{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.95683.v1/t47","@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":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","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...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/856499/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/856499/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/856499/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/856499/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/856499/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"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","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.95683.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1821239?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.95683.v1","@type":"Dataset","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.","name":"Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC","url":"https://www.hepdata.net/record/ins1821239?version=1"},"keywords":"ACC, 13000, SUSY, Supersymmetry, Proton-Proton Scattering, RPV, P P --> STOP STOP X","name":"sttN_Eff_8je5bi","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/101625","version":1}