{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.95928.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2182381"}},{"@id":"https://doi.org/10.1140/epjc/s10052-023-11543-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"A search for supersymmetry involving the pair production of gluinos decaying via off-shell third-generation squarks into the lightest neutralino ($\\displaystyle\\tilde\\chi^0_1$) is reported. It exploits LHC proton--proton collision data at a centre-of-mass energy $\\sqrt{s} = 13$ TeV with an integrated luminosity of 139~fb$^{-1}$ collected with the ATLAS detector from 2015 to 2018. The search uses events containing large missing transverse momentum, up to one electron or muon, and several energetic jets, at least three of which must be identified as containing $b$-hadrons. Both a simple kinematic event selection and an event selection based upon a deep neural-network are used. No significant excess above the predicted background is found.  In simplified models involving the pair production of gluinos that decay via off-shell top (bottom) squarks, gluino masses less than 2.44~TeV (2.35~TeV) are excluded at 95\\% CL for a massless $\\displaystyle\\tilde\\chi^0_1$. Limits are also set on the gluino mass in models with variable branching ratios for gluino decays to $b\\bar{b}\\tilde\\chi^0_1$, $t\\bar{t}\\tilde\\chi^0_1$ and $t\\bar{b}\\tilde\\chi^-_1$ / $\\bar{t}b\\tilde\\chi^+_1$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t1","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-0L-B. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_0L_B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t2","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-0L-M1. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_0L_M1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t3","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-0L-M2. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_0L_M2"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t4","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-0L-C. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_0L_C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t5","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-1L-B. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_1L_B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t6","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-1L-M1. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_1L_M1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t7","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-1L-M2. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_1L_M2"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t8","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-1L-C. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_1L_C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t9","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-B. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t10","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-M. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_M"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t11","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-C. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t12","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtb-B. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtb_B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t13","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtb-M. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtb_M"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t14","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtb-C. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtb_C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t15","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-2100-1. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_2100_1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t16","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-1800-1. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_1800_1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t17","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-2300-1200. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_2300_1200"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t18","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gtt-1900-1400. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gtt_1900_1400"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t19","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-2800-1400. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_2800_1400"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t20","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-2300-1000. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_2300_1000"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t21","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-2100-1600. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_2100_1600"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t22","@type":"Dataset","description":"A summary of the uncertainties in the background estimates for SR-Gbb-2000-1800. The individual experimental and theoretical uncertainties are assumed to...","name":"Systematic table for SR_Gbb_2000_1800"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t23","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_0L_B in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-0LB from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t24","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_0L_M1 in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-0LM1 from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t25","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_0L_M2 in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-0LM2 from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t26","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_0L_C in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-0LC from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t27","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_1L_B in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-1LB from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t28","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_1L_M1 in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-1LM1 from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t29","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_1L_M2 in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-1LM2 from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t30","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_1L_C in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtt-1LC from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t31","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_B in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gbb-B from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t32","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_M