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Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at √s=8 TeV using the αT variable

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Title: Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at √s=8 TeV using the αT variable
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
Krammer, M
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
Cornelis, T
De Wolf, EA
Janssen, X
Knutsson, A
Lauwers, J
Luyckx, S
Van de Klundert, M
Van Haevermaet, H
Van Mechelen, R
Van Remortel, N
Van Spilbeeck, A
Abu Zeid, S
Blekman, F
D'Hondt, J
Daci, N
De Bruyn, I
Deroover, K
Heracleous, N
Keaveney, J
Lowette, S
Moortgat, S
Moreels, L
Olbrechts, A
Python, Q
Strom, D
Tavernier, S
Van Doninck, W
Van Mulders, R
Van Parijs, I
Brun, H
Caillol, C
Clerbaux, B
De Lentdecker, G
Fasanella, G
Favart, L
Goldouzian, R
Grebenyuk, A
Karapostoli, G
Lenzi, T
Leonard, A
Maerschalk, T
Marinov, A
Randle-Conde, A
Seva, T
Vander Velde, C
Vanlaer, R
Yonamine, R
Zenoni, F
Zhang, F
Benucci, L
Cimmino, A
Crucy, S
Dobur, D
Fagot, A
Garcia, G
Gul, M
Mccartin, J
Rios, AAO
Poyraz, D
Ryckbosch, D
Salva, S
SchOfbeck, R
Sigamani, M
Tytgat, M
Van Driessche, W
Yazgan, E
Zaganidis, N
Beluffi, C
Bondu
Brochet, S
Bruno, G
Caudron, A
Ceard, L
De Visscher, S
Delaere, C
Delcourt, M
Forthomme, L
Francois, B
Giammanco, A
Jafari, A
Jez, R
Komm, M
Lemaitre, V
Magitteri, A
Mertens, A
Musich, M
Nuttens, C
Piotrzkowski, K
Quertenmont, L
Selvaggi, M
Marono, MV
Wertz, S
Beliy, N
Hammad, GH
Alda Junior, WL
Alves, FL
Alves, GA
Brito, L
Correa Martins Junior, M
Hamer, M
Hensel, C
Moraes, A
Pol, ME
Rebello Teles, P
Belchior Batista Das Chagas, E
Carvalho, W
Chinellato, J
Custodio, A
Da Costa, EM
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
De Souza Santos, A
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, R
Rodozov, M
Stoykova, S
Sultanov, G
Vutova, M
Dimitrov, A
Glushkov, I
Litov, L
Pavlov, B
Petkov, R
Fang, W
Ahmad, M
Bian, JG
Chen, GM
Chen, HS
Chen, M
Cheng, T
Du, R
Jiang, CH
Leggat, D
Plestina, R
Romeo, F
Shaheen, SM
Spiezia, A
Tao, J
Wang, C
Wang, Z
Zhang, H
Asawatangtrakuldee, C
Ban, Y
Li, Q
Liu, S
Mao, Y
Qian, SJ
Wang, D
Xu, Z
Avila, C
Cabrera, A
Chaparro Sierra, LF
Florez, C
Gomez, JP
Gomez Moreno, B
Sanabria, JC
Godinovic, N
Lelas, D
Puljak, I
Cipriano, PMR
Antunovic, Z
Kovac, M
Brigljevic, V
Ferencek, D
Kadija, K
Luetic, J
Micanovic, S
Sudic, L
Attikis, A
Mavromanolakis, G
Mousa, J
Nicolaou, C
Ptochos, F
Razis, PA
Rykaczewski, H
Fingers, M
Finger, M
Carrera Jarrin, E
Assran, Y
Kamel, AE
Mahrous, A
Radi, A
Calpas, B
Kadastik, M
Murumaa, M
Perrini, L
Raidal, M
Tiko, A
Veelken, C
Eerola, R
Pekkanen, J
Voutilainen, M
Harkonen, J
Karimaki, V
Kinnunen, R
Lampen, T
Lassila-Perini, K
Lehti, S
Linden, T
Luukka
Peltola, T
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
Givernaud, A
Gras, R
De Monchenault, GH
Jarry, R
Locci, E
Machet, M
Malcles, J
Rander, J
Rosowsky, A
Titov, M
Zghiche, A
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Beaudette, F
Busson, R
Cadamuro, L
Chapon, E
Charlot, C
Davignon, O
Dobrzynski, L
Cassagnac, RGD
Jo, M
Lisniak, S
Mine, R
Naranjo, IN
Nguyen, M
Ochando, C
Ortona, G
Paganini, R
Pigard, R
Regnard, S
Salerno, R
Sirois, Y
Strebler, T
Yilmaz, Y
Zabi, A
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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
Goetzmann, C
Le Bihan, A-C
Merlin, JA
Skovpen, K
Van Hove, R
Gadrat, S
Beauceron, S
Bernet, C
Boudoul, G
Bouvier, E
