${{\widetilde{\mathit b}}}$ (Sbottom) mass limit

Limits in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ depend on the mixing angle of the mass eigenstate ${{\widetilde{\mathit b}}_{{1}}}$ = ${{\widetilde{\mathit b}}_{{L}}}$cos $\theta _{{{\mathit b}}}$ $+$ ${{\widetilde{\mathit b}}_{{R}}}$sin$\theta _{{{\mathit b}}}$. Coupling to the ${{\mathit Z}}$ vanishes for $\theta _{{{\mathit b}}}\sim{}1.17$. As a consequence, no absolute constraint in the mass region ${ {}\lesssim{} }$40 GeV is available in the literature at this time from ${{\mathit e}^{+}}{{\mathit e}^{-}}$ collisions. In the Listings below, we use $\Delta \mathit m$ = ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}–{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$.
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 conserving ${{\widetilde{\mathit b}}}$ (Sbottom) mass limit

INSPIRE   PDGID:
S046SBT
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$> 850$ 95 1
AAD
2021AM
 ATLS ${{\mathit \tau}^{\pm}}$'s + ${{\mathit b}}$-jets + $\not E_T$, Tsbot4, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 130 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ $<$ 180 GeV
$\bf{> 1270}$ 95 2
AAD
2021S
 ATLS ${{\mathit b}}$-jets + $\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=0 GeV
$> 660$ 95 2
AAD
2021S
 ATLS ${{\mathit b}}$-jets + $\not E_T$, Tsbot1,${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 10 GeV
$> 1600$ 95 3
SIRUNYAN
2021M
 CMS ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}$ + $\not E_T$, Tsbot3, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = 1500 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 100 GeV
$> 750$ 95 4
AAD
2020V
 ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ + jets, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + 100 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $\sim{}$ 50 GeV
$> 850$ 95 5
SIRUNYAN
2020T
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ or ${}\geq{}3{{\mathit \ell}^{\pm}}$ + jets, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ $<$ 800 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
$> 1500$ 95 6
AAD
2019H
 ATLS ${}\geq{}$3 ${{\mathit b}}$-jets + $\not E_T$, Tsbot4, ${}\geq{}$1 ${{\mathit h}}$( $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ), ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 60 GeV
$> 1300$ 95 7
AAD
2019H
 ATLS ${}\geq{}$3 ${{\mathit b}}$-jets+$\not E_T$, Tsbot4, ${}\geq{}1{{\mathit h}}(\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ), ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ +130 GeV
$> 1220$ 95 8
SIRUNYAN
2019CH
 CMS jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$> 530$ 95 9
SIRUNYAN
2019CI
 CMS ${}\geq{}$1 ${{\mathit H}}$ ( $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ ) + jets + $\not E_T$, Tsbot4, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + 130 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 1 GeV
$> 430$ 95 10
AABOUD
2018I
 ATLS ${}\geq{}$1 jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit b}}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $\sim{}{\mathit m}_{{{\mathit b}}}$
$> 840$ 95 11
SIRUNYAN
2018AL
 CMS ${}\geq{}3{{\mathit \ell}^{\pm}}$ + jets + $\not E_T$, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
$> 975$ 95 12
SIRUNYAN
2018AR
 CMS ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}$ + jets + $\not E_T$, Tsbot3, ${\mathit m}_{{{\widetilde{\mathit \ell}}}}$= (${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}+{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$)/2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$= 100 GeV
$> 1060$ 95 13
SIRUNYAN
2018AY
 CMS jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$> 1230$ 95 14
SIRUNYAN
2018B
 CMS jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$> 420$ 95 15
SIRUNYAN
2018X
 CMS ${}\geq{}$1 ${{\mathit H}}$ ( $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ ) + jets + $\not E_T$, Tsbot4, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + 130 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 225 GeV
$> 700$ 95 16
AABOUD
2017AJ
 ATLS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ $/$ 3 ${{\mathit \ell}}$ + jets + $\not E_T$, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$>950$ 95 17
AABOUD
2017AX
 ATLS 2 ${{\mathit b}}$-jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$\bf{>880}$ 95 18
AABOUD
2017AX
 ATLS 2 ${{\mathit b}}$-jets + $\not E_T$, mixture Tsbot1 and Tsbot2 BR=50$\%$, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 1 GeV
$> 315$ 95 19
KHACHATRYAN
2017A
 CMS 2 VBF jets + $\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit b}}}}−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 5 GeV
$> 450$ 95 20
KHACHATRYAN
2017AW
 CMS ${}\geq{}3{{\mathit \ell}^{\pm}}$, 2 jets, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = 200 GeV
$>800$ 95 21
KHACHATRYAN
2017P
 CMS 1 or more jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$> 1175$ 95 22
SIRUNYAN
2017AZ
 CMS ${}\geq{}$1 jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$>890$ 95 23
SIRUNYAN
2017K
 CMS jets+$\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$> 810$ 95 24
SIRUNYAN
2017S
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ + jets + $\not E_T$, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = 100 GeV
$> 323$ 95 25
AABOUD
2016D
 ATLS ${}\geq{}$1 jet + $\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}−{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 5 GeV
$> 840$ 95 26
AABOUD
2016Q
 ATLS 2 ${{\mathit b}}$-jets + $\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 100 GeV
$> 540$ 95 27
AAD
2016BB
