{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.66764.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1340084"}},{"@id":"https://doi.org/10.1103/PhysRevD.91.052009","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2015","description":"A search for resonances and quantum black holes is performed using the dijet mass spectra measured in proton-proton collisions at $\\sqrt{s}$=8 TeV with the CMS detector at the LHC. The data set corresponds to an integrated luminosity of 19.7 fb$^{-1}$. In a search for narrow resonances that couple to quark-quark, quark-gluon, or gluon-gluon pairs, model-independent upper limits, at 95% confidence level, are obtained on the production cross section of resonances, with masses above 1.2 TeV. When interpreted in the context of specific models the limits exclude: string resonances with masses below 5.0 TeV; excited quarks below 3.5 TeV; scalar diquarks below 4.7 TeV; W.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t1","@type":"Dataset","description":"Inclusive dijet mass spectrum from wide jets (points) compared to a fit (solid curve) and to predictions including detector simulation...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t2","@type":"Dataset","description":"Observed 95% CL upper limits on $\\sigma B A$ for narrow qq, qg, and gg resonances, from the inclusive analysis...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t3","@type":"Dataset","description":"Observed 95% CL upper limits on $\\sigma B A$ for narrow gg/bb, qq/bb, and bg resonances from the b-enriched analysis,...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t4","@type":"Dataset","description":"Observed and expected 95% CL exclusions on the mass of various resonances. Systematic uncertainties are taken into account. For excited...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t5","@type":"Dataset","description":"Observed 95% CL upper limits on $\\sigma B A$ as a function of resonance mass for several values of the...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t6","@type":"Dataset","description":"Observed 95% CL upper limits on $\\sigma B A$ as a function of resonance mass for several values of the...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t7","@type":"Dataset","description":"Observed 95% CL upper limits on $\\sigma B A$ for QBHs from the inclusive analysis. These limits are valid for...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t8","@type":"Dataset","description":"Observed 95% CL lower limits on ${M_{QBH}}^{min}$ for different numbers of extra dimensions n and several values of M$_{D}$.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t9","@type":"Dataset","description":"Correction factors defined as the ratio of the full cross section obtained from Eqs. (5)-(7) to the cross section from...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.66764.v1/t10","@type":"Dataset","description":"Correction factors defined as the ratio of the full cross section obtained from Eqs. (5)-(7) to the cross section from...","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1340084?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/66764"}],"inLanguage":"en","name":"Search for resonances and quantum black holes using dijet mass spectra in proton-proton collisions at sqrt(s)=8 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1340084?version=1","version":1}