{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.159438.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3073143"}},{"@id":"https://doi.org/10.1007/JHEP04(2026)133","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2025","description":"A search is presented for narrow resonances, with a mass between 0.6 and 1.8 TeV, decaying to pairs of jets, in proton-proton collisions at $\\sqrt{s}=13$ TeV. The search is performed using dijets that are reconstructed, selected, and recorded in a compact form by the high-level trigger in a technique referred to as \"data scouting\", from data collected in 2016$-$18 corresponding to an integrated luminosity of 117 fb$^{-1}$. The dijet mass spectra are well described by a smooth parameterization, and no significant evidence for the production of new particles is observed. Model-independent upper limits are presented on the product of the cross section, branching fraction, and acceptance for the individual cases of narrow quark-quark, quark-gluon, and gluon-gluon resonances, and are compared to the predictions from a variety of models of narrow dijet resonance production. The upper limit on the coupling of a dark matter mediator to quarks is presented as a function of the mediator mass. The sensitivity of this search goes beyond what is expected from statistical scaling with luminosity alone, as a consequence of the use of fewer parameters in the background function within a more robust statistical procedure.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t1","@type":"Dataset","description":"Observed differential dijet spectrum using the 2016 data.","name":"Differential dijet spectrum (2016)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t2","@type":"Dataset","description":"Observed differential dijet spectrum using the 2017 data.","name":"Differential dijet spectrum (2017)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t3","@type":"Dataset","description":"Observed differential dijet spectrum using the 2018 data.","name":"Differential dijet spectrum (2018)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t4","@type":"Dataset","description":"Observed differential dijet spectrum using full Run-2 data.","name":"Differential dijet spectrum (Run-2)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t5","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for quark-quark type...","name":"Cross-section limits (quark-quark)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t6","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for quark-gluon type...","name":"Cross-section limits (quark-gluon)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t7","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for gluon-gluon type...","name":"Cross-section limits (gluon-gluon)"},{"@id":"https://doi.org/10.17182/hepdata.159438.v1/t8","@type":"Dataset","description":"The observed and expected 95% CL upper limits on the universal quark coupling $g_{q}'$ as a function of resonance mass...","name":"Coupling limits (Quark only)"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins3073143?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/159438"}],"inLanguage":"en","name":"Search for dijet resonances with data scouting in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins3073143?version=1","version":1}