 ATLS 2 same-sign/3${{\mathit \ell}}$ + jets + $\not E_T$, Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}<$ 55 GeV
$> 680$ 95 28
KHACHATRYAN
2016BJ
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , Tsbot2, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ $<$ 550 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
$> 500$ 95 28
KHACHATRYAN
2016BJ
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , Tsbot2, ${\mathit m}_{{{\widetilde{\mathit b}}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}<$100 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=50 GeV
$> 880$ 95 29
KHACHATRYAN
2016BS
 CMS jets + $\not E_T$, Tsbot1, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
$> 550$ 95 30
KHACHATRYAN
2016BY
 CMS opposite-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , Tsbot3, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 100 GeV
$> 600$ 95 31
AAD
2015CJ
 ATLS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 250 GeV
$> 440$ 95 31
AAD
2015CJ
 ATLS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{(*)}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 60 GeV, ${\mathit m}_{{{\widetilde{\mathit b}}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ $<$ ${\mathit m}_{{{\mathit t}}}$
$\text{none 300 - 650}$ 95 31
AAD
2015CJ
 ATLS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\widetilde{\mathit b}}}{{\mathit b}}{{\widetilde{\mathit \chi}}_{{2}}^{0}}$ , ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit h}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 60 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ $>$ 250 GeV
$> 640$ 95 32
KHACHATRYAN
2015AF
 CMS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0
$> 650$ 95 33
KHACHATRYAN
2015AH
 CMS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0
$> 250$ 95 33
KHACHATRYAN
2015AH
 CMS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit b}}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 10 GeV
$> 570$ 95 34
KHACHATRYAN
2015I
 CMS ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ =50 GeV, 150$<{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}<$300 GeV
$> 255$ 95 35
AAD
2014T
 ATLS ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $\approx{}{\mathit m}_{{{\mathit b}}}$
$> 400$ 95 36
CHATRCHYAN
2014AH
 CMS jets + $\not E_T$, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
37
CHATRCHYAN
2014R
 CMS ${}\geq{}3{{\mathit \ell}^{\pm}}$, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
• • We do not use the following data for averages, fits, limits, etc. • •
38
KHACHATRYAN
2015AD
 CMS ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}$ + jets + $\not E_T$, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\mathit \ell}^{\pm}}{{\mathit \ell}^{\mp}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$
$\text{none 340 - 600}$ 95 39
AAD
2014AX
 ATLS ${}\geq{}$3 ${{\mathit b}}$-jets + $\not E_T$, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{2}}^{0}}$ simplified model with ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit h}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=60 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$=300 GeV
$> 440$ 95 40
AAD
2014E
 ATLS ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$( ${{\mathit \ell}^{\mp}}$) + jets, ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ with ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{(*)\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = 2 ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$
$> 500$ 95 41
CHATRCHYAN
2014H
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ , ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = 2 GeV, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 100 GeV
$\text{> 620}$ 95 42
AAD
2013AU
 ATLS 2 ${{\mathit b}}$-jets + $\not E_T$, ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}<$ 120 GeV
$> 550$ 95 43
CHATRCHYAN
2013AT
 CMS jets + $\not E_T$, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$= 50 GeV
$> 600$ 95 44
CHATRCHYAN
2013T
 CMS jets + $\not E_T$, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$= 0 GeV
$> 450$ 95 45
CHATRCHYAN
2013V
 CMS same-sign ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ + ${}\geq{}$2 ${{\mathit b}}$-jets, ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
$> 390$ 46
AAD
2012AN
 ATLS ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ $<$ 60 GeV
47
CHATRCHYAN
2012AI
 CMS ${{\mathit \ell}^{\pm}}{{\mathit \ell}^{\pm}}$ + ${{\mathit b}}$-jets + $\not E_T$
$> 410$ 95 48
CHATRCHYAN
2012BO
 CMS ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , simplified model, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV
$> 294$ 95 49
AAD
2011K
 ATLS stable ${{\widetilde{\mathit b}}}$
50
AAD
2011O
 ATLS ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\widetilde{\mathit b}}_{{1}}}{{\mathit b}}$ , ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$=60 GeV
51
CHATRCHYAN
2011D
 CMS ${{\widetilde{\mathit b}}}$, ${{\widetilde{\mathit t}}}$ $\rightarrow$ ${{\mathit b}}$
$> 230$ 95 52
AALTONEN
2010R
 CDF ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}<$ 70 GeV
$> 247$ 95 53
ABAZOV
2010L
 D0 ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV
1  AAD 2021AM searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for pair production of bottom squarks in events with hadronically decaying ${{\mathit \tau}^{\pm}}$-leptons, ${{\mathit b}}$-tagged jets, and large $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the bottom squark mass in the Tsbot4 simplified model, assuming ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ $−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 130 GeV, see their Figure 8.