Montoya, CAC
Chierici, R
Contardo, D
Courbon, B
Depasse, R
El Mamouni, H
Fan, J
Fay, J
Gascon, S
Gouzevitch, M
Ille, B
Lagarde, F
Laktineh, IB
Lethuillier, M
Mirabito, L
Pequegnot, AL
Perries, S
Popov, A
Alvarez, JDR
Sabes, D
Sordini, V
Vander Donckt, M
Verdier, R
Viret, S
Toriashvili, T
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Autermann, C
Beranek, S
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Kiesel, MK
Klein, K
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Schulz, J
Verlage, T
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Duchardt, D
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Hoepfner, K
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Merschmeyer, M
Meyer, A
Millet, R
Mukherjee, S
Olschewski, M
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Papacz, P
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Reithler, H
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Item Type: Journal Article
Abstract: An inclusive search is performed for supersymmetry in final states containing jets and an apparent imbalance in transverse momentum, View the MathML sourcep→Tmiss, due to the production of unobserved weakly interacting particles in pp collisions at a centre-of-mass energy of 8 TeV. The data, recorded with the CMS detector at the CERN LHC, correspond to an integrated luminosity of 18.5 fb−1. The dimensionless kinematic variable αTαT is used to discriminate between events with genuine View the MathML sourcep→Tmiss associated with unobserved particles and spurious values of View the MathML sourcep→Tmiss arising from jet energy mismeasurements. No excess of event yields above the expected standard model backgrounds is observed. The results are interpreted in terms of constraints on the parameter space of several simplified models of supersymmetry that assume the pair production of top squarks. The search provides sensitivity to a broad range of top squark (View the MathML sourcet˜) decay modes, including the two-body decay View the MathML sourcet˜→cχ˜10, where c is a charm quark and View the MathML sourceχ˜10 is the lightest neutralino, as well as the four-body decay View the MathML sourcet˜→bff¯′χ˜10, where b is a bottom quark and f and View the MathML sourcef¯′ are fermions produced in the decay of an intermediate off-shell W boson. These modes dominate in scenarios in which the top squark and lightest neutralino are nearly degenerate in mass. For these modes, top squarks with masses as large as 260 and 225 GeV are excluded, respectively, for the two- and four-body decays.
Issue Date: 10-Feb-2017
Date of Acceptance: 6-Feb-2017
URI: http://hdl.handle.net/10044/1/48196
DOI: https://dx.doi.org/10.1016/j.physletb.2017.02.007
ISSN: 0370-2693
Publisher: ELSEVIER
Start Page: 403
End Page: 430
Journal / Book Title: PHYSICS LETTERS B
Volume: 767
Copyright Statement: © 2017 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/ ).
Keywords: Science & Technology
Physical Sciences
Astronomy & Astrophysics
Physics, Nuclear
Physics, Particles & Fields
Physics
CMS
SUSY
Jets
Missing transverse momentum
AlphaT
LIGHT STOP DECAYS
HADRON COLLIDERS
SUPERSYMMETRY
Nuclear & Particles Physics
0202 Atomic, Molecular, Nuclear, Particle And Plasma Physics
Publication Status: Published
Open Access location: http://www.sciencedirect.com/science/article/pii/S0370269317300977
Appears in Collections:Physics
High Energy Physics



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