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Search for massive resonances decaying into WW, WZ, ZZ, qW, and qZ with dijet final states at √s=13 TeV

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dc.contributor.author CMS Collaboration en_US
dc.contributor.author Sirunyan, A. M. en_US
dc.contributor.author CHAUHAN, S. en_US
dc.contributor.author DUBE, SOURABH en_US
dc.contributor.author HEGDE, V. en_US
dc.contributor.author KAPOOR, A. en_US
dc.contributor.author KOTHEKAR, K. en_US
dc.contributor.author PANDEY, S. en_US
dc.contributor.author RANE, A. en_US
dc.contributor.author SHARMA, SEEMA et al. en_US
dc.date.accessioned 2019-09-11T05:59:09Z
dc.date.available 2019-09-11T05:59:09Z
dc.date.issued 2018-04 en_US
dc.identifier.citation Physical Review D, 97(7), 072006. en_US
dc.identifier.issn 2470-0010 en_US
dc.identifier.issn 2470-0029 en_US
dc.identifier.uri http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4083
dc.identifier.uri https://doi.org/10.1103/PhysRevD.97.072006 en_US
dc.description.abstract Results are presented from a search in the dijet final state for new massive narrow resonances decaying to pairs of W and Z bosons or to a W / Z boson and a quark. Results are based on data recorded in proton-proton collisions at √ s = 13     TeV with the CMS detector at the CERN LHC. The data correspond to an integrated luminosity of 35.9     fb − 1 . The mass range investigated extends upwards from 1.2 TeV. No excess is observed above the estimated standard model background and limits are set at 95% confidence level on cross sections, which are interpreted in terms of various models that predict gravitons, heavy spin-1 bosons, and excited quarks. In a heavy vector triplet model, W ′ and Z ′ resonances, with masses below 3.2 and 2.7 TeV, respectively, and spin-1 resonances with degenerate masses below 3.8 TeV are excluded at 95% confidence level. In the case of a singlet W ′ resonance masses between 3.3 and 3.6 TeV can be excluded additionally. Similarly, excited quark resonances, q ∗ , decaying to q W and q Z with masses less than 5.0 and 4.7 TeV, respectively, are excluded. In a narrow-width bulk graviton model, upper limits are set on cross sections ranging from 0.6 fb for high resonance masses above 3.6 TeV, to 36.0 fb for low resonance masses of 1.3 TeV. en_US
dc.language.iso en en_US
dc.publisher American Physical Society en_US
dc.subject Proton-proton collisions en_US
dc.subject Dilepton final states en_US
dc.subject Proton-proton collisions en_US
dc.subject CMS detector en_US
dc.subject 2018 en_US
dc.title Search for massive resonances decaying into WW, WZ, ZZ, qW, and qZ with dijet final states at √s=13 TeV en_US
dc.type Article en_US
dc.contributor.department Dept. of Physics en_US
dc.identifier.sourcetitle Physical Review D en_US
dc.publication.originofpublisher Foreign en_US


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