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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorTumasyan, A.en_US
dc.contributor.authorALPANA, A.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorKANSAL, B.en_US
dc.contributor.authorLAHA,Aen_US
dc.contributor.authorPANDEY, S.en_US
dc.contributor.authorRASTOGI, A.en_US
dc.contributor.authorSHARMA, SEEMA et al.en_US
dc.date.accessioned2022-07-22T10:55:29Z
dc.date.available2022-07-22T10:55:29Z
dc.date.issued2022-06en_US
dc.identifier.citationJournal of High Energy Physics, 2022(6), 156.en_US
dc.identifier.issn1029-8479en_US
dc.identifier.urihttps://doi.org/10.1007/JHEP06(2022)156en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/7261
dc.description.abstractThe first collider search for dark matter arising from a strongly coupled hidden sector is presented and uses a data sample corresponding to 138 fb−1, collected with the CMS detector at the CERN LHC, at s√s = 13 TeV. The hidden sector is hypothesized to couple to the standard model (SM) via a heavy leptophobic Z′ mediator produced as a resonance in proton-proton collisions. The mediator decay results in two “semivisible” jets, containing both visible matter and invisible dark matter. The final state therefore includes moderate missing energy aligned with one of the jets, a signature ignored by most dark matter searches. No structure in the dijet transverse mass spectra compatible with the signal is observed. Assuming the Z′ boson has a universal coupling of 0.25 to the SM quarks, an inclusive search, relevant to any model that exhibits this kinematic behavior, excludes mediator masses of 1.5–4.0 TeV at 95% confidence level, depending on the other signal model parameters. To enhance the sensitivity of the search for this particular class of hidden sector models, a boosted decision tree (BDT) is trained using jet substructure variables to distinguish between semivisible jets and SM jets from background processes. When the BDT is employed to identify each jet in the dijet system as semivisible, the mediator mass exclusion increases to 5.1 TeV, for wider ranges of the other signal model parameters. These limits exclude a wide range of strongly coupled hidden sector models for the first time.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subjectBeyond Standard Modelen_US
dc.subjectDark Matteren_US
dc.subjectHadron-Hadron Scatteringen_US
dc.subject2022-JUL-WEEK2en_US
dc.subjectTOC-JUL-2022en_US
dc.subject2022en_US
dc.titleSearch for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of High Energy Physicsen_US
dc.publication.originofpublisherForeignen_US
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