{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.130817.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2098256"}},{"@id":"https://doi.org/10.1007/JHEP07(2023)161","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"A search for pairs of dijet resonances with the same mass is conducted in final states  with at least four jets. Results are presented separately for the case where the four  jet production proceeds via an intermediate resonant state and for nonresonant production.  The search uses a data sample corresponding to an integrated luminosity of $138~\\mathrm{fb}^{-1}$  collected by the CMS detector in proton-proton collisions at $\\sqrt{s}=13~\\mathrm{TeV}$.  Model-independent limits, at 95$\\%$ confidence level, are reported on the production  cross section of four-jet and dijet resonances. These first LHC limits on resonant pair  production of dijet resonances via high mass intermediate states are applied to a signal  model of diquarks that decay into pairs of vector-like quarks, excluding diquark  masses below $7.6~\\mathrm{TeV}$ for a particular model scenario. There are two events in the tails  of the distributions, each with a four-jet mass of $8~\\mathrm{TeV}$ and an average dijet mass of  $2~\\mathrm{TeV}$, resulting in local and global significances of 3.9 and 1.6 standard deviations,  respectively, if interpreted as a signal. The nonresonant search excludes pair production  of top squarks with masses between 0.50 $\\mathrm{TeV}$ and 0.77 $\\mathrm{TeV}$, with the exception  of a small interval between 0.52 and 0.58 $\\mathrm{TeV}$, for supersymmetric R-parity-violating  decays to quark pairs, significantly extending previous limits. Here, the most significant excess  above the predicted background occurs at an average dijet mass of 0.95 $\\mathrm{TeV}$, for which  the local and global significances are 3.6 and 2.5 standard deviations, respectively.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t1","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.11$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t2","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.13$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t3","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.15$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t4","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.17$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t5","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.19$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t6","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.21$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t7","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.23$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t8","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.25$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t9","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.27$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t10","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.29$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t11","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.31$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t12","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.33$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t13","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production...","name":"Cross-section limits - $M(X)/M(Y) = 0.42$"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t14","@type":"Dataset","description":"The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for the non-resonant...","name":"Cross-section limits - non resonant scenario"},{"@id":"https://doi.org/10.17182/hepdata.130817.v1/t15","@type":"Dataset","description":"Observed differential four-jet mass spectrum for 0.22 &lt; $\\\\a$ &lt; 0.24. 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