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dc.contributor.authorCMS Collaboration
dc.date.accessioned2018-10-23T16:29:48Z
dc.date.available2018-10-23T16:29:48Z
dc.date.issued2017-01
dc.identifier.citationThe CMS collaboration, Khachatryan, V., Sirunyan, A.M. et al. J. High Energ. Phys. (2017) 2017: 76. https://doi.org/10.1007/JHEP01(2017)076en_US
dc.identifier.urihttp://hdl.handle.net/1808/26949
dc.description.abstractThis paper describes the search for a high-mass narrow-width scalar particle decaying into a Z boson and a photon. The analysis is performed using proton-proton collision data recorded with the CMS detector at the LHC at center-of-mass energies of 8 and 13 TeV, corresponding to integrated luminosities of 19.7 and 2.7 fb−1, respectively. The Z bosons are reconstructed from opposite-sign electron or muon pairs. No statistically significant deviation from the standard model predictions has been found in the 200-2000 GeV mass range. Upper limits at 95% confidence level have been derived on the product of the scalar particle production cross section and the branching fraction of the Z decaying into electrons or muons, which range from 280 to 20 fb for resonance masses between 200 and 2000 GeV.en_US
dc.publisherSpringer Verlagen_US
dc.rights© The Author(s) 2017en_US
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/en_US
dc.subjectBeyond Standard Modelen_US
dc.subjectHadron-Hadron scattering (experiments)en_US
dc.titleSearch for high-mass Zγ resonances in e+e−γ and μ + μ −γ final states in proton-proton collisions at s√=8 and 13 TeVen_US
dc.typeArticleen_US
kusw.kuauthorBaringer, Philip, S.
kusw.kudepartmentPhysics and Astronomyen_US
dc.identifier.doihttps://doi.org/10.1007/JHEP01(2017)076en_US
kusw.oaversionScholarly/refereed, publisher versionen_US
kusw.oapolicyThis item meets KU Open Access policy criteria.en_US
dc.rights.accessrightsopenAccessen_US


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Except where otherwise noted, this item's license is described as: © The Author(s) 2017