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Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV

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Sirunyan, A. M.Tumasyan, A.Adam, W.Ambrogi, F.Asilar, E.Bergauer, T.Brandstetter, J.Brondolin, E.Dragicevic, M.Eroe, J.Del Valle, A. EscalanteFlechl, M.Friedl, M.Fruehwirth, R.Ghete, V. M.Grossmann, J.Hrubec, J.Jeitler, M.Koenig, A.Krammer, N.Kraetschmer, I.Liko, D.Madlener, T.Mikulec, I.Pree, E.Rad, N.Rohringer, H.Schieck, J.Schoefbeck, R.Spanring, M.Spitzbart, D.Taurok, A.Waltenberger, W.Wittmann, J.Wulz, C. -E.Zarucki, M.Chekhovsky, V.Mossolov, V.Gonzalez, J. SuarezDe Wolf, E. A.Di Croce, D.Janssen, X.Lauwers, J.Pieters, M.De Klundert, M. VanVan Haevermaet, H.Van Mechelen, P.Van Remortel, N.Abu Zeid, S.Blekman, F.D'Hondt, J.De Bruyn, I.De Clercq, J.Deroover, K.Flouris, G.Lontkovskyi, D.Lowette, S.Marchesini, I.Moortgat, S.Moreels, L.Python, Q.Skovpen, K.Tavernier, S.Van Doninck, W.Van Mulders, P.Van Parijs, I.Beghin, D.Bilin, B.Brun, H.Clerbaux, B.De Lentdecker, G.Delannoy, H.Dorney, B.Fasanella, G.Favart, L.Goldouzian, R.Grebenyuk, A.Kalsi, A. K.Lenzi, T.Luetic, J.Seva, T.Starling, E.Velde, C. VanderVanlaer, P.Vannerom, D.Yonamine, R.Cornelis, T.Dobur, D.Fagot, A.Gul, M.Khvastunov, I.Poyraz, D.Roskas, C.Trocino, D.Tytgat, M.Verbeke, W.Vermassen, B.Vit, M.Zaganidis, N.Bakhshiansohi, H.Bondu, O.Brochet, S.Bruno, G.Caputo, C.Caudron, A.David, P.De Visscher, S.Delaere, C.Delcourt, M.Francois, B.Giammanco, A.Krintiras, G.Lemaitre, V.Magitteri, A.Mertens, A.Musich, M.Piotrzkowski, K.Quertenmont, L.Saggio, A.Marono, M. VidalWertz, S.Zobec, J.Alda Junior, W. L.Alves, F. L.Alves, G. A.Brito, L.Correia Silva, G.Hensel, C.Moraes, A.Pol, M. E.Rebello Teles, P.Belchior Batista Das Chagas, E.Carvalho, W.Chinellato, J.Coelho, E.Da Costa, E. M.Da Silveira, G. G.Damiao, D. De JesusFonseca De Souza, S.Huertas Guativa, M.Malbouisson, H.Medina Jaime, M.Melo De Almeida, M.Mora Herrera, C.Mundim, L.Nogima, H.Sanchez Rosas, L. J.Santoro, A.Sznajder, A.Thiel, M.Tonelli Manganote, E. J.Torres Da Silva De Araujo, F.Vilela Pereira, A.Ahuja, S.Bernardes, C. A.Calligaris, L.Fernandez Perez Tomei, T. R.Gregores, E. M.Mercadante, P. G.Novaes, S. F.Padula, Sandra S.Romero Abad, D.Ruiz Vargas, J. C.Aleksandrov, A.Hadjiiska, R.Iaydjiev, P.Marinov, A.Misheva, M.Rodozov, M.Shopova, M.Sultanov, G.Dimitrov, A.Litov, L.Pavlov, B.Petkov, P.Fang, W.Gao, X.Yuan, L.Ahmad, M.Bian, J. G.Chen, G. M.Chen, H. S.Chen, M.Chen, Y.Jiang, C. H.Leggat, D.Liao, H.Liu, Z.Romeo, F.Shaheen, S. M.Spiezia, A.Tao, J.Wang, C.Wang, Z.Yazgan, E.Zhang, H.Zhao, J.Ban, Y.Chen, G.Li, J.Li, Q.Liu, S.Mao, Y.Qian, S. J.Wang, D.Xu, Z.Wang, Y.Avila, C.Cabrera, A.Carrillo Montoya, C. A.Chaparro Sierra, L. F.Florez, C.Gonzalez Hernandez, C. F.Segura Delgado, M. A.Courbon, B.Godinovic, N.Lelas, D.Puljak, I.Cipriano, P. M. RibeiroSculac, T.Antunovic, Z.Kovac, M.Brigljevic, V.Ferencek, D.Kadija, K.Mesic, B.Starodumov, A.Susa, T.Ather, M. W.Attikis, A.Mavromanolakis, G.Mousa, J.Nicolaou, C.Ptochos, F.Razis, P. A.Rykaczewski, H.Finger, M.Finger, M., Jr.Carrera