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Search for narrow resonances using the dijet mass spectrum in pp collisions at root s=8 TeV

Authors
Chatrchyan, S.Khachatryan, V.Sirunyan, A. M.Tumasyan, A.Adam, W.Aguilo, E.Bergauer, T.Dragicevic, M.Eroe, J.Fabjan, C.Friedl, M.Fruehwirth, R.Ghete, V. M.Hoermann, N.Hrubec, J.Jeitler, M.Kiesenhofer, W.Knuenz, V.Krammer, M.Kraetschmer, I.Liko, D.Mikulec, I.Pernicka, M.Rabady, D.Rahbaran, B.Rohringer, C.Rohringer, H.Schoefbeck, R.Strauss, J.Taurok, A.Waltenberger, W.Wulz, C. -E.Mossolov, V.Shumeiko, N.Gonzalez, J. SuarezAlderweireldt, S.Bansal, M.Bansal, S.Cornelis, T.De Wolf, E. A.Janssen, X.Luyckx, S.Mucibello, L.Ochesanu, S.Roland, B.Rougny, R.Van Haevermaet, H.Van Mechelen, P.Van Remortel, N.Van Spilbeeck, A.Blekman, F.Blyweert, S.D'Hondt, J.Gonzalez Suarez, R.Kalogeropoulos, A.Maes, M.Olbrechts, A.Tavernier, S.Van Doninck, W.Van Mulders, P.Van Onsem, G. P.Villella, I.Clerbaux, B.De Lentdecker, G.Dero, V.Gay, A. P. R.Hreus, T.Leonard, A.Marage, P. E.Mohammadi, A.Reis, T.Thomas, L.Vander Velde, C.Vanlaer, P.Wang, J.Adler, V.Beernaert, K.Cimmino, A.Costantini, S.Garcia, G.Grunewald, M.Klein, B.Lellouch, J.Marinov, A.Mccartin, J.Ocampo Rios, A. A.Ryckbosch, D.Sigamani, M.Strobbe, N.Thyssen, F.Tytgat, M.Walsh, S.Yazgan, E.Zaganidis, N.Basegmez, S.Bruno, G.Castello, R.Ceard, L.Delaere, C.du Pree, T.Favart, D.Forthomme, L.Giammanco, A.Hollar, J.Lemaitre, V.Liao, J.Militaru, O.Nuttens, C.Pagano, D.Pin, A.Piotrzkowski, K.Selvaggi, M.Vizan Garcia, J. M.Beliy, N.Caebergs, T.Daubie, E.Hammad, G. H.Alves, G. A.Correa Martins Junior, M.Martins, T.Pol, M. E.Souza, M. H. G.Alda Junior, W. L.Carvalho, W.Chinellato, J.Custodio, A.Da Costa, E. M.De Jesus Damiao, D.De Oliveira Martins, C.Fonseca De Souza, S.Malbouisson, H.Malek, M.Matos Figueiredo, D.Mundim, L.Nogima, H.Prado Da Silva, W. L.Santoro, A.Soares Jorge, L.Sznajder, A.Tonelli Manganote, E. J.Vilela Pereira, A.Anjos, T. S.Bernardes, C. A.Dias, F. A.Fernandez Perez Tomei, T. R.Gregores, E. M.Lagana, C.Marinho, F.Mercadante, P. G.Novaes, S. F.Padula, Sandra S.Genchev, V.Iaydjiev, P.Piperov, S.Rodozov, M.Stoykova, S.Sultanov, G.Tcholakov, V.Trayanov, R.Vutova, M.Dimitrov, A.Hadjiiska, R.Kozhuharov, V.Litov, L.Pavlov, B.Petkov, P.Bian, J. G.Chen, G. M.Chen, H. S.Jiang, C. H.Liang, D.Liang, S.Meng, X.Tao, J.Wang, J.Wang, X.Wang, Z.Xiao, H.Xu, M.Zang, J.Zhang, Z.Asawatangtrakuldee, C.Ban, Y.Guo, Y.Li, W.Liu, S.Mao, Y.Qian, S. J.Teng, H.Wang, D.Zhang, L.Zou, W.Avila, C.Carrillo Montoya, C. A.Gomez, J. P.Gomez Moreno, B.Osorio Oliveros, A. F.Sanabria, J. C.Godinovic, N.Lelas, D.Plestina, R.Polic, D.Puljak, I.Antunovic, Z.Kovac, M.Brigljevic, V.Duric, S.Kadija, K.Luetic, J.Mekterovic, D.Morovic, S.Tikvica, L.Attikis, A.Mavromanolakis, G.Mousa, J.Nicolaou, C.Ptochos, F.Razis, P. A.Finger, M.Finger, M., Jr.Assran, Y.Elgammal, S.Kamel, A. EllithiAwad, A. M. KuotbMahmoud, M. A.Radi, A.Kadastik, M.Muentel, M.Murumaa, M.Raidal, M.Rebane, L.Tiko, A.Eerola, P.Fedi, G.Voutilainen, M.Harkonen, J.Heikkinen, A.Karimaki, V.Kinnunen, R.Kortelainen, M. J.Lampen, T.Lassila-Perini, K.Lehti, S.Linden, T.Luukka, P.Maenpaa, T.Peltola, T.Tuominen, E.Tuominiemi, J.Tuovinen, E.Ungaro, D.Wendland, L.Korpela, A.Tuuva, T.Besancon, M.Choudhury, S.Couderc, F.Dejardin, M.Denegri, D.Fabbro, B.Faure, J. L.Ferri, F.Ganjour, S.Givernaud, A.Gras, P.de Monchenault, G. HamelJarry, P.Locci, E.Malcles, J.Millischer, L.Nayak, A.Rander, J.Rosowsky, A.Titov, M.Baffioni, S.Beaudette, F.Benhabib, L.Bianchini, L.Bluj, M.Busson, P.Charlot, C.Daci, N.Dahms, T.Dalchenko, M.Dobrzynski, L.Florent, A.de Cassagnac, R. GranierHaguenauer, M.Mine, P.Mironov, C.Naranjo, I. N.Nguyen, M.Ochando, C.Paganini, P.Sabes, D.Salerno, R.Sirois, Y.Veelken, C.Zabi, A.Agram, J. -L.Andrea, J.Bloch, D.Bodin, D.Brom, J. -M.Chabert, E. 