2  AAD 2021S searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for pair production of sbottoms, LQ or dark matter in events with ${{\mathit b}}$-jets and $\not E_T$, also using dedicated secondary-vertex-finding techniques. No significant excess above the Standard Model predictions is observed. Limits are set on ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}$ in the Tsbot1 simplified model, on the LQ masses depending on the BR in ${{\mathit b}}{{\mathit \nu}}$ , on scalar and pseudoscalar dark matter mediator masses. See Figures 8, 9, 10.
3  SIRUNYAN 2021M searched in 137 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for supersymmetry in events with two opposite-sign same-flavor leptons (electrons, muons) and $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the simplified model Tglu4C, see their Figure 10, on the ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ and ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ mass in Tchi1n2Fa, see their Figure 11, on the ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ mass in Tn1n1C and Tn1n1B for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}={\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}={\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$, see their Figure 12. Limits are also set on the light squark mass for the simplified model Tsqk2A, on the sbottom mass in Tsbot3, see their Figure 13, and on the slepton mass in direct electroweak pair production of mass-degenerate left- and right-handed sleptons (selectrons and smuons), see their Figure 14.
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 bottom squark masses in the Tsbot2 simplified model for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + 100 GeV, see their Fig. 8(a).
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  AAD 2019H searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with no charged leptons, three or more ${{\mathit b}}$-jets, and large $\not E_T$. Higgs boson candidates are reconstructed as ${{\mathit b}}$-jet pairs. No significant excess above the Standard Model expectations is observed. Limits up to 1500 GeV are set on the sbottom mass in the Tsbot4 simplified model, see Figure 8(a), for fixed ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 60 GeV and for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ up to 1200 GeV.
7  AAD 2019H searched in 139 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with no charged leptons, three or more ${{\mathit b}}$-jets, and large $\not E_T$. Higgs boson candidates are reconstructed as ${{\mathit b}}$-jet pairs. No significant excess above the Standard Model expectations is observed. Limits up to 1300 GeV are set on the sbottom mass in the Tsbot4 simplified model, see Figure 8(b), for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + 130 GeV and ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{2}}^{0}}}$ from 200 to 750 GeV.
8  SIRUNYAN 2019CH searched in 137 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing multiple jets and large $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu1C, Tglu2A and Tglu3A simplified models, see their Figure 13. Limits are also set on squark, sbottom and stop masses in the Tsqk1, Tsbot1, Tstop1 simplified models, see their Figure 14.
9  SIRUNYAN 2019CI searched in 77.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more high-momentum Higgs bosons, decaying to pairs of photons, jets and $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in the Tsbot4 simplified model, see Figure 3, and on the wino mass in the Tchi1n2E simplified model, see their Figure 4. Limits are also set on the higgsino mass in the Tn1n1A and Tn1n1B simplified models, see their Figure 5.
10  AABOUD 2018I searched in 36.1 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with at least one jet with a transverse momentum above 250 GeV and no leptons. Good agreement is observed between the number of events in data and Standard Model predictions. The results are translated into exclusion limits in Tsbot1 models. In the compressed scenario with sbottom and neutralino masses differing by ${\mathit m}_{{{\mathit b}}}$, sbottom masses below 430 GeV are excluded. For ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 they exclude sbottom masses up to 610 GeV. See their Fig.10(a).
11  SIRUNYAN 2018AL searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with at least three charged leptons, in any combination of electrons and muons, jets and significant $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu3A and Tglu1C simplified models, see their Figure 5. Limits are also set on the sbottom mass in the Tsbot2 simplified model, see their Figure 6, and on the stop mass in the Tstop7 simplified model, see their Figure 7.
12  SIRUNYAN 2018AR searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing two opposite-charge, same-flavour leptons (electrons or muons), jets and $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu4C simplified model, see their Figure 7. Limits are also set on the chargino/neutralino mass in the Tchi1n2F simplified model, see their Figure 8, and on the neutralino mass in the Tn1n1B and Tn1n1C simplified models, see their Figure 9. Finally, limits are set on the sbottom mass in the Tsbot3 simplified model, see their Figure 10.
