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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorKhachatryan, V.en_US
dc.contributor.authorCHAUHAN, S.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorKAPOOR, A.en_US
dc.contributor.authorKOTHEKAR, K.en_US
dc.contributor.authorSHARMA, SEEMA et al.en_US
dc.date.accessioned2019-04-29T10:18:23Z
dc.date.available2019-04-29T10:18:23Z
dc.date.issued2016-06en_US
dc.identifier.citationThe European Physical Journal C, 76(6), 317.en_US
dc.identifier.issn1434-6044en_US
dc.identifier.issn1434-6052en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/2789-
dc.identifier.urihttps://doi.org/10.1140/epjc/s10052-016-4149-yen_US
dc.description.abstractA search for narrow resonances decaying to an electron and a muon is presented. The e μ mass spectrum is also investigated for non-resonant contributions from the production of quantum black holes (QBHs). The analysis is performed using data corresponding to an integrated luminosity of 19.7 fb-1 collected in proton-proton collisions at a centre-of-mass energy of 8 TeV with the CMS detector at the LHC. With no evidence for physics beyond the standard model in the invariant mass spectrum of selected eμ pairs, upper limits are set at 95 % confidence level on the product of cross section and branching fraction for signals arising in theories with charged lepton flavour violation. In the search for narrow resonances, the resonant production of a τ sneutrino in R-parity violating supersymmetry is considered. The τ sneutrino is excluded for masses below 1.28 TeV for couplings λ132=λ231=λ′311=0.01, and below 2.30 TeV for λ132=λ231=0.07 and λ′311=0.11. These are the most stringent limits to date from direct searches at high-energy colliders. In addition, the resonance searches are interpreted in terms of a model with heavy partners of the Z boson and the photon. In a framework of TeV-scale quantum gravity based on a renormalization of Newton’s constant, the search for non-resonant contributions to the e μ mass spectrum excludes QBH production below a threshold mass Mth of 1.99 TeV. In models that invoke extra dimensions, the bounds range from 2.36 TeV for one extra dimension to 3.63 TeV for six extra dimensions. This is the first search for QBHs decaying into the e μ final state.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subjectlepton flavouren_US
dc.subjectViolating decaysen_US
dc.subjectQuantum black holesen_US
dc.subjectProton-proton collisionsen_US
dc.subject2016en_US
dc.titleSearch for lepton flavour violating decays of heavy resonances and quantum black holes to an eμ pair in proton–proton collisions at √s=8 TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleThe European Physical Journal Cen_US
dc.publication.originofpublisherForeignen_US
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