# Heavy ${{\widetilde{\boldsymbol g}}}$ (Gluino) mass limit

For ${\mathit m}_{{{\widetilde{\mathit g}}}}$ $>$ 60$-$70 GeV, it is expected that gluinos would undergo a cascade decay via a number of neutralinos and/or charginos rather than undergo a direct decay to photinos as assumed by some papers. Limits obtained when direct decay is assumed are usually higher than limits when cascade decays are included.
Some earlier papers are now obsolete and have been omitted. They were last listed in our PDG 2014 edition: K. Olive, $\mathit et~al.$ (Particle Data Group), Chinese Physics C38 070001 (2014) (http://pdg.lbl.gov).

# R-parity violating heavy ${{\widetilde{\boldsymbol g}}}$ (Gluino) mass limit INSPIRE search

VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$\bf{> 1500}$ 95 1
 2019 F
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}{{\mathit j}}$
$\bf{> 2260}$ 95 2
 2018 Z
ATLS ${}\geq{}4{{\mathit \ell}}$, ${{\mathit \lambda}_{{12k}}}{}\not=$ 0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $>$ 1000 GeV
$> 1650$ 95 2
 2018 Z
ATLS ${}\geq{}4{{\mathit \ell}}$, ${{\mathit \lambda}_{{i33}}}{}\not=$ 0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $>$ 500 GeV
$> 1610$ 95 3
 2018 AK
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ , ${{\mathit \lambda}_{{332}}^{''}}$ coupling
$> 1690$ 95 4
 2018 D
CMS top quark (hadronically decaying) + jets + $\not E_T$, Tglu3C, ${\mathit m}_{{{\widetilde{\mathit t}}_{{1}}}}−{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 20 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$\text{none 100 - 1410}$ 95 5
 2018 EA
CMS 2 large jets with four-parton substructure, ${{\widetilde{\mathit g}}}$ $\rightarrow$ 5 ${{\mathit q}}$
$>2100$ 95 6
 2017 AI
ATLS ${}\geq{}1{{\mathit \ell}}$+ ${}\geq{}$8 jets, Tglu3A and ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit u}}{{\mathit d}}{{\mathit s}}$ , ${{\mathit \lambda}_{{112}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=1000 GeV
$>1650$ 95 7
 2017 AI
ATLS ${}\geq{}1{{\mathit \ell}}$+ ${}\geq{}$8 jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}}$ , ${{\widetilde{\mathit t}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit s}}$ , ${{\mathit \lambda}_{{323}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit t}}}}$=1000 GeV
$> 1800$ 95 8
 2017 AI
ATLS ${}\geq{}1{{\mathit \ell}}$+ ${}\geq{}$8 jets, Tglu1A and ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit l}}$ , ${{\mathit \lambda}^{\,'}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=1000 GeV
$> 1800$ 95 9
 2017 AJ
ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ $/$ 3 ${{\mathit \ell}}$ + jets + $\not E_T$, Tglu3A, ${{\mathit \lambda}_{{112}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
$> 1750$ 95 10
 2017 AJ
ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ $/$ 3 ${{\mathit \ell}}$ + jets + $\not E_T$, Tglu1A and ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit \ell}}$ , ${{\mathit \lambda}^{\,'}}$ coupling
$> 1450$ 95 11
 2017 AJ
ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ $/$ 3 ${{\mathit \ell}}$ + jets + $\not E_T$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit s}}{{\mathit d}}$ , ${{\mathit \lambda}_{{321}}^{''}}$ coupling
$> 1450$ 95 12
 2017 AJ
ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ $/$ 3 ${{\mathit \ell}}$ + jets + $\not E_T$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit d}}$ , ${{\mathit \lambda}_{{313}}^{''}}$ coupling
$> 400$ 95 13
 2017 AJ
ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ $/$ 3 ${{\mathit \ell}}$ + jets + $\not E_T$, ${{\widetilde{\mathit d}}_{{R}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$( ${{\mathit t}}{{\mathit s}}$), ${{\mathit \lambda}_{{313}}^{''}}$ (${{\mathit \lambda}_{{321}}^{''}}$) coupling
$\text{none 625 - 1375}$ 95 14
 2017 AZ
ATLS ${}\geq{}$7 jets+$\not E_T$, large R-jets and/or ${{\mathit b}}$-jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit s}}$ , ${{\mathit \lambda}_{{323}}^{''}}$ coupling
$\text{none 600 - 650}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}$ , ${{\mathit \lambda}_{{212}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 100 GeV
$\text{none 600 - 1030}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}$ , ${{\mathit \lambda}_{{212}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 900 GeV
$\text{none 600 - 650}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit b}}$ , ${{\mathit \lambda}_{{213}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 100 GeV
$\text{none 600 - 1080}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit b}}$ , ${{\mathit \lambda}_{{213}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 900 GeV
$\text{none 600 - 680}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit b}}{{\mathit b}}$ , ${{\mathit \lambda}_{{212}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 100 GeV
$\text{none 600 - 1080}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}{{\mathit b}}{{\mathit b}}$ , ${{\mathit \lambda}_{{212}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 900 GeV
