{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.67127.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1357199"}},{"@id":"https://doi.org/10.1007/JHEP07(2015)032","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2016","description":"CERN-LHC.  We search for evidence of physics beyond the Standard Model in the production of final states with multiple high transverse momentum jets, using 20.3 fb$^{-1}$ of proton-proton collision data recorded by the ATLAS detector at $\\sqrt{s} = 8$ TeV. No excess of events beyond Standard Model expectations is observed, and upper limits on the visible cross-section for non-Standard Model production of multi-jet final states are set. Using a wide variety of models for black hole and string ball production and decay, the limit on the cross-section times acceptance is as low as 0.16 fb at the 95% CL for a minimum scalar sum of jet transverse momentum in the event of about 4.3 TeV. Using models for black hole and string ball production and decay, exclusion contours are determined as a function of the production mass threshold and the gravity scale. These limits can be interpreted in terms of lower-mass limits on black hole and string ball production that range from 4.6 to 6.2 TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t1","@type":"Dataset","description":"Number of data events (20.3 fb$^{-1}$), number of predicted events from the fit, statistical uncertainty on the fit, systematic uncertainty...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t2","@type":"Dataset","description":"Number of data events (20.3 fb$^{-1}$), number of predicted events from the fit, statistical uncertainty on the fit, systematic uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t3","@type":"Dataset","description":"Number of data events (20.3 fb$^{-1}$), number of predicted events from the fit, statistical uncertainty on the fit, systematic uncertainty...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t4","@type":"Dataset","description":"Number of data events (20.3 fb$^{-1}$), number of predicted events from the fit, statistical uncertainty on the fit, systematic uncertainty...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t5","@type":"Dataset","description":"Number of data events (20.3 fb$^{-1}$), number of predicted events from the fit, statistical uncertainty on the fit, systematic uncertainty...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t6","@type":"Dataset","description":"Number of data events (20.3 fb$^{-1}$), number of predicted events from the fit, statistical uncertainty on the fit, systematic uncertainty...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t7","@type":"Dataset","description":"Upper limits on the visible cross section (cross section ($\\sigma$) times acceptance ($A$) times efficiency ($\\epsilon$)) at the 95% CL...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t8","@type":"Dataset","description":"Upper limits on the visible cross section (cross section ($\\sigma$) times acceptance ($A$) times efficiency ($\\epsilon$)) at the 95% CL...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t9","@type":"Dataset","description":"Upper limits on the visible cross section (cross section ($\\sigma$) times acceptance ($A$) times efficiency ($\\epsilon$)) at the 95% CL...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t10","@type":"Dataset","description":"Upper limits on the visible cross section (cross section ($\\sigma$) times acceptance ($A$) times efficiency ($\\epsilon$)) at the 95% CL...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t11","@type":"Dataset","description":"Upper limits on the visible cross section (cross section ($\\sigma$) times acceptance ($A$) times efficiency ($\\epsilon$)) at the 95% CL...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t12","@type":"Dataset","description":"Upper limits on the visible cross section (cross section ($\\sigma$) times acceptance ($A$) times efficiency ($\\epsilon$)) at the 95% CL...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.67127.v1/t13","@type":"Dataset","description":"Mean reconstruction efficiencies $(\\epsilon)$ and RMS of the reconstruction efficiencies for various black hole and string ball models.","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1357199?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/67127"}],"inLanguage":"en","name":"Search for low-scale gravity signatures in multi-jet final states with the ATLAS detector at $\\sqrt{s} = 8$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1357199?version=1","version":1}