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Search for long-lived particles that decay into final states containing two electrons or two muons in proton-proton collisions at root s=8Tev

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dc.contributor.authorKhachatryan, V-
dc.contributor.authorSirunyan, AM-
dc.contributor.authorTumasyan, A-
dc.contributor.authorAdam, W-
dc.contributor.authorBergauer, T-
dc.contributor.authorDragicevic, M-
dc.contributor.authorEroe, J-
dc.contributor.authorFriedl, M-
dc.contributor.authorFruehwirth, R-
dc.contributor.authorKim, Tae Jeong-
dc.date.accessioned2022-07-07T04:44:46Z-
dc.date.available2022-07-07T04:44:46Z-
dc.date.created2021-05-13-
dc.date.issued2015-03-
dc.identifier.issn1550-7998-
dc.identifier.urihttps://scholarworks.bwise.kr/hanyang/handle/2021.sw.hanyang/143227-
dc.description.abstractA search is performed for long-lived particles that decay into final states that include a pair of electrons or a pair of muons. The experimental signature is a distinctive topology consisting of a pair of charged leptons originating from a displaced secondary vertex. Events corresponding to an integrated luminosity of 19.6 (20.5) fb(-1) in the electron (muon) channel were collected with the CMS detector at the CERN LHC in proton-proton collisions at root s TeV. No significant excess is observed above standard model expectations. Upper limits on the product of the cross section and branching fraction of such a signal are presented as a function of the long-lived particle's mean proper decay length. The limits are presented in an approximately model-independent way, allowing them to be applied to a wide class of models yielding the above topology. Over much of the investigated parameter space, the limits obtained are the most stringent to date. In the specific case of a model in which a Higgs boson in the mass range 125-1000 GeV/c(2) decays into a pair of long-lived neutral bosons in the mass range 20-350 GeV= c(2), each of which can then decay to dileptons, the upper limits obtained are typically in the range 0.2-10 fb for mean proper decay lengths of the long-lived particles in the range 0.01-100 cm. In the case of the lowest Higgs mass considered (125 GeV/c(2)), the limits are in the range 2-50 fb. These limits are sensitive to Higgs boson branching fractions as low as 10(-1).-
dc.language영어-
dc.language.isoen-
dc.publisherAMER PHYSICAL SOC-
dc.titleSearch for long-lived particles that decay into final states containing two electrons or two muons in proton-proton collisions at root s=8Tev-
dc.typeArticle-
dc.contributor.affiliatedAuthorKim, Tae Jeong-
dc.identifier.doi10.1103/PhysRevD.91.052012-
dc.identifier.scopusid2-s2.0-84927587727-
dc.identifier.wosid000352154400001-
dc.identifier.bibliographicCitationPHYSICAL REVIEW D, v.91, no.5, pp.11 - 25-
dc.relation.isPartOfPHYSICAL REVIEW D-
dc.citation.titlePHYSICAL REVIEW D-
dc.citation.volume91-
dc.citation.number5-
dc.citation.startPage11-
dc.citation.endPage25-
dc.type.rimsART-
dc.type.docType정기 학술지(기타)-
dc.description.journalClass1-
dc.description.isOpenAccessY-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaAstronomy & Astrophysics-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryAstronomy & Astrophysics-
dc.relation.journalWebOfScienceCategoryPhysics, Particles & Fields-
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