13  SIRUNYAN 2018AY searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing one or more jets and significant $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu2A and Tglu3A simplified models, see their Figure 3. Limits are also set on squark, sbottom and stop masses in the Tsqk1, Tsbot1, Tstop1 and Tstop4 simplified models, see their Figure 3. Finally, limits are set on long-lived gluino masses in a Tglu1A simplified model where the gluino is metastable or long-lived with proper decay lengths in the range $10^{-3}$ mm $<$ c${{\mathit \tau}}$ $<$ $10^{5}$ mm, see their Figure 4.
14  SIRUNYAN 2018B searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for the pair production of third-generation squarks in events with jets and large $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in the Tsbot1 simplified model, see their Figure 5, and on the stop mass in the Tstop4 simplified model, see their Figure 6.
15  SIRUNYAN 2018X searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more high-momentum Higgs bosons, decaying to pairs of photons, jets and $\not E_T$. The razor variables (${{\mathit M}_{{R}}}$ and ${{\mathit R}^{2}}$) are used to categorise the events. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in the Tsbot4 simplified model and on the wino mass in the Tchi1n2E simplified model, see their Figure 5. Limits are also set on the higgsino mass in the Tn1n1A and Tn1n1B simplified models, see their Figure 6.
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 700 GeV are set on the bottom squark mass in Tsbot2 simplified models assuming ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 GeV. See their Figure 4(d).
17  AABOUD 2017AX searched in 36 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing two jets identified as originating from ${{\mathit b}}$-quarks and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95$\%$ C.L. are set on the masses of bottom squarks. In the Tsbot1 simplified model, a ${{\widetilde{\mathit b}}_{{1}}}$ mass below 950 GeV is excluded for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 ($<$420) GeV. See their Fig. 7(a).
18  AABOUD 2017AX searched in 36 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing two jets identified as originating from ${{\mathit b}}$-quarks and large missing transverse momentum, with or without leptons. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95$\%$ C.L. are set on the masses of bottom squarks. Assuming 50$\%$ BR for Tsbot1 and Tsbot2 simplified models, a ${{\widetilde{\mathit b}}_{{1}}}$ mass below 880 (860) GeV is excluded for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 0 ($<$250) GeV. See their Fig. 7(b).
19  KHACHATRYAN 2017A searched in 18.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with two forward jets, produced through vector boson fusion, and missing transverse momentum. No significant excess above the Standard Model expectations is observed. A limit is set on sbottom masses in the Tsbot1 simplified model, see Fig. 3.
20  KHACHATRYAN 2017AW searched in 2.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with at least three charged leptons, in any combination of electrons and muons, and significant $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu3A and Tglu1C simplified models, and on the sbottom mass in the Tsbot2 simplified model, see their Figure 4.
21  KHACHATRYAN 2017P searched in 2.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more jets and large $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu2A, Tglu3A, Tglu3B, Tglu3C and Tglu3D simplified models, see their Figures 7 and 8. Limits are also set on the squark mass in the Tsqk1 simplified model, see their Fig. 7, and on the sbottom mass in the Tsbot1 simplified model, see Fig. 8. Finally, limits are set on the stop mass in the Tstop1, Tstop3, Tstop4, Tstop6 and Tstop7 simplified models, see Fig. 8.
22  SIRUNYAN 2017AZ searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with one or more jets and large $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu1A, Tglu2A, Tglu3A simplified models, see their Figures 6. Limits are also set on the squark mass in the Tsqk1 simplified model (for single light squark and for 8 degenerate light squarks), on the sbottom mass in the Tsbot1 simplified model and on the stop mass in the Tstop1 simplified model, see their Fig. 7. Finally, limits are set on the stop mass in the Tstop2, Tstop4 and Tstop8 simplified models, see Fig. 8.
23  SIRUNYAN 2017K searched in 2.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for direct production of stop or sbottom pairs in events with multiple jets and significant $\not E_T$. A second search also requires an isolated lepton and is combined with the all-hadronic search. No significant excess above the Standard Model expectations is observed. Limits are set on the stop mass in the Tstop1, Tstop8 and Tstop4 simplified models, see their Figures 7, 8 and 9 (for the Tstop4 limits, only the results of the all-hadronic search are used). Limits are also set on the sbottom mass in the Tsbot1 simplified model, see Fig. 10 (also here, only the results of the all-hadronic search are used).
24  SIRUNYAN 2017S searched in 35.9 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two isolated same-sign leptons, jets, and large $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on the mass of the gluino mass in the Tglu3A, Tglu3B, Tglu3C, Tglu3D and Tglu1B simplified models, see their Figures 5 and 6, and on the sbottom mass in the Tsbot2 simplified model, see their Figure 6.
