{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79059.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1631641"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-5693-4","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"A search for massive coloured resonances which are pair-produced and decay into two jets is presented. The analysis uses 36.7 fb$^{-1}$ of $\\sqrt{s}=$ 13 TeV pp collision data recorded by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the background prediction is observed. Results are interpreted in a SUSY simplified model where the lightest supersymmetric particle is the top squark, $\\tilde{t}$, which decays promptly into two quarks through $R$-parity-violating couplings. Top squarks with masses in the range 100 GeV < $m_{\\tilde{t}}$ < 410 GeV are excluded at 95% confidence level. If the decay is into a $b$-quark and a light quark, a dedicated selection requiring two $b$-tags is used to exclude masses in the ranges 100 GeV < $m_{\\tilde{t}}$ < 470 GeV and 480 GeV < $m_{\\tilde{t}}$ < 610 GeV. Additional limits are set on the pair-production of massive colour-octet resonances.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t1","@type":"Dataset","description":"- - - - - - - - - - - - - - - - - - - -...","name":"Overview"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t2","@type":"Dataset","description":"Cutflow table for a pair produced top squark of 100 GeV decaying into a b- and an s-quark.","name":"Cutflow Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t3","@type":"Dataset","description":"Cutflow table for a pair produced top squark of 500 GeV decaying into a b- and an s-quark.","name":"Cutflow Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t4","@type":"Dataset","description":"Cutflow table for a pair produced coloron of 1500 GeV decaying into two quarks.","name":"Cutflow Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t5","@type":"Dataset","description":"The observed number of data, background and top squark signal events in each of the signal regions of the inclusive...","name":"SR distribution 1"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t6","@type":"Dataset","description":"The observed number of data, background and coloron signal events in each of the signal regions of the inclusive selection","name":"SR distribution 2"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t7","@type":"Dataset","description":"The observed number of data, background and top squark signal events in each of the signal regions of the b-tagged...","name":"SR distribution 3"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t8","@type":"Dataset","description":"Signal acceptance and efficiency (in %) as a function of M(STOP), before mass windows","name":"Acceptance 1"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t9","@type":"Dataset","description":"Signal acceptance (in %) and efficiency as a function of M(STOP), after mass windows","name":"Acceptance 2"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t10","@type":"Dataset","description":"Signal acceptance and efficiency (in %) as a function of M(RHO), before mass windows","name":"Acceptance 3"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t11","@type":"Dataset","description":"Signal acceptance and efficiency (in %) as a function of M(RHO), after mass windows","name":"Acceptance 4"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t12","@type":"Dataset","description":"Signal acceptance (in %) and efficiency as a function of M(STOP), before mass windows","name":"Acceptance 5"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t13","@type":"Dataset","description":"Signal acceptance (in %) and efficiency as a function of M(STOP), after mass windows","name":"Acceptance 6"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t14","@type":"Dataset","description":"Cross section excluded at 95% CL as a function of the top squark mass, for a pair produced top squark...","name":"Limit on cross section 1"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t15","@type":"Dataset","description":"Cross section excluded at 95% CL as a function of the cooron mass, for a pair produced coloron with decays...","name":"Limit on cross section 2"},{"@id":"https://doi.org/10.17182/hepdata.79059.v1/t16","@type":"Dataset","description":"Cross section excluded at 95% CL as a function of the top squark mass, for a pair produced top squark...","name":"Limit on cross section 3"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1631641?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79059"}],"inLanguage":"en","name":"A search for pair-produced resonances in four-jet final states 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/ins1631641?version=1","version":1}