{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.66572.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1305096"}},{"@id":"https://doi.org/10.1103/PhysRevD.91.052007","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2015","description":"Dijet events produced in LHC proton--proton collisions at a center-of-mass energy $\\sqrt{s}=8$ TeV are studied with the ATLAS detector using the full 2012 data set, with an integrated luminosity of 20.3 fb$^{-1}$. Dijet masses up to about 4.5 TeV are probed. No resonance-like features are observed in the dijet mass spectrum. Limits on the cross section times acceptance are set at the 95% credibility level for various hypotheses of new phenomena in terms of mass or energy scale, as appropriate. This analysis excludes excited quarks with a mass below 4.06 TeV, color-octet scalars with a mass below 2.70 TeV, heavy $W'$ bosons with a mass below 2.45 TeV, chiral ${W^{\\ast}}$ bosons with a mass below 1.75 TeV, and quantum black holes with six extra space-time dimensions with threshold mass below 5.66 TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t1","@type":"Dataset","description":"The reconstructed dijet mass distribution (observed) fitted with a smooth functional form (expected) of 4-parameter or 5-parameter.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t2","@type":"Dataset","description":"Dijet mass resolution obtained from fully simulated PYTHIA QCD Monte Carlo PYTHIA 8.175 [43], with the AU2 tune obtained from...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t3","@type":"Dataset","description":"Total cross sections, branching ratios in qg only and acceptances for qg, qgamma, qW, qZ decays (A) for the q*...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t4","@type":"Dataset","description":"Total cross sections (cross section), branching ratios (BR(gg)) and acceptances (A) for decays in gg, for the S8 model.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t5","@type":"Dataset","description":"Total cross sections (cross section),next-to-next-to-leading order k-factors, branching ratios (BR(qqbar prime)) and acceptances for decays in q anti-q prime only...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t6","@type":"Dataset","description":"Total cross sections (cross section), branching ratios (BR(qqbar prime)) and acceptances for decays in q anti-q prime only (A) for...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t7","@type":"Dataset","description":"Total cross sections (cross section), branching ratios (BR(qqbar prime)) and acceptances for all decays (A) for the W* leptophilic model.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t8","@type":"Dataset","description":"Total cross sections (cross section), branching ratios only involving q and g (BR(q/g)) and acceptances for all decays into jets...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t9","@type":"Dataset","description":"Total cross sections (cross section), branching ratios only involving q and g (BR(q/g)) and acceptances for all decays into jets...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t10","@type":"Dataset","description":"Observed limit on cross section times acceptance for each width and mass of Gaussian signal shape tested.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t11","@type":"Dataset","description":"Observed limit on cross section times acceptance for each intrinsic width and mass of Breit-Wigner signal shape tested. The limits...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t12","@type":"Dataset","description":"Observed limit on cross section times acceptance for each intrinsic width and mass of Breit-Wigner signal shape tested. The limits...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t13","@type":"Dataset","description":"Observed limit on cross section times acceptance for each intrinsic width and mass of Breit-Wigner signal shape tested. The limits...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.66572.v1/t14","@type":"Dataset","description":"Observed limit on cross section times acceptance for each intrinsic width and mass of Breit-Wigner signal shape tested. The limits...","name":"Table 14"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1305096?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/66572"}],"inLanguage":"en","name":"Search for new phenomena in the dijet mass distribution using $p-p$ collision data at $\\sqrt{s}=8$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1305096?version=1","version":1}