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Search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV in the diphoton final state in proton-proton collisions at root s=8 and 13 TeV

Authors
Sirunyan, A. M.Tumasyan, A.Adam, W.Ambrogi, F.Asilar, E.Bergauer, T.Brandstetter, J.Dragicevic, M.Eroe, J.Del Valle, A. EscalanteFlechl, M.Fruehwirth, R.Ghete, V. M.Hrubec, J.Jeitler, M.Krammer, N.Kraetschmer, ILiko, D.Madlener, T.Mikulec, IRad, N.Rohringer, H.Schieck, J.Schoefbeck, R.Spanring, M.Spitzbart, D.Taurok, A.Waltenberger, W.Wittmann, J.Wulz, C-EZarucki, M.Chekhovsky, VMossolov, VGonzalez, J. SuarezDe Wolf, E. A.Di Croce, D.Janssen, X.Lauwers, J.Pieters, M.Van De Klundert, M.Van Haevermaet, H.Van Mechelen, P.Van Remortel, N.Abu Zeid, S.Blekman, F.D'Hondt, J.De Bruyn, IDe Clercq, J.Deroover, K.Flouris, G.Lontkovskyi, D.Lowette, S.Marchesini, IMoortgat, S.Moreels, L.Python, Q.Skovpen, K.Tavernier, S.Van Doninck, W.Van Mulders, P.Van Parijs, IBeghin, 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.Vander Velde, C.Vanlaer, R.Vannerom, D.Yonamine, R.Bakhshiansohi, H.Bondu, O.Brochet, S.Bruno, G.Caputo, C.Caudron, A.David, R.De Visscher, S.Delaere, C.Delcourt, M.Francois, B.Giammanco, A.Krintiras, G.Lemaitre, VMagitteri, 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, R.Belchior Batista Das Chagas, E.Carvalho, W.Chinellato, J.Coelho, E.Da Costa, E. M.Da Silveira, G. G.De Jesus Damiao, D.Fonseca De Souza, S.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, R.Marinov, A.Misheva, M.Rodozov, M.Shopova, M.Sultanov, G.Dimitrov, A.Litov, L.Pavlov, B.Petkov, R.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, ISculac, T.Antunovic, Z.Kovac, M.Brigljevic, VFerencek, 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.Fingers, M.Finger, M., Jr.Carrera Jarrin, E.Abdalla, H.Abdelalim, A. A.Salama, E.Bhowmik, S.De Oliveira, A. Carvalho AntunesDewanjee, R. 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C.Collard, C.Conte, E.Coubez, X.Drouhin, F.Fontaine, J-CGele, D.Goerlach, U.Jansova, M.Juillot, R.Le Bihan, A-CTonon, N.Van Hove, R.Gadrat, S.Beauceron, S.Bernet, C.Boudoul, G.Chanon, N.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.Lattaud, H.Lethuillier, M.Mirabito, L.Pequegnot, A. L.Perries, S.Popov, A.Sordini, VVander Donckt, M.Viret, S.Zhang, S.Toriashvili, T.Tsamalaidze, Z.Autermann, C.Feld, L.Kiesel, M. K.Klein, K.Lipinski, M.Preuten, M.Rauch, M. P.Schomakers, C.Schulz, J.Teroerde, M.Wittmer, B.Zhukov, VAlbert, A.Duchardt, D.Endres, M.Erdmann, M.Erdweg, S.Esch, T.Fischer, R.Ghosh, S.Gueth, A.Hebbeker, T.Heidemann, C.Hoepfner, K.Knutzen, S.Merschmeyer, M.Meyer, A.Millet, P.Mukherjee, S.Pook, T.Radziej, M.Reithler, H.Rieger, M.Scheuch, F.Teyssier, D.Thueer, S.Fluegge, G.Kargoll, B.Kress, T.Kuensken, A.Mueller, T.Nehrkorn, A.Nowack, A.Pistone, C.Pooth, O.Stahl, A.Martin, M. 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CentisDreyer, T.Garutti, E.Gonzalez, D.Haller, J.Hinzmann, A.Hoffmann, M.Karavdina, A.Kasieczka, G.Klanner, R.Kogler, R.Kovalchuk, N.Kurz, S.Kutzner, VLange, J.Marconi, D.Multhaup, J.Niedziela, M.Nowatschin, D.Peiffer, T.Perieanu, A.Reimers, A.Scharf, C.Schleper, R.Schmidt, A.Schumann, S.Schwandt, J.Sonneveld, J.Stadie, H.Steinbrueck, G.Stober, F. M.Stoever, M.Troendle, D.Usai, E.Vanhoefer, A.Vormwald, B.Akbiyik, M.Barth, C.Baselga, M.Baur, S.Butz, E.Caspart, R.Chwalek, T.Colombo, F.De Boer, W.Dierlamm, A.Faltermann, N.Freund, B.Friese, R.Giffels, M.Harrendorf, M. A.Hartmann, F.Heindl, S. M.Husemann, U.Kassel, F.Kudella, S.Mildner, H.Mozer, M. U.Mueller, ThPlagge, M.Quast, G.Rabbertz, K.Schroeder, M.Shvetsov, ISieber, G.Simonis, H. 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Issue Date
10-6월-2019
Publisher
ELSEVIER
Keywords
CMS; Physics; Higgs; Diphoton
Citation
PHYSICS LETTERS B, v.793, pp.320 - 347
Indexed
SCIE
SCOPUS
Journal Title
PHYSICS LETTERS B
Volume
793
Start Page
320
End Page
347
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/126193
DOI
10.1016/j.physletb.2019.03.064
ISSN
0370-2693
Abstract
The results of a search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV decaying into two photons are presented. The analysis uses the data set collected with the CMS experiment in proton-proton collisions during the 2012 and 2016 LHC running periods. The data sample corresponds to an integrated luminosity of 19.7 (35.9) fb(-1) at root s = 8 (13) TeV. The expected and observed 95% confidence level upper limits on the product of the cross section and branching fraction into two photons are presented. The observed upper limit for the 2012 (2016) data set ranges from 129 (161) fb to 31 (26) fb. The statistical combination of the results from the analyses of the two data sets in the common mass range between 80 and 110 GeV yields an upper limit on the product of the cross section and branching fraction, normalized to that for a standard model-like Higgs boson, ranging from 0.7 to 0.2, with two notable exceptions: one in the region around the Z boson peak, where the limit rises to 1.1, which may be due to the presence of Drell-Yan dielectron production where electrons could be misidentified as isolated photons, and a second due to an observed excess with respect to the standard model prediction, which is maximal for a mass hypothesis of 95.3 GeV with a local (global) significance of 2.8 (1.3) standard deviations. (C) 2019 The Author(s). Published by Elsevier B.V.
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