342 137

Full metadata record

DC FieldValueLanguage
dc.contributor.author김태정-
dc.date.accessioned2016-08-22T07:49:14Z-
dc.date.available2016-08-22T07:49:14Z-
dc.date.issued2015-03-
dc.identifier.citationPHYSICAL REVIEW D, v. 91, NO 5, Page. 11-25en_US
dc.identifier.issn1550-7998-
dc.identifier.issn1550-2368-
dc.identifier.urihttp://journals.aps.org/prd/abstract/10.1103/PhysRevD.91.052012-
dc.identifier.urihttp://hdl.handle.net/20.500.11754/22683-
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).en_US
dc.description.sponsorshipBMWFW (Austria) FWF (Austria) FNRS (Belgium) FWO (Belgium) CNPq (Brazil) CAPES (Brazil) FAPERJ (Brazil) FAPESP (Brazil) MES (Bulgaria) CERN CAS (China) MoST (China) NSFC (China) COLCIENCIAS (Colombia) MSES (Croatia) CSF (Croatia) RPF (Cyprus) MoER (Estonia) ERC IUT (Estonia) ERDF (Estonia) Academy of Finland (Finland) MEC (Finland) HIP (Finland) CEA (France) CNRS/IN2P3 (France) BMBF (Germany) DFG (Germany) HGF (Germany) GSRT (Greece) OTKA (Hungary) NIH (Hungary) DAE (India) DST (India) IPM (Iran) SFI (Ireland) INFN (Italy) MSIP (Republic of Korea) NRF (Republic of Korea) LAS (Lithuania) MOE (Malaysia) UM (Malaysia) CINVESTAV (Mexico) CONACYT (Mexico) SEP (Mexico) UASLP-FAI (Mexico) MBIE (New Zealand) PAEC (Pakistan) MSHE (Poland) NSC (Poland) FCT (Portugal) JINR (Dubna) MON (Russia) RosAtom (Russia) RAS (Russia) RFBR (Russia) MESTD (Serbia) SEIDI (Spain) CPAN (Spain) Swiss Funding Agencies (Switzerland) MST (Taipei) ThEPCenter (Thailand) IPST (Thailand) STAR (Thailand) NSTDA (Thailand) TUBITAK (Turkey) TAEK (Turkey) NASU (Ukraine) SFFR (Ukraine) STFC (United Kingdom) DOE (USA) NSF (USA) Marie Curie program (European Union) European Research Council (European Union) EPLANET (European Union) Leventis Foundation A. P. Sloan Foundation Alexander von Humboldt Foundation Belgian Federal Science Policy Office Fonds pour la Formation a la Recherche dans l'Industrie et dans l'Agriculture (FRIA Belgium) Agentschap voor Innovatie door Wetenschap en Technologie (IWT Belgium) Ministry of Education, Youth and Sports (MEYS) of the Czech Republic Council of Science and Industrial Research, India HOMING PLUS program of Foundation for Polish Science European Union, Regional Development Fund Compagnia di San Paolo (Torino) Consorzio per la Fisica (Trieste) MIUR (Italy) Thalis programme Aristeia programme EU-ESF Greek NSRF National Priorities Research Program by Qatar National Research Funden_US
dc.language.isoenen_US
dc.publisherAMER PHYSICAL SOCen_US
dc.titleSearch for long-lived particles that decay into final states containing two electrons or two muons in proton-proton collisions at root s=8Teven_US
dc.typeArticleen_US
dc.relation.no5-
dc.relation.volume91-
dc.identifier.doi10.1103/PhysRevD.91.052012-
dc.relation.page11-25-
dc.relation.journalPHYSICAL REVIEW D-
dc.contributor.googleauthorKhachatryan, V.-
dc.contributor.googleauthorSirunyan, A. M.-
dc.contributor.googleauthorTumasyan, A.-
dc.contributor.googleauthorAdam, W.-
dc.contributor.googleauthorBergauer, T.-
dc.contributor.googleauthorDragicevic, M.-
dc.contributor.googleauthorEroe, J.-
dc.contributor.googleauthorFriedl, M.-
dc.contributor.googleauthorFruehwirth, R.-
dc.contributor.googleauthorKim, T.J.-
dc.relation.code2015002842-
dc.sector.campusS-
dc.sector.daehakCOLLEGE OF NATURAL SCIENCES[S]-
dc.sector.departmentDEPARTMENT OF PHYSICS-
dc.identifier.pidtaekim-


qrcode

Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.

BROWSE