25  AABOUD 2016D searched in 3.2 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with an energetic jet and large missing transverse momentum. The results are interpreted as 95$\%$C.L. limits on mass of sbottom decaying into a ${{\mathit b}}$-quark and the lightest neutralino in scenarios with ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}−$ ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ between 5 and 20 GeV. See their Fig. 6.
26  AABOUD 2016Q searched in 3.2 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events containing two jets identified as originating from ${{\mathit b}}$-quarks and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95$\%$ C.L. are set on the masses of third-generation squarks. Assuming that the decay ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ (Tsbot1) takes place 100$\%$ of the time, a ${{\widetilde{\mathit b}}_{{1}}}$ mass below 840 (800) GeV is excluded for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}<$ 100 (360) GeV. Differences in mass above 100 GeV between the ${{\widetilde{\mathit b}}_{{1}}}$ and the ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ are excluded up to a ${{\widetilde{\mathit b}}_{{1}}}$ mass of 500 GeV. For more details, see their Fig. 4.
27  AAD 2016BB searched in 3.2 ${\mathrm {fb}}{}^{-1}$ of pp collisions at $\sqrt {s }$ = 13 TeV for events with exactly two same-sign leptons or at least three leptons, multiple hadronic jets, ${{\mathit b}}$-jets, and $\not E_T$. No significant excess over the Standard Model expectation is found. Exclusion limits at 95$\%$ C.L. are set on the sbottom mass for the Tsbot2 model, assuming ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}}$ = ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ + 100 GeV. See their Fig. 4c.
28  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 sbottom mass in the Tsbot2 simplified model, see Fig. 6.
29  KHACHATRYAN 2016BS searched in 2.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with at least one energetic jet , no isolated leptons, and significant $\not E_T$, using the transverse mass variable ${{\mathit M}_{{T2}}}$ to discriminate between signal and background processes. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in the Tsbot1 simplified model, see Fig. 11 and Table 3.
30  KHACHATRYAN 2016BY searched in 2.3 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV for events with two opposite-sign, same-flavour leptons, jets, and missing transverse momentum. No significant excess above the Standard Model expectations is observed. Limits are set on the gluino mass in the Tglu4C simplified model, see Fig. 4, and on sbottom masses in the Tsbot3 simplified model, see Fig. 5.
31  AAD 2015CJ searched in 20 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for evidence of third generation squarks by combining a large number of searches covering various final states. Limits on the sbottom mass are shown, either assuming the ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}$ ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ decay, see Fig. 11, or assuming the ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ decay, with ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{(*)}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , see Fig. 12a, or assuming the ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{2}}^{0}}$ decay, with ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit h}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , see Fig. 12b. Interpretations in the pMSSM are also discussed, see Figures $13 - 15$.
32  KHACHATRYAN 2015AF searched in 19.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with at least two energetic jets and significant $\not E_T$, using the transverse mass variable ${{\mathit M}_{{T2}}}$ to discriminate between signal and background processes. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in simplified models where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see Fig. 12. See also Table 5. Exclusions in the CMSSM, assuming tan ${{\mathit \beta}}$ = 30, $\mathit A_{0}$ = $−$2 max(${\mathit m}_{\mathrm {0}}$, ${\mathit m}_{\mathrm {1/2}}$) and ${{\mathit \mu}}$ $>$ 0, are also presented, see Fig. 15.
33  KHACHATRYAN 2015AH searched in 19.4 or 19.7 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events containing either a fully reconstructed top quark, or events containing dijets requiring one or both jets to originate from ${\mathit {\mathit b}}$-quarks, or events containing a mono-jet. No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in simplified models where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see Fig. 12. Limits are also set in a simplified model where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit c}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see Fig. 12.
34  KHACHATRYAN 2015I searched in 19.5 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events in which ${\mathit {\mathit b}}$-jets and four ${{\mathit W}}$-bosons are produced. Five individual search channels are combined (fully hadronic, single lepton, same-sign dilepton, opposite-sign dilepton, multilepton). No significant excess above the Standard Model expectations is observed. Limits are set on the sbottom mass in a simplified model where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , with ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , takes place with a branching ratio of 100$\%$, see Fig. 7.
35  AAD 2014T searched in 20.3 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for monojet-like events. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95$\%$ C.L. are set on the masses of third-generation squarks in simplified models which assume that the decay ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place 100$\%$ of the time, see Fig. 12.
36  CHATRCHYAN 2014AH searched in 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for events with at least two energetic jets and significant $\not E_T$, using the razor variables (${{\mathit M}_{{R}}}$ and ${{\mathit R}^{2}}$) to discriminate between signal and background processes. A second analysis requires at least one of the jets to be originating from a ${{\mathit b}}$-quark. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see Figs. 28 and 29. Exclusions in the CMSSM, assuming tan $\beta $ = 10, ${{\mathit A}_{{0}}}$ = 0 and ${{\mathit \mu}}$ $>$0, are also presented, see Fig. 26.
