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

INSPIRE  
$\Lambda_{LL}^+({\mathrm {TeV}}$) $\Lambda_{LL}^-({\mathrm {TeV}}$) CL% DOCUMENT ID TECN  COMMENT
$ > 22.3 $ > 32.7 95 1
AAD
2021Q
 ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ > 23.3 $ $\mathbf {> 40.0}$ 95 2
SIRUNYAN
2021N
 CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ \mathbf {>22.3} $ >32.7 95 3
AAD
2020AP
 ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ >20.4 $ > 30.4 95 4
SIRUNYAN
2019AC
 CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ >20 $ > 30 95 5
AABOUD
2017AT
 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
AAD
2021AU
 ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit b}}{{\mathit s}}$ )
$ >15.8 $ >21.8 95 7
AABOUD
2016U
 ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ > 12.0 $ >15.2 95 8
KHACHATRYAN
2015AE
 CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ > 12.5 $ > 16.7 95 9
AAD
2014BE
 ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ )
$ > 9.6 $ > 12.9 95 10
AAD
2013E
 ATLS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ ) (isosinglet)
$ > 9.5 $ > 13.1 95 11
CHATRCHYAN
2013K
 CMS ( ${{\mathit \mu}}{{\mathit \mu}}{{\mathit q}}{{\mathit q}}$ ) (isosinglet)
$ > 8.0 $ > 7.0 95 12
AAD
2012AB
 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:
AAD 2021Q
JHEP 2104 142 Search for new non-resonant phenomena in high-mass dilepton final states with the ATLAS detector
AAD 2021AU
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
AAD 2020AP
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
AAD 2014BE
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
AAD 2013E
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
CHATRCHYAN 2013K
PR D87 032001 Search for Contact Interactions in ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ Events in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AAD 2012AB
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