Mimar Sinan Güzel Sanatlar Üniversitesi Açık Bilim, Sanat Arşivi
Açık Bilim, Sanat Arşivi, Mimar Sinan Güzel Sanatlar Üniversitesi tarafından doğrudan ve dolaylı olarak yayınlanan; kitap, makale, tez, bildiri, rapor gibi tüm akademik kaynakları uluslararası standartlarda dijital ortamda depolar, Üniversitenin akademik performansını izlemeye aracılık eder, kaynakları uzun süreli saklar ve yayınların etkisini artırmak için telif haklarına uygun olarak Açık Erişime sunar.MSGSÜ'de Ara
Search for electroweak production of charginos in final states with two ? leptons in pp collisions at ?s=8 TeV
dc.contributor.author | Khachatryan, V. | |
dc.contributor.author | Sirunyan, A.M. | |
dc.contributor.author | Tumasyan, A. | |
dc.contributor.author | Adam, W. | |
dc.contributor.author | Asilar, E. | |
dc.contributor.author | Bergauer, T. | |
dc.contributor.author | Özok, Ferhat | |
dc.date.accessioned | 2025-01-09T20:03:28Z | |
dc.date.available | 2025-01-09T20:03:28Z | |
dc.date.issued | 2017 | |
dc.identifier.issn | 1029-8479 | |
dc.identifier.uri | https://doi.org/10.1007/JHEP04(2017)018 | |
dc.identifier.uri | https://hdl.handle.net/20.500.14124/7431 | |
dc.description.abstract | Results are presented from a search for the electroweak production of supersymmetric particles in pp collisions in final states with two ? leptons. The data sample corresponds to an integrated luminosity between 18.1 fb?1 and 19.6 fb?1 depending on the final state of ? lepton decays, at s=8 TeV, collected by the CMS experiment at the LHC. The observed event yields in the signal regions are consistent with the expected standard model backgrounds. The results are interpreted using simplified models describing the pair production and decays of charginos or ? sleptons. For models describing the pair production of the lightest chargino, exclusion regions are obtained in the plane of chargino mass vs. neutralino mass under the following assumptions: the chargino decays into third-generation sleptons, which are taken to be the lightest sleptons, and the sleptons masses lie midway between those of the chargino and the neutralino. Chargino masses below 420 GeV are excluded at a 95% confidence level in the limit of a massless neutralino, and for neutralino masses up to 100 GeV, chargino masses up to 325 GeV are excluded at 95% confidence level. Constraints are also placed on the cross section for pair production of ? sleptons as a function of mass, assuming a massless neutralino.[Figure not available: see fulltext.] © 2017, The Author(s). | en_US |
dc.description.sponsorship | Austrian Federal Ministry of Science; Canton Zurich; Desarrollo e Innovación and Programa Consolider-Ingenio 2010; ETH Board; EU-ESF; FRIA-Belgium; Fundacão para a Ciência e a Tecnologia; Helsinki Institute of Physics; IWT-Belgium; Institute for Studies in Theoretical Physics and Mathematics; LNS; Mexican Funding Agencies; National Innovation Office; National Science and Technology Development Agency of Thailand; National Scientific Research Foundation; Republic of Korea; Secretariat for Higher Education, Science, Technology and Innovation; Secretaría de Estado de Investigación; State Fund for Fundamental Researches; UASLP-FAI; UniZH; National Science Foundation, NSF, (1151640, 1211067, 1506130, 1506168, 1508869, 1606321, 1624356); National Science Foundation, NSF; U.S. Department of Energy, USDOE; Alfred P. Sloan Foundation; Welch Foundation, (C-1845); Welch Foundation; Alexander von Humboldt-Stiftung; Departamento Administrativo de Ciencia, Tecnología e Innovación (COLCIENCIAS); Qatar National Research Fund, QNRF; Secretaría de Educación Pública, SEP; Türkiye Atom Enerjisi Kurumu, TAEK; CERN; Thailand Center of Excellence in Physics; Institute for the Promotion of Teaching Science and Technology, IPST; Science and Technology Facilities Council, STFC, (GRIDPP, PP/E000479/1, ST/H000925/1, ST/M004775/1, ST/N001273/1); Science and Technology Facilities Council, STFC; European Commission, EC; European Research Council, ERC; Department of