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HajHoehle, F.Kargoll, B.Kress, T.Kuessel, Y.Lingemann, J.Nowack, A.Nugent, I. M.Perchalla, L.Pooth, O.Sauerland, P.Stahl, A.Aldaya Martin, M.Asin, I.Bartosik, N.Behr, J.Behrenhoff, W.Behrens, U.Bergholz, M.Bethani, A.Borras, K.Burgmeier, A.Cakir, A.Calligaris, L.Campbell, A.Castro, E.Costanza, F.Dammann, D.Pardos, C. DiezDorland, T.Eckerlin, G.Eckstein, D.Flucke, G.Geiser, A.Glushkov, I.Gunnellini, P.Habib, S.Hauk, J.Hellwig, G.Jung, H.Kasemann, M.Katsas, P.Kleinwort, C.Kluge, H.Knutsson, A.Kraemer, M.Kruecker, D.Kuznetsova, E.Lange, W.Leonard, J.Lohmann, W.Lutz, B.Mankel, R.Marfin, I.Marienfeld, M.Melzer-Pellmann, I. -A.Meyer, A. B.Mnich, J.Mussgiller, A.Naumann-Emme, S.Novgorodova, O.Nowak, F.Olzem, J.Perrey, H.Petrukhin, A.Pitzl, D.Raspereza, A.Ribeiro Cipriano, P. 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M.Troendle, D.Ulrich, R.Wagner-Kuhr, J.Wayand, S.Weiler, T.Zeise, M.Anagnostou, G.Daskalakis, G.Geralis, T.Kesisoglou, S.Kyriakis, A.Loukas, D.Markou, A.Markou, C.Ntomari, E.Gouskos, L.Mertzimekis, T. J.Panagiotou, A.Saoulidou, N.Evangelou, I.Foudas, C.Kokkas, P.Manthos, N.Papadopoulos, I.Bencze, G.Hajdu, C.Hidas, P.Horvath, D.Sikler, F.Veszpremi, V.Vesztergombi, G.Zsigmond, A. J.Beni, N.Czellar, S.Molnar, J.Palinkas, J.Szillasi, Z.Karancsi, J.Raics, P.Trocsanyi, Z. L.Ujvari, B.Beri, S. B.Bhatnagar, V.Dhingra, N.Gupta, R.Kaur, M.Mehta, M. Z.Mittal, M.Nishu, N.Saini, L. K.Sharma, A.Singh, J. B.Kumar, AshokKumar, ArunAhuja, S.Bhardwaj, A.Choudhary, B. C.Malhotra, S.Naimuddin, M.Ranjan, K.Saxena, P.Sharma, V.Shivpuri, R. K.Banerjee, S.Bhattacharya, S.Chatterjee, K.Dutta, S.Gomber, B.Jain, Sa.Jain, Sh.Khurana, R.Modak, A.Mukherjee, S.Roy, D.Sarkar, S.Sharan, M.Abdulsalam, A.Dutta, D.Kailas, S.Kumar, V.Mohanty, A. K.Pant, L. M.Shukla, P.Aziz, T.Chatterjee, R. 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Issue Date
17-6월-2013
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW D, v.87, no.11
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW D
Volume
87
Number
11
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/127031
DOI
10.1103/PhysRevD.87.114015
ISSN
1550-7998
Abstract
Results are presented of a search for the production of new particles decaying to pairs of partons (quarks, antiquarks, or gluons), in the dijet mass spectrum in proton-proton collisions at root s = 8 TeV. The data sample corresponds to an integrated luminosity of 4.0 fb(-1), collected with the CMS detector at the LHC in 2012. No significant evidence for narrow resonance production is observed. Upper limits are set at the 95% confidence level on the production cross section of hypothetical new particles decaying to quark-quark, quark-gluon, or gluon-gluon final states. These limits are then translated into lower limits on the masses of new resonances in specific scenarios of physics beyond the standard model. The limits reach up to 4.8 TeV, depending on the model, and extend previous exclusions from similar searches performed at lower collision energies. For the first time mass limits are set for the Randall-Sundrum graviton model in the dijet channel.
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