{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.58020.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/939560"}},{"@id":"https://doi.org/10.1140/epjc/s10052-011-1828-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"1970","description":"CERN-LHC. Measurement of the properties of four-jet events produced in proton-proton  collisions at a centre-of-mass energy of 7 TeV in the search for pair-produced scalar particles,  in particular scalar gluons.  Distributions as a function of the average invariant masses of   di-jet pairs are presented as well of several other variables.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t1","@type":"Dataset","description":"The distributions of the momentum of the 4th jet.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t2","@type":"Dataset","description":"The di-jet delta(R) distribution for the sgluon candidate with the highest PT jet after applying the PT cut of 55...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t3","@type":"Dataset","description":"The distribution in relative mass difference of the two sgluon candidates after application of the PT and di-jet delta(R) cuts.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t4","@type":"Dataset","description":"The scattering angle in the 4-jet centre-of-mass frame after all other cuts.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t5","@type":"Dataset","description":"Number of events as a function of the average mass of the reconstructed dijet pairs for jet masses > 55...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t6","@type":"Dataset","description":"Number of events as a function of the average mass of the reconstructed dijet pairs for jet masses > 77...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t7","@type":"Dataset","description":"Number of events as a function of the average mass of the reconstructed dijet pairs for jet masses > 88...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t8","@type":"Dataset","description":"Number of events as a function of the average mass of the reconstructed dijet pairs for jet masses > 104...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.58020.v1/t9","@type":"Dataset","description":"The observed 95% CL upper bounds on scalar pair production cross-section as a function of the scalar particle mass.","name":"Table 9"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins939560?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/58020"}],"inLanguage":"en","name":"Search for Massive Colored Scalars in Four-Jet Final States in sqrt{s}=7 TeV proton-proton collisions with the ATLAS Detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins939560?version=1","version":1}