$\text{none 600 - 650}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit b}}{{\mathit b}}{{\mathit b}}$ , ${{\mathit \lambda}_{{213}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 100 GeV
$\text{none 600 - 1100}$ 95 15
 2017 Y
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit b}}{{\mathit b}}{{\mathit b}}$ , ${{\mathit \lambda}_{{213}}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ = 900 GeV
$>1050$ 95 16
 2016 BJ
CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , Tglu3A, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 800 GeV
$>1140$ 95 16
 2016 BJ
CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , Tglu3B, ${\mathit m}_{{{\widetilde{\mathit t}}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 20 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0
$> 1030$ 95 17
 2016 BX
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ , ${{\mathit \lambda}_{{332}}^{''}}$ coupling
$>1150$ 95 18
 2015 BV
ATLS general RPC ${{\widetilde{\mathit g}}}$ decays, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 100 GeV
$> 1350$ 95 19
 2014 X
ATLS ${}\geq{}4{{\mathit \ell}^{\pm}}$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}{{\mathit \nu}}$
$> 650$ 95 20
 2014 P
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}{{\mathit j}}$
$\text{none 200 - 835}$ 95 20
 2014 P
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit j}}{{\mathit j}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$> 1875$ 95 21
 2018 CF
ATLS jets and large R-jets, Tglu2RPV and ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ , ${{\mathit \lambda}^{''}}$ coupling, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=1000 GeV
$> 1400$ 95 22
 2016 BX
CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \nu}}$ , ${{\mathit \lambda}_{{121}}}$ or ${{\mathit \lambda}_{{122}}}{}\not=$0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}>$ 400 GeV
$>1600$ 95 18
 2015 BV
ATLS pMSSM, M$_{1}$ = 60 GeV, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ $<$ 1500 GeV
$>1280$ 95 18
 2015 BV
ATLS mSUGRA, ${\mathit m}_{\mathrm {0}}$ $>$ 2 TeV
$>1100$ 95 18
 2015 BV
ATLS via ${{\widetilde{\mathit \tau}}}$, natural GMSB, all ${\mathit m}_{{{\widetilde{\mathit \tau}}}}$
$>1220$ 95 18
 2015 BV
ATLS ${\mathit {\mathit b}}$-jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\widetilde{\mathit t}}_{{1}}}{{\mathit t}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\mathit T}_{{1}}}}$ $<$ 1000 GeV
$>1180$ 95 18
 2015 BV
ATLS ${\mathit {\mathit b}}$-jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\widetilde{\mathit t}}_{{1}}}{{\mathit t}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${\mathit m}_{{{\mathit T}_{{1}}}}$ $<$ 1000 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 60 GeV
$>880$ 95 18
 2015 BV
ATLS jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\widetilde{\mathit t}}_{{1}}}{{\mathit t}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit s}}{{\mathit b}}$ , 400 $<$ ${\mathit m}_{{{\widetilde{\mathit t}}_{{1}}}}$ $<$ 1000 GeV
23
 2015 CB
ATLS ${{\mathit \ell}}$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ( ${{\mathit e}}$ $/$ ${{\mathit \mu}}$) ${{\mathit q}}{{\mathit q}}$ , benchmark gluino, neutralino masses
$>600$ 95 23
 2015 CB
ATLS ${{\mathit \ell}}{{\mathit \ell}}$ /${{\mathit Z}}$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ( ${{\mathit e}}{{\mathit e}}$ $/$ ${{\mathit \mu}}{{\mathit \mu}}$ $/$ ${{\mathit e}}{{\mathit \mu}}$) ${{\mathit q}}{{\mathit q}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 400 GeV and 0.7 $<$ c$\tau _{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ $3 \times 10^{5}$ mm
$>1000$ 95 24
 2015 X
ATLS ${}\geq{}$10 jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=500 GeV
$>917$ 95 24
 2015 X
ATLS ${}\geq{}$6,7 jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ , (light-quark, $\lambda {}^{''}$ couplings)
$>929$ 95 24
 2015 X
ATLS ${}\geq{}$6,7 jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ , (b-quark, $\lambda {}^{''}$ couplings)
$> 1180$ 95 25
 2014 AX
ATLS ${}\geq{}$3 ${{\mathit b}}$-jets + $\not E_T$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\widetilde{\mathit t}}_{{1}}}{{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}=2{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=60 GeV, ${\mathit m}_{{{\widetilde{\mathit t}}_{{1}}}}<$1000 GeV
$> 850$ 95 26
 2014 E
ATLS ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$( ${{\mathit \ell}^{\mp}}$) + jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ with ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit s}}$ simplified model
$> 900$ 95 27
 2014 H
CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ simplified model
1  SIRUNYAN 2019F searched in 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for three-jet resonances produced in the decay of a gluino in R-parity violating supersymmetric models. The mass range from 200 to 2000GeV is explored in four separate mass regions. The observations show agreement with standard model expectations. The results are interpreted within the framework of R-parity violating SUSY, where pair-produced gluinos decay to a six quark final state. Gluino masses below 1500GeV are excluded at 95$\%$ C.L. See their Fig.5.