in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gbb-M from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t33","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_C in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gbb-C from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t34","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtb_B in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtb-B from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t35","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtb_M in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtb-M from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t36","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtb_C in the CC analysis, for both the total expected background yields and...","name":"Yield table for Gtb-C from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t37","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_2100_1 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gtt-2100-1 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t38","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_1800_1 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gtt-1800-1 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t39","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_2300_1200 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gtt-2300-1200 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t40","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gtt_1900_1400 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gtt-1900-1400 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t41","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_2800_1400 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gbb-2800-1400 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t42","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_2300_1000 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gbb-2300-1000 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t43","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_2100_1600 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gbb-2100-1600 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t44","@type":"Dataset","description":"Results of the background-only fit extrapolated to SR_Gbb_2000_1800 in the NN analysis, for both the total expected background yields and...","name":"Yield table for Gbb-2000-1800 from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t45","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the NN analysis. The dashed and...","name":"Observed CLs limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t46","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the NN analysis. The dashed and...","name":"Observed Up CLs limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t47","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the NN analysis. The dashed and...","name":"Observed Down CLs limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t48","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the NN analysis. The dashed and...","name":"Expected CLs limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t49","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the NN analysis. The dashed and...","name":"Expected Up CLs limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t50","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the NN analysis. The dashed and...","name":"Expected Down CLs limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t51","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the NN analysis. The dashed and...","name":"Observed CLs limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t52","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the NN analysis. The dashed and...","name":"Observed Up CLs limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t53","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the NN analysis. The dashed and...","name":"Observed Down CLs limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t54","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the NN analysis. The dashed and...","name":"Expected CLs limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t55","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the NN analysis. The dashed and...","name":"Expected Up CLs limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t56","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the NN analysis. The dashed and...","name":"Expected Down CLs limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t57","@type":"Dataset","description":"Observed (left) 95\\%~CL exclusion limits on the gluino mass as a function of BR$(\\tilde{g} \\to b\\bar{b}\\tilde\\chi^{0}_{1}$) (vertical) and BR$(\\tilde{g} \\to...","name":"Observed gluino limit for m($\\tilde{\\chi}^{0}_{1}$)=1 GeV"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t58","@type":"Dataset","description":"Expected (right) 95\\%~CL exclusion limits on the gluino mass as a function of BR$(\\tilde{g} \\to b\\bar{b}\\tilde\\chi^{0}_{1}$) (vertical) and BR$(\\tilde{g} \\to...","name":"Expected gluino limit for m($\\tilde{\\chi}^{0}_{1}$)=1 GeV"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t59","@type":"Dataset","description":"Observed (left) 95\\%~CL exclusion limits on the gluino mass as a function of BR$(\\tilde{g} \\to b\\bar{b}\\tilde\\chi^{0}_{1}$) (vertical) and BR$(\\tilde{g} \\to...","name":"Observed gluino limit for m($\\tilde{\\chi}^{0}_{1}$)=600 GeV"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t60","@type":"Dataset","description":"Expected (right) 95\\%~CL exclusion limits on the gluino mass as a function of BR$(\\tilde{g} \\to b\\bar{b}\\tilde\\chi^{0}_{1}$) (vertical) and BR$(\\tilde{g} \\to...","name":"Expected gluino limit for m($\\tilde{\\chi}^{0}_{1}$)=600 GeV"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t61","@type":"Dataset","description":"Observed (left) 95\\%~CL exclusion limits on the gluino mass as a function of BR$(\\tilde{g} \\to b\\bar{b}\\tilde\\chi^{0}_{1}$) (vertical) and BR$(\\tilde{g} \\to...","name":"Observed gluino limit for m($\\tilde{\\chi}^{0}_{1}$)=1000 GeV"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t62","@type":"Dataset","description":"Expected (right) 95\\%~CL exclusion limits on the gluino mass as a function of BR$(\\tilde{g} \\to b\\bar{b}\\tilde\\chi^{0}_{1}$) (vertical) and BR$(\\tilde{g} \\to...","name":"Expected gluino limit for m($\\tilde{\\chi}^{0}_{1}$)=1000 GeV"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t63","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the CC analysis. The dashed and...","name":"Observed CLs limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t64","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the CC analysis. The dashed and...","name":"Observed Up CLs limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t65","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the CC analysis. The dashed and...","name":"Observed Down CLs limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t66","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the CC analysis. The