Jarrin, E.Assran, Y.Elgammal, S.Kamel, A. EllithiBhowmik, S.Dewanjee, R. K.Kadastik, M.Perrini, L.Raidal, M.Veelken, C.Eerola, P.Kirschenmann, H.Pekkanen, J.Voutilainen, M.Havukainen, J.Heikkila, J. K.Jarvinen, T.Karimaki, V.Kinnunen, R.Lampen, T.Lassila-Perini, K.Laurila, S.Lehti, S.Linden, T.Luukka, P.Maenpaa, T.Siikonen, H.Tuominen, E.Tuominiemi, J.Tuuva, T.Besancon, M.Couderc, F.Dejardin, M.Denegri, D.Faure, J. L.Ferri, F.Ganjour, S.Ghosh, S.Givernaud, A.Gras, P.de Monchenault, G. HamelJarry, P.Leloup, C.Locci, E.Machet, M.Malcles, J.Negro, G.Rander, J.Rosowsky, A.Sahin, M. O.Titov, M.Abdulsalam, A.Amendola, C.Antropov, I.Baffioni, S.Beaudette, F.Busson, P.Cadamuro, L.Charlot, C.de Cassagnac, R. GranierJo, M.Kucher, I.Lisniak, S.Lobanov, A.Blanco, J. MartinNguyen, M.Ochando, C.Ortona, G.Paganini, P.Pigard, P.Salerno, R.Sauvan, J. B.Sirois, Y.Leiton, A. G. 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F.Duchardt, D.Endres, M.Erdmann, M.Erdweg, S.Esch, T.Fischer, R.Gueuth, A.Hebbeker, T.Heidemann, C.Hoepfner, K.Knutzen, S.Materok, M.Merschmeyer, M.Meyer, A.Millet, P.Mukherjee, S.Pook, T.Radziej, M.Reithler, H.Rieger, M.Scheuch, F.Teyssier, D.Thueer, S.Wiedenbeck, S.Fluegge, G.Kargoll, B.Kress, T.Kuensken, A.Mueller, T.Nehrkorn, A.Nowack, A.Pistone, C.Pooth, O.Stahl, A.Martin, M. AldayaArndt, T.Asawatangtrakuldee, C.Beernaert, K.Behnke, O.Behrens, U.Martinez, A. BermudezBin Anuar, A. A.Borras, K.Botta, V.Campbell, A.Connor, P.Contreras-Campana, C.Costanza, F.Danilov, V.De Wit, A.Pardos, C. DiezDamiani, D. DominguezEckerlin, G.Eckstein, D.Eichhorn, T.Eren, E.Gallo, E.Garcia, J. GarayGeiser, A.Luyando, J. M. GradosGrohsjean, A.Gunnellini, P.Guthoff, M.Harb, A.Hauk, J.Hempel, M.Jung, H.Kasemann, M.Keaveney, J.Kleinwort, C.Knolle, J.Korol, I.Kruecker, D.Lange, W.Lelek, A.Lenz, T.Lipka, K.Lohmann, W.Mankel, R.Melzer-Pellmann, I. -A.Meyer, A. 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Issue Date
25-6월-2018
Publisher
SPRINGER
Keywords
Beyond Standard Model; Hadron-Hadron scattering (experiments)
Citation
JOURNAL OF HIGH ENERGY PHYSICS, no.6
Indexed
SCIE
SCOPUS
Journal Title
JOURNAL OF HIGH ENERGY PHYSICS
Number
6
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/131774
DOI
10.1007/JHEP06(2018)128
ISSN
1126-6708
Abstract
A search for new high-mass resonances in proton-proton collisions having final states with an electron or muon and missing transverse momentum is presented. The analysis uses proton-proton collision data collected in 2016 with the CMS detector at the LHC at a center-of-mass energy of 13TeV, corresponding to an integrated luminosity of 35.9 fb(-1). The transverse mass distribution of the charged lepton-neutrino system is used as the discriminating variable. No significant deviation from the standard model prediction is found. The best limit, from the combination of electron and muon channels, is 5.2TeV at 95% confidence level for the mass of a W' boson with the same couplings as those of the standard model Wboson. Exclusion limits of 2.9TeV are set on the inverse radius of the extra dimension in the framework of split universal extra dimensions. In addition, model-independent limits are set on the production cross section and coupling strength of W' bosons decaying into this final state. An interpretation is also made in the context of an R parity violating supersymmetric model with a slepton as a mediator and flavor violating decay.
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