2  AABOUD 2018Z searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing four or more charged leptons (electrons, muons and up to two hadronically decaying taus). No significant deviation from the expected SM background is observed. Limits are set on the Higgsino mass in simplified models of general gauge mediated supersymmetry Tn1n1A/Tn1n1B/Tn1n1C, see their Figure 9. Limits are also set on the wino, slepton, sneutrino and gluino mass in a simplified model of NLSP pair production with R-parity violating decays of the LSP via ${{\mathit \lambda}_{{12k}}}$ or ${{\mathit \lambda}_{{i33}}}$ to charged leptons, see their Figures 7, 8.
3  SIRUNYAN 2018AK searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing a single lepton, large jet and ${{\mathit b}}$-quark jet multiplicities, coming from R-parity-violating decays of gluinos. No excess over the expected background is observed. Limits are derived on the gluino mass, assuming the RPV ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ decay, see their Figure 9.
4  SIRUNYAN 2018D searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing identified hadronically decaying top quarks, no leptons, and $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop1 simplified model, see their Figure 8, and on the gluino mass in the Tglu3A, Tglu3B, Tglu3C and Tglu3E simplified models, see their Figure 9.
5  SIRUNYAN 2018EA searched in 38.2 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for the pair production of resonances, each decaying to at least four quarks. Reconstructed particles are clustered into two large jets of similar mass, each consistent with four-parton substructure. No statistically significant excess over the Standard Model expectation is observed. Limits are set on the squark and gluino mass in RPV supersymmetry models where squarks (gluinos) decay, through intermediate higgsinos, to four (five) quarks, see their Figure 4.
6  AABOUD 2017AI searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more isolated lepton, at least eight jets, either zero or many ${{\mathit b}}$-jets, for evidence of R-parity violating decays of the gluino. No significant excess above the Standard Model expectations is observed. Limits up to 2.1 TeV are set on the gluino mass in R-parity-violating supersymmetry models as Tglu3A with LSP decay through the non-zero ${{\mathit \lambda}_{{112}}^{''}}$ coupling as ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit u}}{{\mathit d}}{{\mathit s}}$ . See their Figure 9.
7  AABOUD 2017AI searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more isolated lepton, at least eight jets, either zero or many ${{\mathit b}}$-jets, for evidence of R-parity violating decays of the gluino. No significant excess above the Standard Model expectations is observed. Limits up to 1.65 TeV are set on the gluino mass in R-parity-violating supersymmetry models with ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}}$ , ${{\widetilde{\mathit t}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit s}}$ through the non-zero ${{\mathit \lambda}_{{323}}^{''}}$ coupling. See their Figure 9.
8  AABOUD 2017AI searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more isolated lepton, at least eight jets, either zero or many ${{\mathit b}}$-jets, for evidence of R-parity violating decays of the gluino. No significant excess above the Standard Model expectations is observed. Limits up to 1.8 TeV are set on the gluino mass in R-parity-violating supersymmetry models as Tglu1A with the LSP decay through the non-zero ${{\mathit \lambda}^{\,'}}$ coupling as ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit \ell}}$ . See their Figure 9.
9  AABOUD 2017AJ searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two same-sign or three leptons, jets and large missing transverse momentum. No significant excess above the Standard Model expectations is observed. Limits up to 1.8 TeV are set on the gluino mass in R-parity-violating supersymmetry models as Tglu3A with LSP decaying through the non-zero ${{\mathit \lambda}_{{112}}^{''}}$ coupling as ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit u}}{{\mathit d}}{{\mathit s}}$ . See their Figure 5(d).
