{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77491.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1597123"}},{"@id":"https://doi.org/10.1007/JHEP09(2017)088","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"CERN-LHC. A search for new phenomena in final states characterized by high jet multiplicity, an isolated lepton (electron or muon) and either zero or at least three b-tagged jets is presented. \nThe search uses 36.1 fb-1 of sqrt(s) = 13 TeV proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider in 2015 and 2016. The dominant sources of background are estimated using parameterized extrapolations, based on observables at medium jet multiplicity, to predict the b-tagged jet multiplicity distribution at the higher jet multiplicities used in the search. No significant excess over the Standard Model expectation is observed and 95% confidence-level limits are extracted constraining four simplified models of R-parity-violating supersymmetry that feature either gluino or top-squark pair production. \nThe exclusion limits reach as high as 2.1 TeV in gluino mass and 1.2 TeV in top-squark mass in the models considered. In addition, an upper limit is set on the cross-section for Standard Model tttt production of 60 fb (6.5 times the Standard Model prediction) at 95% confidence level. Finally, model-independent limits are set on the contribution from new phenomena to the signal-region yields.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t1","@type":"Dataset","description":"The expected background and observed data with five jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t2","@type":"Dataset","description":"The expected background and observed data with six jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t3","@type":"Dataset","description":"The expected background and observed data with seven jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t4","@type":"Dataset","description":"The expected background and observed data with eight jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t5","@type":"Dataset","description":"The expected background and observed data with nine jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t6","@type":"Dataset","description":"The expected background and observed data with ten jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t7","@type":"Dataset","description":"The expected background and observed data with eleven jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t8","@type":"Dataset","description":"The expected background and observed data with twelve-or-more jets in the different b-tag multiplicity bins for the 40 GeV jet...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t9","@type":"Dataset","description":"The expected background and observed data with five jets in the different b-tag multiplicity bins for the 60 GeV jet...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t10","@type":"Dataset","description":"The expected background and observed data with six jets in the different b-tag multiplicity bins for the 60 GeV jet...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t11","@type":"Dataset","description":"The expected background and observed data with seven jets in the different b-tag multiplicity bins for the 60 GeV jet...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t12","@type":"Dataset","description":"The expected background and observed data with eight jets in the different b-tag multiplicity bins for the 60 GeV jet...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t13","@type":"Dataset","description":"The expected background and observed data with nine jets in the different b-tag multiplicity bins for the 60 GeV jet...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t14","@type":"Dataset","description":"The expected background and observed data with ten-or-more jets in the different b-tag multiplicity bins for the 60 GeV jet...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t15","@type":"Dataset","description":"The expected background and observed data with five jets in the different b-tag multiplicity bins for the 80 GeV jet...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t16","@type":"Dataset","description":"The expected background and observed data with six jets in the different b-tag multiplicity bins for the 80 GeV jet...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t17","@type":"Dataset","description":"The expected background and observed data with seven jets in the different b-tag multiplicity bins for the 80 GeV jet...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t18","@type":"Dataset","description":"The expected background and observed data with eight jets in the different b-tag multiplicity bins for the 80 GeV jet...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t19","@type":"Dataset","description":"The expected background and observed data with nine jets in the different b-tag multiplicity bins for the 80 GeV jet...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t20","@type":"Dataset","description":"The expected background and observed data with ten-or-more jets in the different b-tag multiplicity bins for the 80 GeV jet...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t21","@type":"Dataset","description":"Observed exclusion contours on the gluino and neutralino masses in a model where the gluino decays via a virtual top...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t22","@type":"Dataset","description":"Expected exclusion contours on the gluino and neutralino masses in a model where the gluino decays via a virtual top...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t23","@type":"Dataset","description":"Observed exclusion contours on the gluino and stop masses in a model where the gluino decays to a top quark...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t24","@type":"Dataset","description":"Expected exclusion contours on the gluino and stop masses in a model where the gluino decays to a top quark...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t25","@type":"Dataset","description":"Observed exclusion contours on the gluino and neutralino masses in a model with a gluino decaying to two light quarks...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t26","@type":"Dataset","description":"Expected exclusion contours on the gluino and neutralino masses in a model with a gluino decaying to two light quarks...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t27","@type":"Dataset","description":"Observed exclusion contours on the stop and neutralino masses in a model where the stop decays to a third-generation quark...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t28","@type":"Dataset","description":"Expected exclusion contours on the stop and neutralino masses in a model where the stop decays to a third-generation quark...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t29","@type":"Dataset","description":"Observed exclusion contours on the stop and neutralino masses in a model where the stop decays to a top and...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t30","@type":"Dataset","description":"Expected exclusion contours on the stop and neutralino masses in a model where the stop decays to a top and...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t31","@type":"Dataset","description":"Observed upper limits on the model cross-section in units of pb as a function of the gluino and neutralino masses...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t32","@type":"Dataset","description":"Observed upper limits on the model cross-section in units of pb as a function of the gluino and stop masses...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t33","@type":"Dataset","description":"Observed upper limits on the model cross-section in units of pb as a function of the gluino and neutralino masses...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t34","@type":"Dataset","description":"Observed upper limits on the model cross-section in units of pb as a function of the stop and neutralino masses...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t35","@type":"Dataset","description":"Observed upper limits on the model cross-section in units of pb as a function of the stop and neutralino masses...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t36","@type":"Dataset","description":"Acceptance as a function of the gluino and stop masses in a model where the gluino decays to a top...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t37","@type":"Dataset","description":"Efficiency as a function of the gluino and stop masses in a model where the gluino decays to a top...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t38","@type":"Dataset","description":"Acceptance as a function of the gluino and neutralino masses in a model with a gluino decaying to two light...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t39","@type":"Dataset","description":"Efficiency as a function of the gluino and neutralino masses in a model with a gluino decaying to two light...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t40","@type":"Dataset","description":"Cut flow for a model of gluino pair production where the gluino decays to two (u, d, s, c) quarks...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t41","@type":"Dataset","description":"Cut flow for a model of gluino pair production where each gluino decays to a top quark and a top...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t42","@type":"Dataset","description":"Cut flow for a model of gluino pair production where each gluino decays via an off-shell top squark to two...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.77491.v3/t43","@type":"Dataset","description":"Cut flow for a model of right-handed top squark pair production with the top squark decaying to the lightest supersymmetric...","name":"Table 43"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1597123?version=3"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77491"}],"inLanguage":"en","name":"Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using $\\sqrt{s}$ = 13 Tev proton-proton collision data","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1597123?version=3","version":3}