Science and Technology, Ministry of Science and Technology, India, ??????; Council of Scientific and Industrial Research, India, CSIR; Department of Atomic Energy, Government of India, ????; Science Foundation Ireland, SFI; Helmholtz-Gemeinschaft, HGF; Deutsche Forschungsgemeinschaft, DFG; Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung, SNF; Fundação de Amparo à Pesquisa do Estado de São Paulo, FAPESP; National Natural Science Foundation of China, NSFC; Research Promotion Foundation, ????; Ministerstvo Školství, Mláde?e a T?lov?chovy, MŠMT; Fundacja na rzecz Nauki Polskiej, FNP; Russian Foundation for Basic Research, ????; Eesti Teadusagentuur, ETAg, (IUT23-4, IUT23-6); Eesti Teadusagentuur, ETAg; Coordenação de Aperfeiçoamento de Pessoal de Nível Superior, CAPES; Suomen Akatemia; Bundesministerium für Bildung und Forschung, BMBF; Chinese Academy of Sciences, CAS; Austrian Science Fund, FWF; Fonds De La Recherche Scientifique - FNRS, FNRS; Russian Academy of Sciences, ???; Belgian Federal Science Policy Office, BELSPO; Chulalongkorn University, CU; Eidgenössische Technische Hochschule Zürich, ETH; Opetus- ja Kulttuuriministeriö; Fonds Wetenschappelijk Onderzoek, FWO; Agentschap voor Innovatie door Wetenschap en Technologie, IWT; Fonds pour la Formation à la Recherche dans l’Industrie et dans l’Agriculture, FRIA; Consejo Nacional de Ciencia y Tecnología, CONACYT; Ministry of Education and Science of the Russian Federation, Minobrnauka; General Secretariat for Research and Technology, GSRT; Ministry of Business, Innovation and Employment, MBIE; Conselho Nacional de Desenvolvimento Científico e Tecnológico, CNPq; Ministry of Science, ICT and Future Planning, MSIP; National Research Foundation of Korea, NRF; Joint Institute for Nuclear Research, JINR; Instituto Nazionale di Fisica Nucleare, INFN; A.G. Leventis Foundation; Paul Scherrer Institut, PSI; Narodowe Centrum Nauki, NCN; Universiti Malaya, UM; Türkiye Bilimsel ve Teknolojik Araştirma Kurumu, TÜBITAK; Hrvatska Zaklada za Znanost, HRZZ; Ministarstvo Prosvete, Nauke i Tehnološkog Razvoja, MPNTR; Ministerstwo Nauki i Szkolnictwa Wy?szego, MNiSW, (2014/13/B/ST2/02543, DEC-2012/07/E/ST2/01406); Ministerstwo Nauki i Szkolnictwa Wy?szego, MNiSW; Fundação Carlos Chagas Filho de Amparo à Pesquisa do Estado do Rio de Janeiro, FAPERJ; Ministry of Science and Technology, Taiwan, MOST; National Academy of Sciences of Ukraine, NASU; Centre National de la Recherche Scientifique, CNRS; Benemérita Universidad Autónoma de Puebla, BUAP; Commissariat à l'Énergie Atomique et aux Énergies Alternatives, CEA; Ministarstvo Znanosti, Obrazovanja i Sporta, MZOS; Lietuvos Moksl? Akademija; European Regional Development Fund, ERDF; Centro de Investigación y de Estudios Avanzados del Instituto Politécnico Nacional, CINVESTAV; Pakistan Atomic Energy Commission, PAEC; Institut National de Physique Nucléaire et de Physique des Particules, IN2P3; Federal Agency of Atomic Energy of the Russian Federation; Sociedad Española de Reumatología, SER; Kementerian Pendidikan Malaysia, KPM | en_US |
dc.language.iso | eng | en_US |
dc.publisher | Springer Science and Business Media Deutschland GmbH | en_US |
dc.relation.ispartof | Journal of High Energy Physics | en_US |
dc.rights | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.subject | Hadron-Hadron scattering (experiments) | en_US |
dc.subject | Supersymmetry | en_US |
dc.title | Search for electroweak production of charginos in final states with two ? leptons in pp collisions at ?s=8 TeV | en_US |
dc.type | article | en_US |
dc.department | Fakülteler, Fen Edebiyat Fakültesi, Fizik Bölümü | en_US |
dc.institutionauthor | Özok, Ferhat | |
dc.identifier.doi | 10.1007/JHEP04(2017)018 | |
dc.identifier.volume | 2017 | en_US |
dc.identifier.issue | 4 | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.identifier.scopus | 2-s2.0-85031806028 | en_US |
dc.identifier.scopusquality | Q1 | |
dc.indekslendigikaynak | Scopus | |
dc.snmz | KA_20250105 |
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