10  AABOUD 2017AJ searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two same-sign or three leptons, jets and large missing transverse momentum. No significant excess above the Standard Model expectations is observed. Limits up to 1.75 TeV are set on the gluino mass in R-parity-violating supersymmetry models as Tglu1A with LSP decaying through the non-zero ${{\mathit \lambda}^{\,'}}$ coupling as ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit \ell}}$ . See their Figure 5(c).
11  AABOUD 2017AJ searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two same-sign or three leptons, jets and large missing transverse momentum. No significant excess above the Standard Model expectations is observed. Limits up to 1.45 TeV are set on the gluino mass in R-parity-violating supersymmetry models where ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit s}}{{\mathit d}}$ through the non-zero ${{\mathit \lambda}_{{321}}^{''}}$ coupling. See their Figure 5(b).
12  AABOUD 2017AJ searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two same-sign or three leptons, jets and large missing transverse momentum. No significant excess above the Standard Model expectations is observed. Limits up to 1.45 TeV are set on the gluino mass in R-parity-violating supersymmetry models where ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit d}}$ through the non-zero ${{\mathit \lambda}_{{313}}^{''}}$ coupling. See their Figure 5(a).
13  AABOUD 2017AJ searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two same-sign or three leptons, jets and large missing transverse momentum. No significant excess above the Standard Model expectations is observed. Limits up to 400 GeV are set on the down type squark ( ${{\widetilde{\mathit d}}_{{R}}}$ mass in R-parity-violating supersymmetry models where ${{\widetilde{\mathit d}}_{{R}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}$ through the non-zero ${{\mathit \lambda}_{{313}}^{''}}$ coupling or ${{\widetilde{\mathit d}}_{{R}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit s}}$ through the non-zero ${{\mathit \lambda}_{{321}}^{''}}$. See their Figure 5(e) and 5(f).
14  AABOUD 2017AZ searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with at least seven jets and large missing transverse momentum. Selected events are further classified based on the presence of large R-jets or ${{\mathit b}}$-jets and no leptons. No significant excess above the Standard Model expectations is observed. Limits are set for R-parity violating decays of the gluino assuming ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit t}}_{{1}}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit s}}$ through the non-zero ${{\mathit \lambda}_{{323}}^{''}}$ couplings. The range $625 - 1375$ GeV is excluded for ${\mathit m}_{{{\widetilde{\mathit t}}_{{1}}}}$ = 400 GeV. See their Figure 7b.
15  KHACHATRYAN 2017Y searched in 19.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events containing at least 8 or 10 jets, possibly ${{\mathit b}}$-tagged, coming from R-parity-violating decays of supersymmetric particles. No excess over the expected background is observed. Limits are derived on the gluino mass, assuming various RPV decay modes, see Fig. 7.
16  KHACHATRYAN 2016BJ searched in 2.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the following simplified models: Tglu3A and Tglu3D, see Fig. 4, Tglu3B and Tglu3C, see Fig. 5, and Tglu1B, see Fig. 7.
17  KHACHATRYAN 2016BX searched in 19.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events containing 0 or 1 leptons and ${{\mathit b}}$-tagged jets, coming from R-parity-violating decays of supersymmetric particles. No excess over the expected background is observed. Limits are derived on the gluino mass, assuming the RPV ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ decay, see Fig. 7 and 10.
18  AAD 2015BV summarized and extended ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or ${\mathit {\mathit b}}$-jets in the $\sqrt {s }$ =8 TeV data set collected in 2012. The paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as new analyses. Exclusion limits at 95$\%$ C.L. are set on the gluino mass in several R-parity conserving models, leading to a generalized constraint on gluino masses exceeding 1150 GeV for lightest supersymmetric particle masses below 100 GeV. See their Figs. 10, 19, 20, 21, 23, 25, 26, 29-37.
19  AAD 2014X searched in 20.3 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with at least four leptons (electrons, muons, taus) in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in an R-parity violating simplified model where the decay ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , with ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}{{\mathit \nu}}$ , takes place with a branching ratio of 100$\%$, see Fig. 8.
