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dc.creatorAad, G.
dc.creatorAgatonović-Jovin, Tatjana
dc.creatorBozic, I.
dc.creatorDimitrievska, A.
dc.creatorKrstić, Jelena
dc.creatorMamužić, Judita
dc.creatorMarjanović, M.
dc.creatorPopović, D. S.
dc.creatorSijacki, Dj.
dc.creatorSimić, Lj.
dc.creatorVranješ, Nenad
dc.creatorVranješ Milosavljević, Marija
dc.creatorŽivković, Lada
dc.date.accessioned2018-03-01T16:23:35Z
dc.date.available2018-03-01T16:23:35Z
dc.date.issued2015
dc.identifier.issn2470-0010
dc.identifier.issn2470-0029
dc.identifier.urihttps://vinar.vin.bg.ac.rs/handle/123456789/725
dc.description.abstractA search for the decay to a pair of new particles of either the 125 GeV Higgs boson (h) or a second charge parity (CP)-even Higgs boson (H) is presented. The data set corresponds to an integrated luminosity of 20.3 fb(-1) of pp collisions at root s = 8 TeV recorded by the ATLAS experiment at the LHC in 2012. The search was done in the context of the next-to-minimal supersymmetric standard model, in which the new particles are the lightest neutral pseudoscalar Higgs bosons (a). One of the two a bosons is required to decay to two muons while the other is required to decay to two tau leptons. No significant excess is observed above the expected backgrounds in the dimuon invariant mass range from 3.7 to 50 GeV. Upper limits are placed on the production of h - GT aa relative to the standard model gg - GT h production, assuming no coupling of the a boson to quarks. The most stringent limit is placed at 3.5% for m(a) = 3.75 GeV. Upper limits are also placed on the production cross section of H - GT aa from 2.33 to 0.72 pb, for fixed m(a) = GeV with m(H) ranging from 100 to 500 GeV.en
dc.relationANPCyT, Argentina, YerPhI, Armenia, ARC, Australia, BMWFW, Austria, FWF, Austria, ANAS, Azerbaijan, SSTC, Belarus, CNPq, Brazil, FAPESP, Brazil, NSERC, Canada, NRC, Canada, CFI, Canada, CERN, CONICYT, Chile, CAS, China, MOST, China, NSFC, China, COLCIENCIAS, Colombia, MSMT CR, Czech Republic, MPO CR, Czech Republic, VSC CR, Czech Republic, DNRF, Denmark, DNSRC, Denmark, Lundbeck Foundation, Denmark, EPLANET, European Union, ERC, European Union, NSRF, European Union, IN2P3-CNRS, France, CEA-DSM/IRFU, France, GNSF, Georgia, BMBF, Germany, DFG, Germany, HGF, Germany, MPG, Germany, AvH Foundation, Germany, GSRT, Greece, NSRF, Greece, RGC, China, Hong Kong SAR, China, ISF, Israel, MINERVA, Israel, GIF, Israel, I-CORE, Israel, Benoziyo Center, Israel, INFN, Italy, MEXT, Japan, JSPS, Japan, CNRST, Morocco, FOM, Netherlands, NWO, Netherlands, BRF, Norway, RCN, Norway, MNiSW, Poland, NCN, Poland, GRICES, Portugal, FCT, Portugal, MNE/IFA, Romania, MES of Russia, Russian Federation, NRC KI, Russian Federation, JINR, MSTD, Serbia, MSSR, Slovakia, ARRS, Slovenia, MIZS, Slovenia, DST/NRF, South Africa, MINECO, Spain, SRC, Sweden, Wallenberg Foundation, Sweden, SER, Switzerland, SNSF, Switzerland, Canton of Bern, Switzerland, Canton of Geneva, Switzerland, NSC, Taiwan, TAEK, Turkey, STFC, United Kingdom, Royal Society, United Kingdom, Leverhulme Trust, United Kingdom, DOE, United States of America, NSF, United States of America, ICREA
dc.rightsopenAccessen
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.sourcePhysical Review Den
dc.titleSearch for Higgs bosons decaying to aa in the mu mu tau tau final state in pp collisions at root s=8 TeV with the ATLAS experimenten
dc.typearticleen
dc.rights.licenseBY
dcterms.abstractМарјановиц, М.; Aгатоновић-Јовин Татјана; Поповиц, Д. С.; Мамузић Јудита; Крстиц, Ј.; Врањес, Н.; Симиц, Љ.; Милосављевиц, М. Врањес; Димитриевска, A.; Бозиц, И.; Сијацки, Дј.; Aад, Г.; Зивковиц, Л.;
dc.citation.volume92
dc.citation.issue5
dc.identifier.wos000360885900001
dc.identifier.doi10.1103/PhysRevD.92.052002
dc.citation.otherArticle Number: 052002
dc.citation.rankM21
dc.contributor.countATLAS Collaboration (ukupan broj autora: 2827)
dc.type.versionpublishedVersion
dc.identifier.scopus2-s2.0-84978024375
dc.identifier.fulltexthttps://vinar.vin.bg.ac.rs//bitstream/id/13902/721.pdf


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