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Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at root s=13 TeV

Authors
Sirunyan, A. M.Tumasyan, A.Adam, W.Ambrogi, F.Asilar, E.Bergauer, T.Brandstetter, J.Brondolin, E.Drag-Icevic, M.Eroe, J.Flechl, M.Friedl, M.Fruewirth, R.Ghete, V. M.Grossmann, J.Hrubec, J.Jeitler, M.Koenig, A.Krammer, N.Kraetschmer, I.Liko, D.Madlener, T.Mikulec, I.Pree, E.Rabady, D.Rad, N.Rohringer, H.Schieck, J.Schoefbeck, R.Spanring, M.Spitzbart, D.Strauss, J.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.Van De Klundert, M.Van Haevermaet, H.Van Mechelen, P.Van Remortel, N.Van Spilbeeck, A.Abu Zeid, S.Blekman, F.D'Hondt, J.De Bruyn, I.De Clercq, J.Deroover, K.Flouris, G.Lontkovskyi, D.Lowette, S.Moortgat, S.Moreels, L.Olbrechts, A.Python, Q.Skovpen, K.Tavernier, S.Van Doninck, W.Van Mulders, P.Van Parijs, I.Brun, H.Clerbaux, B.De Lentdecker, G.Delannoy, H.Fasanella, G.Favart, L.Goldouzian, R.Grebenyuk, A.Karapostoli, G.Lenzi, T.Luetic, J.Maerschalk, T.Marinov, A.Randle-conde, A.Seva, T.Vander Velde, C.Vanlaer, P.Vannerom, D.Yonamine, R.Zenoni, F.Zhang, F.Cimmino, A.Cornelis, T.Dobur, D.Fagot, A.Gul, M.Khvastunov, I.Poyraz, D.Roskas, C.Salva, S.Tytgat, M.Verbeke, W.Zaganidis, N.Bakhshiansohi, H.Bondu, O.Brochet, S.Bruno, G.Caudron, A.De Visscher, S.Delaere, C.Delcourt, M.Francois, B.Giammanco, A.Jafari, A.Komm, M.Krintiras, G.Lemaitre, V.Magitteri, A.Mertens, A.Musich, M.Piotrzkowski, K.Quertenmont, L.Marono, M. VidalWertz, S.Beliy, N.Alda Junior, W. L.Alves, F. L.Alves, G. A.Brito, L.Correa Martins Junior, M.Hensel, C.Moraes, A.Pol, M. E.Rebello Teles, P.Belchior Batista Das Chagas, E.Carvalho, W.Chinellato, J.Custodio, A.Da Costa, E. M.Da Silveira, G. G.De Jesus Damiao, D.Fonseca De Souza, S.Huertas Guativa, L. M.Malbouisson, H.Melo De Almeida, M.Mora Herrera, C.Mundim, L.Nogima, H.Santoro, A.Sznajder, A.Tonelli Manganote, E. J.Torres Da Silva De Araujo, F.Vilela Pereira, A.Ahuja, S.Bernardes, C. A.Fernandez Perez Tomei, T. R.Gregores, E. M.Mercadante, P. G.Moon, C. S.Novaes, S. F.Padula, Sandra S.Romero Abad, D.Ruiz Vargas, J. C.Aleksandrov, A.Hadjiiska, R.Iaydjiev, P.Misheva, M.Rodozov, M.Shopova, M.Stoykova, S.Sultanov, G.Dimitrov, A.Glushkov, I.Litov, L.Pavlov, B.Petkov, P.Fang, W.Gao, X.Ahmad, M.Bian, J. G.Chen, G. M.Chen, H. S.Chen, M.Chen, Y.Jiang, C. H.Leggat, D.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, Q.Liu, S.Mao, Y.Qian, S. J.Wang, D.Xu, Z.Avila, C.Cabrera, A.Chaparro Sierra, L. F.Florez, C.Gonzalez Hernandez, C. F.Ruiz Alvarez, J. D.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.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.Abdelalim, A. A.Mohammed, Y.Salama, E.Dewanjee, R. K.Kadastik, M.Perrini, L.Raidal, M.Tiko, A.Veelken, C.Eerola, P.Pekkanen, J.Voutilainen, M.Harkonen, J.Jarvinen, T.Karimaki, V.Kinnunen, R.Lampen, T.Lassila-Perini, K.Lehti, S.Linden, T.Luukka, P.Tuominen, E.Tuominiemi, J.Tuovinen, E.Talvitie, 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.Kucher, I.Locci, E.Machet, M.Malcles, J.Negro, G.Rander, J.Rosowsky, A.Sahin, M. O.Titov, M.Abdulsalam, A.Antropov, I.Baffioni, S.Beaudette, F.Busson, P.Cadamuro, L.Charlot, C.Davignon, O.de Cassagnac, R. GranierJo, M.Lisniak, S.Lobanov, A.Blanco, J. MartinNguyen, M.Ochando, C.Ortona, G.Paganini, P.Pigard, P.Regnard, S.Salerno, R.Sauvan, J. B.Sirois, Y.Leiton, A. G. StahlStrebler, T.Yilmaz, Y.Zabi, A.Zghiche, A.Agram, J. -L.Andrea, J.Bloch, D.Brom, J. -M.Buttignol, M.Chabert, E. C.Chanon, N.Collard, C.Conte, E.Coubez, X.Fontaine, J. -C.Gele, D.Goerlach, U.Jansova, M.Le Bihan, A. -C.Van Hove, P.Gadrat, S.Beauceron, S.Bernet, C.Boudoul, G.Chierici, R.Contardo, D.Depasse, P.El Mamouni, H.Fay, J.Finco, L.Gascon, S.Gouzevitch, M.Grenier, G.Ille, B.Lagarde, F.Laktineh, I. B.Lethuillier, M.Mirabito, L.Pequegnot, A. L.Perries, S.Popov, A.Sordini, V.Donckt, M. VanderViret, S.Khvedelidze, A.Bagaturia, I.Autermann, C.Beranek, S.Feld, L.Kiesel, M. 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Issue Date
15-11월-2017
Publisher
SPRINGER
Keywords
Hadron-Hadron scattering (experiments); Heavy quark production; vector-like quarks
Citation
JOURNAL OF HIGH ENERGY PHYSICS, no.11
Indexed
SCIE
SCOPUS
Journal Title
JOURNAL OF HIGH ENERGY PHYSICS
Number
11
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/132170
DOI
10.1007/JHEP11(2017)085
ISSN
1126-6708
Abstract
A search for pair production of massive vector-like T and B quarks in proton-proton collisions at root s = 13 TeV is presented. The data set was collected in 2015 by the CMS experiment at the LHC and corresponds to an integrated luminosity of up to 2.6 fb(-1). The T and B quarks are assumed to decay through three possible channels into a heavy boson (either a W, Z or Higgs boson) and a third generation quark. This search is performed in final states with one charged lepton and several jets, exploiting techniques to identify W or Higgs bosons decaying hadronically with large transverse momenta. No excess over the predicted standard model background is observed. Upper limits at 95% confidence level on the T quark pair production cross section are set that exclude T quark masses below 860 GeV in the singlet, and below 830 GeV in the doublet branching fraction scenario. For other branching fraction combinations with B (T -> tH) + B(T -> bW) >= 0.4, lower limits on the T quark range from 790 to 940 GeV. Limits are also set on pair production of singlet vector-like B quarks, which can be excluded up to a mass of 730 GeV. The techniques showcased here for understanding highly-boosted final states are important as the sensitivity to new particles is extended to higher masses.
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