20  CHATRCHYAN 2014P searched in 19.4 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for three-jet resonances produced in the decay of a gluino in R-parity violating supersymmetric models. No excess over the expected SM background is observed. Assuming a 100$\%$ branching ratio for the gluino decay into three light-flavour jets, limits are set on the cross section of gluino pair production, see Fig. 7, and gluino masses below 650 GeV are excluded at 95$\%$ C.L. Assuming a 100$\%$ branching ratio for the gluino decaying to one b-quark jet and two light-flavour jets, gluino masses between 200 GeV and 835 GeV are excluded at 95$\%$ C L.
21  AABOUD 2018CF searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with several jets, possibly ${{\mathit b}}$-jets, and large-radius jets for evidence of R-parity violating decays of the gluino. No significant excess above the Standard Model expectations is observed. Limits between 1000 and 1875 GeV are set on the gluino mass in R-parity-violating supersymmetry models as Tglu2RPV with the LSP decay through the non-zero ${{\mathit \lambda}^{''}}$ coupling as ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ . The most stringent limit is obtained for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 1000 GeV, the weakest for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV. See their Figure 7(b). Figure 7(a) presents results for gluinos directly decaying into 3 quarks, Tglu1RPV.
22  KHACHATRYAN 2016BX searched in 19.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events containing 4 leptons coming from R-parity-violating decays of ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \nu}}$ with ${{\mathit \lambda}_{{121}}}{}\not=$ 0 or ${{\mathit \lambda}_{{122}}}{}\not=$ 0. No excess over the expected background is observed. Limits are derived on the gluino, squark and stop masses, see Fig. 23.
23  AAD 2015CB searched for events containing at least one long-lived particle that decays at a significant distance from its production point (displaced vertex, DV) into two leptons or into five or more charged particles in 20.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The dilepton signature is characterised by DV formed from at least two lepton candidates. Four different final states were considered for the multitrak signature, in which the DV must be accompanied by a high-transverse momentum muon or electron candidate that originates from the DV, jets or missing transverse momentum. No events were observed in any of the signal regions. Results were interpreted in SUSY scenarios involving $\mathit R$-parity violation, split supersymmetry, and gauge mediation. See their Fig. $12 - 20$.
24  AAD 2015X searched in 20.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events containing large number of jets, no requirements on missing transverse momentum and no isolated electrons or muons. The sensitivity of the search is enhanced by considering the number of ${{\mathit b}}$-tagged jets and the scalar sum of masses of large-radius jets in an event. No evidence was found for excesses above the expected level of Standard Model background. Exclusion limits at 95$\%$ C.L. are set on the gluino mass assuming the gluino decays to various quark flavors, and for various neutralino masses. See their Fig. $11 - 16$.
25  AAD 2014AX searched in 20.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for the strong production of supersymmetric particles in events containing either zero or at last one high high-$p_T$ lepton, large missing transverse momentum, high jet multiplicity and at least three jets identified as originating from ${{\mathit b}}$-quarks. No excess over the expected SM background is observed. Limits are derived in mSUGRA/CMSSM models with tan $\beta$ = 30, ${{\mathit A}_{{0}}}$ = $-2{{\mathit m}_{{0}}}$ and ${{\mathit \mu}}$ $>$ 0, see their Fig. 14. Also, exclusion limits in simplified models containing gluinos and scalar top and bottom quarks are set, see their Figures 12, 13.
26  AAD 2014E searched in 20.3 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for strongly produced supersymmetric particles in events containing jets and two same-sign leptons or three leptons. The search also utilises jets originating from ${{\mathit b}}$-quarks, missing transverse momentum and other variables. No excess over the expected SM background is observed. Exclusion limits are derived in simplified models containing gluinos and squarks, see Figures 5 and 6. In the ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}^{\,'}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{(*)\pm}}{{\widetilde{\mathit \chi}}_{{2}}^{0}}$ , ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit Z}^{(*)}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, the following assumptions have been made: ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = 0.5 ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + ${\mathit m}_{{{\widetilde{\mathit g}}}}$, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = 0.5 (${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$), ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 520 GeV. In the ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}^{\,'}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \nu}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ or ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}^{\,'}}{{\widetilde{\mathit \chi}}_{{2}}^{0}}$ , ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}$( ${{\mathit \nu}}{{\mathit \nu}}$) ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, the following assumptions have been made: ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = 0.5 (${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + ${\mathit m}_{{{\widetilde{\mathit g}}}}$), ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 660 GeV. Limits are also derived in the mSUGRA/CMSSM, bRPV and GMSB models, see their Fig. 8.
27  CHATRCHYAN 2014H searched in 19.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with two isolated same-sign dileptons and jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in simplified models where the R-parity violating decay ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ takes place with a branching ratio of 100$\%$, see Fig. 8.
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