37  CHATRCHYAN 2014R searched in 19.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with at least three 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 a simplified model where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , with ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ , takes place with a branching ratio of 100$\%$, see Fig. 11.
38  KHACHATRYAN 2015AD searched in 19.4 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with two opposite-sign same flavor isolated leptons featuring either a kinematic edge, or a peak at the ${{\mathit Z}}$-boson mass, in the invariant mass spectrum. No evidence for a statistically significant excess over the expected SM backgrounds is observed and 95$\%$ C.L. exclusion limits are derived in a simplified model of sbottom pair production where the sbottom decays into a ${\mathit {\mathit b}}$-quark, two opposite-sign dileptons and a neutralino LSP, through an intermediate state containing either an off-shell ${{\mathit Z}}$-boson or a slepton, see Fig. 8.
39  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 are set in simplified models containing scalar bottom quarks, where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{2}}^{0}}$ and ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$ $\rightarrow$ ${{\mathit h}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see their Figures 11.
40  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 bottom, see Fig. 7. Limits are also derived in the mSUGRA/CMSSM, bRPV and GMSB models, see their Fig. 8.
41  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 sbottom mass in a simplified models where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, with varying mass of the ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$, for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV, see Fig. 6.
42  AAD 2013AU searched in 20.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events containing two jets identified as originating from ${{\mathit b}}$-quarks and large missing transverse momentum. No excess of events above the expected level of Standard Model background was found. Exclusion limits at 95$\%$ C.L. are set on the masses of third-generation squarks. Assuming that the decay ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place 100$\%$ of the time, a ${{\widetilde{\mathit b}}_{{1}}}$ mass below 620 GeV is excluded for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}<$ 120 GeV. For more details, see their Fig. 5.
43  CHATRCHYAN 2013AT provides interpretations of various searches for supersymmetry by the CMS experiment based on $4.73 - 4.98$ fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV in the framework of simplified models. Limits are set on the sbottom mass in a simplified models where sbottom quarks are pair-produced and the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see Fig. 4.
44  CHATRCHYAN 2013T searched in 11.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with at least two energetic jets and significant $\not E_T$, using the ${{\mathit \alpha}_{{T}}}$ variable to discriminate between processes with genuine and misreconstructed $\not E_T$. No significant excess above the Standard Model expectations is observed. Limits are set on sbottom masses in simplified models where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, see Fig. 8 and Table 9.
45  CHATRCHYAN 2013V searched in 10.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV for events with two isolated same-sign dileptons and at least two ${{\mathit b}}$-jets in the final state. No significant excess above the Standard Model expectations is observed. Limits are set on the bottom mass in a simplified models where the decay ${{\widetilde{\mathit b}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ , ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ $\rightarrow$ ${{\mathit W}^{\pm}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ takes place with a branching ratio of 100$\%$, with varying mass of the ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$, for ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 50 GeV, see Fig. 4.
46  AAD 2012AN searched in 2.05 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for scalar bottom quarks in events with large missing transverse momentum and two ${{\mathit b}}$-jets in the final state. The data are found to be consistent with the Standard Model expectations. Limits are set in an R-parity conserving minimal supersymmetric scenario, assuming B( ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ ) = 100$\%$, see their Fig. 2.
47  CHATRCHYAN 2012AI looked in 4.98 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for events with two same-sign leptons (${{\mathit e}}$, ${{\mathit \mu}}$), but not necessarily same flavor, at least 2 ${{\mathit b}}$-jets and missing transverse energy. No excess beyond the Standard Model expectation is observed. Exclusion limits are derived in a simplified model for sbottom pair production, where the sbottom decays through ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit t}}{{\widetilde{\mathit \chi}}_{{1}}}{{\mathit W}}$ , see Fig. 8.
48  CHATRCHYAN 2012BO searched in 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for scalar bottom quarks in events with large missing transverse momentum and two ${{\mathit b}}$-jets in the final state. The data are found to be consistent with the Standard Model expectations. Limits are set in an R-parity conserving minimal supersymmetric scenario, assuming B( ${{\widetilde{\mathit b}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ ) = 100$\%$, see their Fig. 2.
49  AAD 2011K looked in 34 pb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for events with heavy stable particles, identified by their anomalous dE/dx in the tracker or time of flight in the tile calorimeter, from pair production of ${{\widetilde{\mathit b}}}$. No evidence for an excess over the SM expectation is observed and limits on the mass are derived for pair production of sbottom, see Fig. 4.
