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Search for electroweak production of charginos in final states with two T leptons in pp collisions at root s=8 TeV

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Title: Search for electroweak production of charginos in final states with two T leptons in pp collisions at root s=8 TeV
Authors: Khachatryan, V
Sirunyan, AM
Tumasyan, A
Adam, W
Asilar, E
Bergauer, T
Brandstetter, J
Brondolin, E
Dragicevic, M
Eroe, J
Flechl, M
Friedl, M
Fruehwirth, R
Ghete, VM
Hartl, C
Hoermann, N
Hrubec, J
Jeitler, M
Koenig, A
Kraetschmer, I
Liko, D
Matsushita, T
Mikulec, I
Rabady, D
Rad, N
Rahbaran, B
Rohringer, H
Schieck, J
Strauss, J
Treberer-Treberspurg, W
Waltenberger, W
Wulz, C-E
Mossolov, V
Shumeiko, N
Gonzalez, JS
Alderweireldt, S
De Wolf, EA
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
Daci, N
De Bruyn, I
Deroover, K
Heracleous, N
Lowette, S
Moortgat, S
Moreels, L
Olbrechts, A
Python, Q
Tavernier, S
Van Doninck, W
Van Mulders, P
Van Parijs, I
Brun, H
Caillol, C
Clerbaux, B
De Lentdecker, G
Delannoy, H
Fasanella, G
Favart, L
Goldouzian, R
Grebenyuk, A
Karapostoli, G
Lenzi, T
Leonard, A
Luetic, J
Maer-Schalk, T
Marinov, A
Randle-Conde, A
Seva, T
Velde, CV
Vanlaer, P
Yonamine, R
Zenoni, F
Zhang, F
Cimmino, A
Cornelis, T
Dobur, D
Fagot, A
Garcia, G
Gul, M
Poyraz, D
Salva, S
Schofbeck, R
Sharma, A
Tytgat, M
Van Driessche, W
Yazgan, E
Zaganidis, N
Bakhshiansohi, H
Beluffi, C
Bondu, O
Brochet, S
Bruno, G
Caudron, A
De Visscher, S
Delaere, C
Delcourt, M
Francois, B
Giammanco, A
Jafari, A
Jez, P
Komm, M
Lemaitre, V
Magitteri, A
Mertens, A
Musich, M
Nuttens, C
Piotrzkowski, K
Quertenmont, L
Selvaggi, M
Marono, MV
Wertz, S
Beliy, N
Alda Junior, WL
Alves, FL
Alves, GA
Brito, L
Hensel, C
Moraes, A
Pol, ME
Rebello Teles, P
Belchior Batista Das Chagas, E
Chinellato, J
Custodio, A
Da Costa, EM
Da Silveira, GG
De Jesus Damiao, D
De Oliveira Martins, C
Fonseca De Souza, S
Huertas Guativa, LM
Malbouisson, H
Matos Figueiredo, D
Mora Herrera, C
Mundim, L
Nogima, H
Prado Da Silva, WL
Santoro, A
Sznajder, A
Tonelli Manganote, EJ
Vilela Pereira, A
Ahuja, S
Bernardes, CA
Dogra, S
Fernandez Perez Tomei, TR
Gregores, EM
Mercadante, PG
Moon, CS
Novaes, SF
Padula, SS
Romero Abad, D
Ruiz Vargas, JC
Aleksandrov, A
Hadjiiska, R
Iaydjiev, P
Rodozov, M
Stoykova, S
Sultanov, G
Vu-Tova, M
Dimitrov, A
Glushkov, I
Litov, L
Pavlov, B
Petkov, P
Fang, W
Ahmad, M
Bian, JG
Chen, GM
Chen, HS
Chen, M
Chen, Y
Cheng, T
Jiang, CH
Leggat, D
Liu, Z
Romeo, F
Shaheen, SM
Spiezia, A
Tao, J
Wang, C
Wang, Z
Zhang, H
Zhao, J
Ban, Y
Chen, G
Li, Q
Liu, S
Mao, Y
Qian, SJ
Wang, D
Xu, Z
Avila, C
Cabrera, A
Chaparro Sierra, LF
Florez, C
Gomez, JP
Gonzalez Hernandez, CF
Ruiz Alvarez, JD
Sanabria, JC
Godinovic, N
Lelas, D
Puljak, I
Cipriano, PMR
Sculac, T
Antunovic, Z
Kovac, M
Brigljevic, V
Ferencek, D
Kadija, K
Micanovic, S
Sudic, L
Susa, T
Attikis, A
Mavromanolakis, G
Mousa, J
Nicolaou, C
Ptochos, F
Razis, PA
Rykaczewski, H
Finger, M
Finger, M
Carrera Jarrin, E
Kamel, AE
Mahmoud, MA
Radi, A
Kamel, AE
Mahmoud, MA
Radi, A
Calpas, B
Kadastik, M
Murumaa, M
Perrini, L
Raidal, M
Tiko, A
Veelken, C
Eerola, P
Pekkanen, J
Voutilainen, M
Harkonen, J
Karimaki, V
Kinnunen, R
Lampen, T
Lassila-Perini, K
Lehti, S
Linden, T
Luukka, P
Tuominiemi, J
Tuovinen, E
Wendland, L
Talvitie, J
Tuuva, T
Besancon, M
Couderc, F
Dejardin, M
Denegri, D
Fabbro, B
Faure, JL
Favaro, C
Ferri, F
Ganjour, S
Ghosh, S