dashed and...","name":"Expected CLs limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t67","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the CC analysis. The dashed and...","name":"Expected Up CLs limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t68","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt models obtained from the CC analysis. The dashed and...","name":"Expected Down CLs limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t69","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the CC analysis. The dashed and...","name":"Observed CLs limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t70","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the CC analysis. The dashed and...","name":"Observed Up CLs limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t71","@type":"Dataset","description":"Observed exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the CC analysis. The dashed and...","name":"Observed Down CLs limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t72","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the CC analysis. The dashed and...","name":"Expected CLs limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t73","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the CC analysis. The dashed and...","name":"Expected Up CLs limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t74","@type":"Dataset","description":"Expected exclusion limit in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb models obtained from the CC analysis. The dashed and...","name":"Expected Down CLs limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t75","@type":"Dataset","description":"Upper limit at 95\\% CL on the cross-section times branching ratio (fb) in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb...","name":"Cross-section limit for Gbb from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t76","@type":"Dataset","description":"Upper limit at 95\\% CL on the cross-section times branching ratio (fb) in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gbb...","name":"Cross-section limit for Gbb from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t77","@type":"Dataset","description":"Upper limit at 95\\% CL on the cross-section times branching ratio (fb) in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt...","name":"Cross-section limit for Gtt from CC"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t78","@type":"Dataset","description":"Upper limit at 95\\% CL on the cross-section times branching ratio (fb) in the $\\tilde{g}$--$\\tilde\\chi^0_1$ mass plane for the Gtt...","name":"Cross-section limit for Gtt from NN"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t79","@type":"Dataset","description":"Acceptance for SR-Gtt-0L-B and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-0L-B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t80","@type":"Dataset","description":"Efficiency for SR-Gtt-0L-B and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-0L-B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t81","@type":"Dataset","description":"Acceptance for SR-Gtt-0L-M1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-0L-M1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t82","@type":"Dataset","description":"Efficiency for SR-Gtt-0L-M1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-0L-M1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t83","@type":"Dataset","description":"Acceptance for SR-Gtt-0L-M2 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-0L-M2"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t84","@type":"Dataset","description":"Efficiency for SR-Gtt-0L-M2 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-0L-M2"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t85","@type":"Dataset","description":"Acceptance for SR-Gtt-0L-C and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-0L-C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t86","@type":"Dataset","description":"Efficiency for SR-Gtt-0L-C and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-0L-C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t87","@type":"Dataset","description":"Acceptance for SR-Gtt-1L-B and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-1L-B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t88","@type":"Dataset","description":"Efficiency for SR-Gtt-1L-B and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-1L-B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t89","@type":"Dataset","description":"Acceptance for SR-Gtt-1L-M1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-1L-M1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t90","@type":"Dataset","description":"Efficiency for SR-Gtt-1L-M1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-1L-M1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t91","@type":"Dataset","description":"Acceptance for SR-Gtt-1L-M2 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-1L-M2"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t92","@type":"Dataset","description":"Efficiency for SR-Gtt-1L-M2 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-1L-M2"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t93","@type":"Dataset","description":"Acceptance for SR-Gtt-1L-C and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-1L-C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t94","@type":"Dataset","description":"Efficiency for SR-Gtt-1L-C and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-1L-C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t95","@type":"Dataset","description":"Acceptance for SR-Gbb-B and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t96","@type":"Dataset","description":"Efficiency for SR-Gbb-B and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-B"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t97","@type":"Dataset","description":"Acceptance for SR-Gbb-M and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-M"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t98","@type":"Dataset","description":"Efficiency for SR-Gbb-M and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-M"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t99","@type":"Dataset","description":"Acceptance for SR-Gbb-C and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t100","@type":"Dataset","description":"Efficiency for SR-Gbb-C and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-C"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t101","@type":"Dataset","description":"Acceptance for SR-Gtt-2100-1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-2100-1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t102","@type":"Dataset","description":"Efficiency for SR-Gtt-2100-1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-2100-1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t103","@type":"Dataset","description":"Acceptance for SR-Gtt-1800-1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-1800-1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t104","@type":"Dataset","description":"Efficiency for SR-Gtt-1800-1 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-1800-1"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t105","@type":"Dataset","description":"Acceptance for SR-Gtt-2300-1200 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-2300-1200"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t106","@type":"Dataset","description":"Efficiency for SR-Gtt-2300-1200 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-2300-1200"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t107","@type":"Dataset","description":"Acceptance for SR-Gtt-1900-1400 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gtt-1900-1400"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t108","@type":"Dataset","description":"Efficiency for SR-Gtt-1900-1400 and the $\\tilde{g}\\rightarrow t\\bar{t}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gtt-1900-1400"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t109","@type":"Dataset","description":"Acceptance for SR-Gbb-2800-1400 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-2800-1400"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t110","@type":"Dataset","description":"Efficiency for SR-Gbb-2800-1400 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-2800-1400"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t111","@type":"Dataset","description":"Acceptance for SR-Gbb-2300-1000 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-2300-1000"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t112","@type":"Dataset","description":"Efficiency for SR-Gbb-2300-1000 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-2300-1000"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t113","@type":"Dataset","description":"Acceptance for SR-Gbb-2100-1600 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-2100-1600"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t114","@type":"Dataset","description":"Efficiency for SR-Gbb-2100-1600 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-2100-1600"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t115","@type":"Dataset","description":"Acceptance for SR-Gbb-2000-1800 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"acceptance SR-Gbb-2000-1800"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t116","@type":"Dataset","description":"Efficiency for SR-Gbb-2000-1800 and the $\\tilde{g}\\rightarrow b\\bar{b}\\tilde\\chi^0_1$ signal process.","name":"efficiency SR-Gbb-2000-1800"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t117","@type":"Dataset","description":"Cutflow for the SR-Gtt-0L-B for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-0L-B and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t118","@type":"Dataset","description":"Cutflow for the SR-Gtt-0L-M1 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-0L-M1 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t119","@type":"Dataset","description":"Cutflow for the SR-Gtt-0L-M2 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-0L-M2 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t120","@type":"Dataset","description":"Cutflow for the SR-Gtt-0L-C for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-0L-C and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t121","@type":"Dataset","description":"Cutflow for the SR-Gtt-1L-B for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-1L-B and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t122","@type":"Dataset","description":"Cutflow for the SR-Gtt-1L-M1 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-1L-M1 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t123","@type":"Dataset","description":"Cutflow for the SR-Gtt-1L-M2 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-1L-M2 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t124","@type":"Dataset","description":"Cutflow for the SR-Gtt-1L-C for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-1L-C and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t125","@type":"Dataset","description":"Cutflow for the SR-Gbb-B for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-B and sample Gbb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t126","@type":"Dataset","description":"Cutflow for the SR-Gbb-M for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-M and sample Gbb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t127","@type":"Dataset","description":"Cutflow for the SR-Gbb-C for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-C and sample Gbb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t128","@type":"Dataset","description":"Cutflow for the SR-Gtb-B for a representative Gtb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtb-B and sample Gtb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t129","@type":"Dataset","description":"Cutflow for the SR-Gtb-M for a representative Gtb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtb-M and sample Gtb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t130","@type":"Dataset","description":"Cutflow for the SR-Gtb-C for a representative Gtb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtb-C and sample Gtb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t131","@type":"Dataset","description":"Cutflow for the SR-Gtt-2100-1 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-2100-1 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t132","@type":"Dataset","description":"Cutflow for the SR-Gtt-1800-1 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-1800-1 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t133","@type":"Dataset","description":"Cutflow for the SR-Gtt-2300-1200 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-2300-1200 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t134","@type":"Dataset","description":"Cutflow for the SR-Gtt-1900-1400 for a representative Gtt signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gtt-1900-1400 and sample Gtt"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t135","@type":"Dataset","description":"Cutflow for the SR-Gbb-2800-1400 for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-2800-1400 and sample Gbb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t136","@type":"Dataset","description":"Cutflow for the SR-Gbb-2300-1000 for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-2300-1000 and sample Gbb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t137","@type":"Dataset","description":"Cutflow for the SR-Gbb-2100-1600 for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-2100-1600 and sample Gbb"},{"@id":"https://doi.org/10.17182/hepdata.95928.v2/t138","@type":"Dataset","description":"Cutflow for the SR-Gbb-2000-1800 for a representative Gbb signal. Signal was generated with 30000 events. Expected yields are normalised to...","name":"Cutflow for SR-Gbb-2000-1800 and sample Gbb"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2182381?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/95928"}],"inLanguage":"en","name":"Search for supersymmetry in final states with missing transverse momentum and three or more $b$-jets in 139 fb$^{-1}$ of proton$-$proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2182381?version=2","version":2}