{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.95683.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1821239"}},{"@id":"https://doi.org/10.1140/epjc/s10052-020-08730-0","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"A search is presented for new phenomena in events characterised by high jet multiplicity, no leptons (electrons or muons), and four or more jets originating from the fragmentation of $b$-quarks ($b$-jets). The search uses 139 fb$^{-1}$ of $\\sqrt{s}$ = 13 TeV proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider during Run 2. The dominant Standard Model background originates from multijet production and is estimated using a data-driven technique based on an extrapolation from events with low $b$-jet multiplicity to the high $b$-jet multiplicities used in the search. No significant excess over the Standard Model expectation is observed and 95% confidence-level limits that constrain simplified models of R-parity-violating supersymmetry are determined. The exclusion limits reach 950 GeV in top-squark mass in the models considered.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t1","@type":"Dataset","description":"- - - - - - - - Overview of HEPData Record - - - - - - - -...","name":"Overview"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t2","@type":"Dataset","description":"The observed exclusion contour at 95% CL as a function of the $\\it{m}_{\\tilde{\\chi}^{\\pm}_{1}}$ vs. $\\it{m}_{\\tilde{t}}$. Masses that are within the...","name":"stbchionly_obs"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t3","@type":"Dataset","description":"The expected exclusion contour at 95% CL as a function of the $\\it{m}_{\\tilde{\\chi}^{\\pm}_{1}}$ vs. $\\it{m}_{\\tilde{t}}$. Masses that are within the...","name":"stbchionly_exp"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t4","@type":"Dataset","description":"The observed exclusion contour at 95% CL as a function of the $\\it{m}_{\\tilde{\\chi}^{0}_{1}}$ vs. $\\it{m}_{\\tilde{t}}$. Masses that are within the...","name":"stbchi_obs"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t5","@type":"Dataset","description":"The expected exclusion contour at 95% CL as a function of the $\\it{m}_{\\tilde{\\chi}^{0}_{1}}$ vs. $\\it{m}_{\\tilde{t}}$. Masses that are within the...","name":"stbchi_exp"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t6","@type":"Dataset","description":"The observed exclusion contour at 95% CL as a function of the $\\it{m}_{\\tilde{\\chi}^{0}_{1}}$ vs. $\\it{m}_{\\tilde{t}}$. Masses that are within the...","name":"sttN_obs"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t7","@type":"Dataset","description":"The expected exclusion contour at 95% CL as a function of the $\\it{m}_{\\tilde{\\chi}^{0}_{1}}$ vs. $\\it{m}_{\\tilde{t}}$. Masses that are within the...","name":"sttN_exp"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t8","@type":"Dataset","description":"Observed model-dependent upper limit on the cross section for the $(\\tilde{t},\\tilde{\\chi}^{\\pm}_{1})$ signal grid. Limits are shown for $B(\\tilde{t} \\rightarrow b...","name":"stbchionly_xSecUL_obs"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t9","@type":"Dataset","description":"Observed model-dependent upper limit on the cross section for the $(\\tilde{t},\\tilde{\\chi}^{\\pm}_{1} / \\tilde{\\chi}^{0}_{1,2})$ signal grid. Limits are shown in the...","name":"stop_xSecUL_obs"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t10","@type":"Dataset","description":"Expected model-dependent upper limit on the cross section for the $(\\tilde{t},\\tilde{\\chi}^{\\pm}_{1})$ signal grid. Limits are shown for $B(\\tilde{t} \\rightarrow b...","name":"stbchionly_xSecUL_exp"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t11","@type":"Dataset","description":"Expected model-dependent upper limit on the cross section for the $(\\tilde{t},\\tilde{\\chi}^{\\pm}_{1} / \\tilde{\\chi}^{0}_{1,2})$ signal grid. Limits are shown in the...","name":"stop_xSecUL_exp"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t12","@type":"Dataset","description":"Expected background and observed number of events in different jet and $b$-tag multiplicity bins.","name":"SR_yields"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t13","@type":"Dataset","description":"Cut flow for a model of top-squark pair production with the top squark decaying to a $b$-quark and a chargino....","name":"cutflow"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t14","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_6je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t15","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_7je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t16","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_8je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t17","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_9ji4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t18","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_6je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t19","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_7je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t20","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_8je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t21","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_9ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t22","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the acceptance given in the...","name":"stbchi_Acc_8ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t23","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_6je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t24","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_7je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t25","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_8je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t26","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_9ji4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t27","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_6je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t28","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_7je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t29","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_8je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t30","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_9ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t31","@type":"Dataset","description":"Signal efficiency for $\\tilde{t} \\rightarrow b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the efficiency given in the...","name":"stbchi_Eff_8ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t32","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_6je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t33","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_7je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t34","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_8je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t35","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_9ji4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t36","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_6je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t37","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_7je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t38","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_8je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t39","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_9ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t40","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Acc_8ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t41","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_6je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t42","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_7je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t43","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_8je4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t44","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_9ji4be"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t45","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_6je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t46","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_7je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t47","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_8je5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t48","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_9ji5bi"},{"@id":"https://doi.org/10.17182/hepdata.95683.v1/t49","@type":"Dataset","description":"Signal acceptance for $\\tilde{t} \\rightarrow t\\tilde{\\chi}^{0}_{1,2}(\\tilde{\\chi}^{0}_{1,2} \\rightarrow tbs) / b\\tilde{\\chi}^{+}_{1}(\\tilde{\\chi}^{+}_{1} \\rightarrow \\bar{b}\\bar{b}\\bar{s}) $ and c.c. model. Please mind that the...","name":"sttN_Eff_8ji5bi"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1821239?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/95683"}],"inLanguage":"en","name":"Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1821239?version=1","version":1}