Givernaud, A
Gras, P
De Monchenault, GH
Jarry, P
Kucher, I
Locci, E
Machet, M
Malcles, J
Rander, J
Rosowsky, A
Titov, M
Zghiche, A
Abdulsalam, A
Antropov, I
Baffioni, S
Beaudette, F
Busson, P
Cadamuro, L
Chapon, E
Charlot, C
Davignon, O
De Cassagnac, RG
Jo, M
Lisniak, S
Mine, P
Nguyen, M
Ochando, C
Ortona, G
Paganini, P
Pigard, P
Regnard, S
Salerno, R
Sirois, Y
Strebler, T
Yilmaz, Y
Zabi, A
Agram, J-L
Andrea, J
Aubin, A
Bloch, D
Brom, J-M
Buttignol, M
Chabert, EC
Chanon, N
Collard, C
Conte, E
Coubez, X
Fontaine, J-C
Gele, D
Goerlach, U
Le Bihan, A-C
Skovpen, K
Van Hove, P
Gadrat, S
Beauceron, S
Bernet, C
Boudoul, G
Bouvier, E
Montoya, CAC
Chierici, R
Contardo, D
Courbon, B
Depasse, P
El Mamouni, H
Fan, J
Fay, J
Gascon, S
Gouzevitch, M
Grenier, G
Ille, B
Lagarde, F
Laktineh, IB
Lethuillier, M
Mirabito, L
Pequegnot, AL
Perries, S
Popov, A
Sabes, D
Sordini, V
Donckt, MV
Verdier, P
Viret, S
Toriashvili, T
Tsamalaidze, Z
Autermann, C
Beranek, S
Feld, L
Heister, A
Kiesel, MK
Klein, K
Lipinski, M
Ostapchuk, A
Preuten, M
Raupach, F
Schael, S
Schomakers, C
Schulte, JF
Schulz, J
Verlage, T
Weber, H
Zhukov, V
Brodski, M
Dietz-Laursonn, E
Duchardt, D
Endres, M
Erdmann, M
Erdweg, S
Esch, T
Fischer, R
Gueth, A
Hamer, M
Hebbeker, T
Heidemann, C
Hoepfner, K
Knutzen, S
Merschmeyer, M
Meyer, A
Millet, P
Mukherjee, S
Olschewski, M
Padeken, K
Pook, T
Radziej, M
Reithler, H
Rieger, M
Scheuch, F
Sonnenschein, L
Teyssier, D
Thueer, S
Cherepanov, V
Fluegge, G
Ahmad, WH
Hoehle, F
Kargoll, B
Kress, T
Kuensken, A
Lingemann, J
Mueller, T
Nehrkorn, A
Nowack, A
Nugent, IM
Pistone, C
Pooth, O
Stahl, A
Martin, MA
Asawatangtrakuldee, C
Beernaert, K
Behnke, O
Behrens, U
Bin Anuar, AA
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Campbell, A
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Eckerlin, G
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Kruecker, D
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Melzer-Pellmann, I-A
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Woods, N
Item Type: Journal Article
Abstract: Results are presented from a search for the electroweak production of supersymmetric particles in pp collisions in final states with two τ 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 τ 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 τ 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 τ sleptons as a function of mass, assuming a massless neutralino.
Issue Date: 4-Apr-2017
Date of Acceptance: 12-Mar-2017
URI: http://hdl.handle.net/10044/1/48100
DOI: https://dx.doi.org/10.1007/JHEP04(2017)018
ISSN: 1029-8479
Publisher: SPRINGER
Journal / Book Title: JOURNAL OF HIGH ENERGY PHYSICS
Volume: 2017
Issue: 4
Copyright Statement: © 2017 The Author(s). Open Access. This article is distributed under the terms of the Creative Commons Attribution License ( CC-BY 4.0 https://creativecommons.org/licenses/by/4.0/), which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited.
Keywords: Science & Technology
Physical Sciences
Physics, Particles & Fields
Physics
Hadron-Hadron scattering (experiments)
Supersymmetry
HADRON COLLIDERS
SUPERGAUGE TRANSFORMATIONS
MEASURING MASSES
CROSS-SECTION
ENERGY
01 Mathematical Sciences
02 Physical Sciences
Publication Status: Published
Open Access location: https://link.springer.com/article/10.1007/JHEP04(2017)018
Article Number: ARTN 018
Appears in Collections:Physics
High Energy Physics



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