50  AAD 2011O looked in 35 pb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for events with jets, of which at least one is a ${{\mathit b}}$-jet, and $\not E_T$. No excess above the Standard Model was found. Limits are derived in the (${\mathit m}_{{{\widetilde{\mathit g}}}}$, ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}$) plane (see Fig. 2) under the assumption of 100$\%$ branching ratios and ${{\widetilde{\mathit b}}_{{1}}}$ being the lightest squark. The quoted limit is valid for ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}$ $<$ 500 GeV. A similar approach for ${{\widetilde{\mathit t}}_{{1}}}$ as the lightest squark with ${{\widetilde{\mathit g}}}$ $\rightarrow$ ${{\widetilde{\mathit t}}_{{1}}}{{\mathit t}}$ and ${{\widetilde{\mathit t}}_{{1}}}$ $\rightarrow$ ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$ with 100$\%$ branching ratios leads to a gluino mass limit of 520 GeV for 130 $<$ ${\mathit m}_{{{\widetilde{\mathit t}}_{{1}}}}$ $<$ 300 GeV. Limits are also derived in the CMSSM (${{\mathit m}_{{0}}}$, ${{\mathit m}_{{1/2}}}$) plane for tan ${{\mathit \beta}}$ = 40, see Fig. 4, and in scenarios based on the gauge group SO(10).
51  CHATRCHYAN 2011D looked in 35 pb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV for events with ${}\geq{}$ 2 jets, at least one of which is b-tagged, and $\not E_T$, where the ${{\mathit b}}$-jets are decay products of ${{\widetilde{\mathit t}}}$ or ${{\widetilde{\mathit b}}}$. No evidence for an excess over the expected background is observed. Limits are derived in the CMSSM (${{\mathit m}_{{0}}}$, ${{\mathit m}_{{1/2}}}$) plane for tan ${{\mathit \beta}}$ = 50 (see Fig. 2).
52  AALTONEN 2010R searched in 2.65 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV for events with $\not E_T$ and exactly two jets, at least one of which is ${{\mathit b}}$-tagged. The results are in agreement with the SM prediction, and a limit on the cross section of 0.1 pb is obtained for the range of masses 80 $<$ ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}<$ 280 GeV assuming that the sbottom decays exclusively to ${{\mathit b}}{{\widetilde{\mathit \chi}}_{{1}}^{0}}$ . The excluded mass region in the framework of conserved ${{\mathit R}_{{p}}}$ is shown in a plane of (${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}$, ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$), see their Fig.2.
53  ABAZOV 2010L looked in 5.2 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\sqrt {s }$ = 1.96 TeV for events with at least 2 b-jets and $\not E_T$ from the production of ${{\widetilde{\mathit b}}_{{1}}}{{\widetilde{\mathit b}}_{{1}}}$ . No evidence for an excess over the SM expectation is observed, and a limit on the cross section is derived under the assumption of 100$\%$ branching ratio. The excluded mass region in the framework of conserved ${{\mathit R}_{{p}}}$ is shown in a plane of (${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}},{\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$), see their Fig. 3b. The exclusion also extends to ${\mathit m}_{{{\widetilde{\mathit \chi}}_{{1}}^{0}}}$ = 110 GeV for 160$<$ ${\mathit m}_{{{\widetilde{\mathit b}}_{{1}}}}$ $<$ 200 GeV.
References:
AAD 2021S
JHEP 2105 093 Search for new phenomena in final states with $b$-jets and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector
AAD 2021AM
PR D104 032014 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
SIRUNYAN 2021M
JHEP 2104 123 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
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
AAD 2019H
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SIRUNYAN 2019CH
JHEP 1910 244 Search for supersymmetry in proton-proton collisions at 13 TeV in final states with jets and missing transverse momentum
SIRUNYAN 2019CI
JHEP 1911 109 Search for supersymmetry using Higgs boson to diphoton decays at $\sqrt{s}$ = 13 TeV
AABOUD 2018I
JHEP 1801 126 Search for Dark Matter and other New Phenomena in Events with an Energetic Jet and Large Missing Transverse Momentum using the ATLAS Detector
SIRUNYAN 2018AY
JHEP 1805 025 Search for natural and split supersymmetry in proton-proton collisions at $ \sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum
SIRUNYAN 2018AR
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SIRUNYAN 2018AL
JHEP 1802 067 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
SIRUNYAN 2018X
PL B779 166 Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at $\sqrt{s} = $ 13 TeV
SIRUNYAN 2018B
PL B778 263 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
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
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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 2017AX
JHEP 1711 195 Search for Supersymmetry in Events with ${\mathit {\mathit b}}$-Tagged Jets and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
KHACHATRYAN 2017P
EPJ C77 294 A Search for New Phenomena in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13TeV in Final States with Missing Transverse Momentum and at Least One Jet using the $\alpha _{T}$ Variable
KHACHATRYAN 2017A
PRL 118 021802 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
KHACHATRYAN 2017AW
EPJ C77 635 Search for New Phenomena with Multiple Charged Leptons in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017AZ
EPJ C77 710 Search for New Phenomena with the $\mathit M_{T2}$ Variable in the All-Hadronic Final State Produced in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017S
EPJ C77 578 Search for Physics beyond the Standard Model in Events with Two Leptons of Same Sign, Missing Transverse Momentum, and Jets in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017K
EPJ C77 327 Searches for Pair Production of Third-Generation squarks in $\sqrt {s }$ = 13 TeV ${{\mathit p}}{{\mathit p}}$ Collisions
AABOUD 2016Q
EPJ C76 547 Search for Bottom Squark Pair Production in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
AABOUD 2016D
PR D94 032005 Search for New Phenomena in Final States with an Energetic Jet and Large Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV using the ATLAS Detector
AAD 2016BB
EPJ C76 259 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
KHACHATRYAN 2016BS
JHEP 1610 006 Search for New Physics with the MT2 Variable in all-Jets Final States Produced in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV
KHACHATRYAN 2016BJ
EPJ C76 439 Search for New Physics in Same-sign Dilepton Events in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
KHACHATRYAN 2016BY
JHEP 1612 013 Search for New Physics in Final States with Two Opposite-Sign, Same-Flavor leptons, jets, and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV
AAD 2015CJ
EPJ C75 510 ATLAS Run 1 Searches for Direct Pair Production of Third-Generation Squarks at the Large Hadron Collider
KHACHATRYAN 2015AH
JHEP 1506 116 Searches for Third-Generation Squark Production in Fully Hadronic Final States in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2015AD
JHEP 1504 124 Search for Physics Beyond the Standard Model in Events with Two Leptons, Jets, and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2015AF
JHEP 1505 078 Searches for Supersymmetry using the $\mathit M_{T2}$ Variable in Hadronic Events Produced in ${{\mathit p}}{{\mathit p}}$ Collisions at 8 TeV
KHACHATRYAN 2015I
PL B745 5 Searches for Supersymmetry Based on Events with ${\mathit {\mathit b}}$ Jets and Four ${{\mathit W}}$ Bosons in ${{\mathit p}}{{\mathit p}}$ Collisions at 8 TeV
AAD 2014T
PR D90 052008 Search for Pair-Produced Third-Generation squarks Decaying via Charm Quarks or in Compressed Supersymmetric Scenarios in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV 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
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
CHATRCHYAN 2014R
PR D90 032006 Search for Anomalous Production of Events with Three or More Leptons 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
CHATRCHYAN 2014AH
PR D90 112001 Search for Supersymmetry with Razor Variables in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AAD 2013AU
JHEP 1310 189 Search for Direct Third-Generation Squark Pair Production in Final States with Missing Transverse Momentum and Two ${\mathit {\mathit b}}$-Jets in $\sqrt {s }$ = 8 TeV ${{\mathit p}}{{\mathit p}}$ Collisions with the ATLAS Detector
CHATRCHYAN 2013T
EPJ C73 2568 Search for Supersymmetry in Hadronic Final States with Missing Transverse Energy using the Variables $\alpha _{T}$ and ${\mathit {\mathit b}}$-Quark Multiplicity in ${{\mathit p}}{{\mathit p}}$ Collisions at 8 TeV
CHATRCHYAN 2013V
JHEP 1303 037 Search for New Physics in Events with Same-Sign Dileptons and ${\mathit {\mathit b}}$ Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
Also
JHEP 1307 041 (errat.) Erratum CHATRCHYAN 2013V: Search for New Physics in Events with Same-Sign Dileptons and ${\mathit {\mathit b}}$ Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
CHATRCHYAN 2013AT
PR D88 052017 Interpretation of Searches for Supersymmetry with Simplified Models
AAD 2012AN
PRL 108 181802 Search for Scalar Bottom Quark Pair Production with the ATLAS Detector in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
CHATRCHYAN 2012AI
JHEP 1208 110 Search for New Physics in events with Same-Sign Dileptons and ${\mathit {\mathit b}}$-Tagged Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
CHATRCHYAN 2012BO
JHEP 1212 055 Search for Third-Generation Leptoquarks and Scalar Bottom Quarks in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
AAD 2011O
PL B701 398 Search for Supersymmetry in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV in Final States with Missing Transverse Momentum and ${\mathit {\mathit b}}$-Jets
AAD 2011K
PL B701 1 Search for Stable Hadronising squarks and gluinos with the ATLAS Experiment at the LHC
CHATRCHYAN 2011D
JHEP 1107 113 Search for Supersymmetry in Events with ${\mathit {\mathit b}}$ Jets and Missing Transverse Momentum at the LHC
AALTONEN 2010R
PRL 105 081802 Search for the Production of Scalar Bottom Quarks in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
ABAZOV 2010L
PL B693 95 Search for Scalar Bottom Quarks and Third-Generation Leptoquarks in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV