$ 95 2
 2021 N
CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$\mathbf {>22.3}$ >32.7 95 3
 2020 AP
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$>20.4$ > 30.4 95 4
 2019 AC
CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$>20$ > 30 95 5
 2017 AT
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
• • We do not use the following data for averages, fits, limits, etc. • •
$> 8.5$ > 8.5 95 6
 2021 AU
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit b}}{{\mathit s}}$ )
$>15.8$ >21.8 95 7
 2016 U
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$> 12.0$ >15.2 95 8
 2015 AE
CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$> 12.5$ > 16.7 95 9
 2014 BE
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$> 9.6$ > 12.9 95 10
 2013 E
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ ) (isosinglet)
$> 9.5$ > 13.1 95 11
 2013 K
CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ ) (isosinglet)
$> 8.0$ > 7.0 95 12
 2012 AB
ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ ) (isosinglet)
 1 AAD 2021Q limits are from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. A frequentist statistical framework is used to remove the prior dependence.
 2 SIRUNYAN 2021N limits are from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
 3 AAD 2020AP limits are from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
 4 SIRUNYAN 2019AC limits are from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV.
 5 AABOUD 2017AT limits are from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit uses a uniform positive prior in 1/${{\mathit \Lambda}^{2}}$ .
 6 AAD 2021AU search for new phenomena in final states with ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ and one or no ${{\mathit b}}$ -tagged jets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limits assume ${{\mathit g}_{{*}}^{2}}$ = 4 $\pi$.
 7 AABOUD 2016U limits are from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The quoted limit uses a uniform positive prior in 1/${{\mathit \Lambda}^{2}}$ .
 8 KHACHATRYAN 2015AE limit is from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV.
 9 AAD 2014BE limits are from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The quoted limit uses a uniform positive prior in 1/${{\mathit \Lambda}^{2}}$ .
 10 AAD 2013E limis are from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV.
 11 CHATRCHYAN 2013K limis are from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV.
 12 AAD 2012AB limis are from ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ mass distribution in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV.
References:
JHEP 2104 142 Search for new non-resonant phenomena in high-mass dilepton final states with the ATLAS detector
PRL 127 141801
 SIRUNYAN 2021N
JHEP 2107 208 Search for resonant and nonresonant new phenomena in high-mass dilepton final states at $\sqrt{s}$ = 13 TeV
JHEP 2011 005 Search for new non-resonant phenomena in high-mass dilepton final states with the ATLAS detector
 SIRUNYAN 2019AC
JHEP 1904 114 Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at $\sqrt{s} =$ 13 TeV
 AABOUD 2017AT
JHEP 1710 182 Search for New High-Mass Phenomena in the Dilepton Final State using 36 ${\mathrm {fb}}{}^{-1}$ of Proton-Proton Collision Data at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
 AABOUD 2016U
PL B761 372 Search for High-Mass New Phenomena in the Dilepton Final State using Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
 KHACHATRYAN 2015AE
JHEP 1504 025 Search for Physics Beyond the Standard Model in Dilepton Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
EPJ C74 3134 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
PR D87 015010 Search for Contact Interactions and Large Extra Dimensions in Dilepton Events from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector
PR D87 032001 Search for Contact Interactions in ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ Events in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
PL B712 40 Search for Contact Interactions in Dilepton Events from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector