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

INSPIRE   PDGID:
S046GNV
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$> 2200$ 95 1
AAD
2021BF
 ATLS ${{\mathit \ell}^{\pm}}$ + ${{\mathit b}}$-jets + many jets, Tglu3F, $\lambda {}^{''}_{323}$ electroweakino decay, 500 GeV $<$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 1600 GeV
$> 2250$ 95 1
AAD
2021BF
 ATLS ${{\mathit \ell}^{\pm}}$ + ${{\mathit b}}$-jets + many jets, Tglu3G, $\lambda {}^{''}_{323}$ electroweakino decay, 600 GeV $<$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 1600 GeV
$> 2200$ 95 1
AAD
2021BF
 ATLS ${{\mathit \ell}^{\pm}}$ + ${{\mathit b}}$-jets + many jets, Tglu3B, $\lambda {}^{''}_{323}$ electroweakino decay, 600 GeV $<$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 1600 GeV
$> 1800$ 95 1
AAD
2021BF
 ATLS ${{\mathit \ell}^{\pm}}$ + ${{\mathit b}}$-jets + many jets, Tglu3B, $\lambda {}^{''}_{323}$, ${{\widetilde{\mathit t}}}$ decay, ${\mathit m}_{{{\widetilde{\mathit t}}}}$ $<$ 1200 GeV
$> 2200$ 95 1
AAD
2021BF
 ATLS ${{\mathit \ell}^{\pm}}$ + ${{\mathit b}}$-jets + many jets, Tglu1A, ${{\mathit \lambda}^{\,'}}$, ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ decay with equal probability into ${{\mathit e}}$, ${{\mathit \mu}}$, ${{\mathit \nu}_{{e}}}$, ${{\mathit \nu}_{{\mu}}}$, 400 GeV $<$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 1700 GeV
$> 2500$ 95 2
AAD
2021Y
 ATLS ${}\geq{}4{{\mathit \ell}}$, Tglu1A with ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}{{\mathit \nu}}$ , ${{\mathit \lambda}_{{12k}}}{}\not=$ 0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 2200 GeV
$> 1900$ 95 2
AAD
2021Y
 ATLS ${}\geq{}4{{\mathit \ell}}$, Tglu1A with ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}{{\mathit \nu}}$ , ${{\mathit \lambda}_{{i33}}}{}\not=$ 0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 1550 GeV
$> 1600$ 95 3
AAD
2020AL
 ATLS 8 or more jets+$\not E_T$, Tglu2RPV
$> 1600$ 95 4
AAD
2020V
 ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ + jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit d}}$ simplified model
$> 2150$ 95 5
SIRUNYAN
2020T
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ or ${}\geq{}3{{\mathit \ell}^{\pm}}$ + jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\overline{\mathit q}}}{{\overline{\mathit q}}}{+}$ ${{\mathit e}}$ $/$ ${{\mathit \mu}}$ $/$ ${{\mathit \tau}}$ simplified model
$\bf{> 1725}$ 95 5
SIRUNYAN
2020T
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ or ${}\geq{}3{{\mathit \ell}^{\pm}}$+jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ simplified model
$\bf{> 1500}$ 95 6
SIRUNYAN
2019F
 CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}{{\mathit j}}$
$\bf{> 2260}$ 95 7
AABOUD
2018Z
 ATLS ${}\geq{}4{{\mathit \ell}}$, ${{\mathit \lambda}_{{12k}}}{}\not=$ 0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $>$ 1000 GeV
$> 1650$ 95 7
AABOUD
2018Z
 ATLS ${}\geq{}4{{\mathit \ell}}$, ${{\mathit \lambda}_{{i33}}}{}\not=$ 0, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $>$ 500 GeV
$> 1610$ 95 8
SIRUNYAN
2018AK
 CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ , ${{\mathit \lambda}_{{332}}^{''}}$ coupling
$> 1690$ 95 9
SIRUNYAN
2018D
 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 10
SIRUNYAN
2018EA
 CMS 2 large jets with four-parton substructure, ${{\widetilde{\mathit g}}}$ $\rightarrow$ 5 ${{\mathit q}}$
$>2100$ 95 11
AABOUD
2017AI
 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 12
AABOUD
2017AI
 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 13
AABOUD
2017AI
 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 14
AABOUD
2017AJ
 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 15
AABOUD
2017AJ
 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 16
AABOUD
2017AJ
 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 17
AABOUD
2017AJ
 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 18
AABOUD
2017AJ
 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 19
AABOUD
2017AZ
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 20
KHACHATRYAN
2017Y
 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 21
KHACHATRYAN
2016BJ
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , Tglu3A, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 800 GeV
$>1140$ 95 21
KHACHATRYAN
2016BJ
 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 22
KHACHATRYAN
2016BX
 CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ , ${{\mathit \lambda}_{{332}}^{''}}$ coupling
$>1150$ 95 23
AAD
2015BV
 ATLS general RPC ${{\widetilde{\mathit g}}}$ decays, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 100 GeV
$> 1350$ 95 24
AAD
2014X
 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 25
CHATRCHYAN
2014P
 CMS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}{{\mathit j}}$
$\text{none 200 - 835}$ 95 25
CHATRCHYAN
2014P
 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 26
AABOUD
2018CF
 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 27
KHACHATRYAN
2016BX
 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 23
AAD
2015BV
 ATLS pMSSM, M$_{1}$ = 60 GeV, ${\mathit m}_{{{\widetilde{\mathit q}}}}$ $<$ 1500 GeV
$>1280$ 95 23
AAD
2015BV
 ATLS mSUGRA, ${\mathit m}_{\mathrm {0}}$ $>$ 2 TeV
$>1100$ 95 23
AAD
2015BV
 ATLS via ${{\widetilde{\mathit \tau}}}$, natural GMSB, all ${\mathit m}_{{{\widetilde{\mathit \tau}}}}$
$>1220$ 95 23
AAD
2015BV
 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 23
AAD
2015BV
 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 23
AAD
2015BV
 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
28
AAD
2015CB
 ATLS ${{\mathit \ell}}$, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ( ${{\mathit e}}$ $/$ ${{\mathit \mu}}$) ${{\mathit q}}{{\mathit q}}$ , benchmark gluino, neutralino masses
$>600$ 95 28
AAD
2015CB
 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 29
AAD
2015X
 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 29
AAD
2015X
 ATLS ${}\geq{}$6,7 jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ , (light-quark, $\lambda {}^{''}$ couplings)
$>929$ 95 29
AAD
2015X
 ATLS ${}\geq{}$6,7 jets, ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit q}}$ , (b-quark, $\lambda {}^{''}$ couplings)
$> 1180$ 95 30
AAD
2014AX
 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 31
AAD
2014E
 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 32
CHATRCHYAN
2014H
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ simplified model
1  AAD 2021BF searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for pair production of gluinos, stops, electroweakinos decaying RPV either directly or indirectly via the LSP. The final state in all cases is one or two leptons, many jets (up to fifteen) and ${{\mathit b}}$-jets. Different models with different branching fractions of the gluino or stop follow from the assumptions on the nature of the electroweakinos. No significant excess above the Standard Model predictions is observed. Limits are set on the , ${{\widetilde{\mathit t}}_{{1}}}$, electroweakino masses as a function of the ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ mass in several scenarios of gluino, stop and electroweakino pair production.
2  AAD 2021Y searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for supersymmetry in events with four or more leptons (electrons, muons and tau-leptons). No significant excess above the Standard Model expectations is observed. Limits are set on Tchi1n12-GGM, and RPV models similar to Tchi1n2I, Tglu1A (with ${{\mathit q}}$ = ${{\mathit u}}$, ${{\mathit d}}$, ${{\mathit s}}$, ${{\mathit c}}$, ${{\mathit b}}$, with equal branching fractions), and ${{\widetilde{\mathit \ell}}_{{L}}}$ $/$ ${{\widetilde{\mathit \nu}}}$ $\rightarrow$ ${{\mathit \ell}}$ $/$ ${{\mathit \nu}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ (mass-degenerate ${{\widetilde{\mathit \ell}}_{{L}}}$ and ${{\widetilde{\mathit \nu}}}$ of all 3 generations), all with ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $\rightarrow$ ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}{{\mathit \nu}}$ via ${{\mathit \lambda}_{{12k}}}$ or ${{\mathit \lambda}_{{i 33}}}$ (where $\mathit i,k$ $\in$ 1,2), see their Figure 11.
3  AAD 2020AL searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with 8 or more jets and moderate missing transverse momentum. The selection makes requirements according to the number of ${{\mathit b}}$-tagged jets and the scalar sum of masses of large-radius jets. No significant excess above the Standard Model expectations is observed. Exclusion limits at 95$\%$ C.L. are set on the gluino mass in RPV simplified models where the gluino decays via ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit d}}$ or ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ . They extend up to almost 1.6 TeV for a ${{\widetilde{\mathit t}}_{{1}}}$ mass of 900 GeV. See their Fig. 10(c).
4  AAD 2020V searched in 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two same-sign charged leptons (electrons or muons) and jets. No significant excess above the Standard Model expectations is observed. Exclusion limits at 95$\%$ C.L. are set on the gluino mass in RPV simplified models where the gluino decays via ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit d}}$ , see Figure 7(b).
5  SIRUNYAN 2020T searched in 137 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with at least two jets, and two isolated same-sign or three or more charged leptons (electrons or muons). No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu3A, Tglu3B, Tglu3C and Tglu3D simplified models, see their Figure 7, and in the Tglu1C and Tglu1B simplified models, see their Figures 8 and 9. Limits are also set on the sbottom mass in the Tsbot2 simplified model, see their Figure 10, and on the stop mass in the Tstop7 simplified model, see their Figure 11. Finally, limits are set on the gluino mass in RPV simplified models where the gluino decays either via ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\overline{\mathit q}}}{{\overline{\mathit q}}}{+}$ ${{\mathit e}}$ $/$ ${{\mathit \mu}}$ $/$ ${{\mathit \tau}}$ or via ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\mathit t}}{{\mathit b}}{{\mathit s}}$ , see Figure 12.
6  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.
7  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.
8  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.
9  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.
10  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.
11  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.
12  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.
13  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.
14  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).
15  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).
16  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).
17  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).
18  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).
19  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.
20  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.
21  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.
22  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.
23  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.
24  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.
25  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.
26  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.
27  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.
28  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. $12 - 20$.
29  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. $11 - 16$.
30  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.
31  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.
32  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.
References:
AAD 2021BF
EPJ C81 1023 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
AAD 2021Y
JHEP 2107 167 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
AAD 2020AL
JHEP 2010 062 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
AAD 2020V
JHEP 2006 046 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
SIRUNYAN 2020T
EPJ C80 752 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
SIRUNYAN 2019F
PR D99 012010 Search for pair-produced three-jet resonances in proton-proton collisions at $\sqrt s$ =13 TeV
AABOUD 2018CF
PL B785 136 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
AABOUD 2018Z
PR D98 032009 Search for supersymmetry in events with four or more leptons in $\sqrt{s}=13$ TeV $pp$ collisions with ATLAS
SIRUNYAN 2018AK
PL B783 114 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
SIRUNYAN 2018D
PR D97 012007 Search for Supersymmetry in Proton-Proton Collisions at 13 TeV using Identified Top Quarks
SIRUNYAN 2018EA
PRL 121 141802 Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
AABOUD 2017AI
JHEP 1709 088 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
AABOUD 2017AJ
JHEP 1709 084 Search for Supersymmetry in Final States with Two Same-Sign or Three Leptons and Jets using 36 ${\mathrm {fb}}{}^{-1}$ of $\sqrt {s }$ = 13 TeV ${{\mathit p}}{{\mathit p}}$ Collision Data with the ATLAS Detector
Also
JHEP 1908 121 (errat.) 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
AABOUD 2017AZ
JHEP 1712 034 Search for New Phenomena with Large Jet Multiplicities and Missing Transverse Momentum using Large-Radius Jets and Flavour-Tagging at ATLAS in 13 TeV ${{\mathit p}}{{\mathit p}}$ Collisions
KHACHATRYAN 2017Y
PL B770 257 Search for New Phenomena in Events with High Jet Multiplicity and Low Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2016BX
PR D94 112009 Searches for $\mathit R$-Parity-Violating Supersymmetry in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV in Final States with $0 - 4$ Leptons
KHACHATRYAN 2016BJ
EPJ C76 439 Search for New Physics in Same-sign Dilepton Events in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
AAD 2015CB
PR D92 072004 Search for Massive, Long-Lived Particles using Multitrack Displaced Vertices or Displaced Lepton Pairs in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2015X
PR D91 112016 Search for Massive Supersymmetric Particles Decaying to Many Jets using the ATLAS Detector in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
AAD 2015BV
JHEP 1510 054 Summary of the Searches for Squarks and Gluinos using $\sqrt {s }$ = 8 TeV ${{\mathit p}}{{\mathit p}}$ Collisions with the ATLAS Experiment at the LHC
AAD 2014X
PR D90 052001 Search for Supersymmetry in Events with Four or More Leptons in $\sqrt {s }$ = 8 TeV ${{\mathit p}}{{\mathit p}}$ Collisions with the ATLAS Detector
AAD 2014E
JHEP 1406 035 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
AAD 2014AX
JHEP 1410 024 Search for Strong Production of Supersymmetric Particles in Final States with Missing Transverse Momentum and at Least Three ${\mathit {\mathit b}}$-Jets at $\sqrt {s }$ = 8 TeV Proton-Proton Collisions with the ATLAS Detector
CHATRCHYAN 2014P
PL B730 193 Searches for Light- and Heavy-Flavour Three-Jet Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
CHATRCHYAN 2014H
JHEP 1401 163 Search for New Physics in Events with Same-Sign Dileptons and Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV