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@article{Khachatryan:2017:10.1007/JHEP04(2017)018,
author = {Khachatryan, V and Sirunyan, AM and Tumasyan, A and Adam, W and Asilar, E and Bergauer, T and Brandstetter, J and Brondolin, E and Dragicevic, M and Eroe, J and Flechl, M and Friedl, M and Fruehwirth, R and Ghete, VM and Hartl, C and Hoermann, N and Hrubec, J and Jeitler, M and Koenig, A and Kraetschmer, I and Liko, D and Matsushita, T and Mikulec, I and Rabady, D and Rad, N and Rahbaran, B and Rohringer, H and Schieck, J and Strauss, J and Treberer-Treberspurg, W and Waltenberger, W and Wulz, C-E and Mossolov, V and Shumeiko, N and Gonzalez, JS and Alderweireldt, S and De, Wolf EA and Janssen, X and Lauwers, J and Van, De Klundert M and Van, Haevermaet H and Van, Mechelen P and Van, Remortel N and Van, Spilbeeck A and Abu, Zeid S and Blekman, F and D'Hondt, J and Daci, N and De, Bruyn I and Deroover, K and Heracleous, N and Lowette, S and Moortgat, S and Moreels, L and Olbrechts, A and Python, Q and Tavernier, S and Van, Doninck W and Van, Mulders P and Van, Parijs I and Brun, H and C},
doi = {10.1007/JHEP04(2017)018},
journal = {JOURNAL OF HIGH ENERGY PHYSICS},
title = {Search for electroweak production of charginos in final states with two T leptons in pp collisions at root s=8 TeV},
url = {http://dx.doi.org/10.1007/JHEP04(2017)018},
volume = {2017},
year = {2017}
}

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TY  - JOUR
AB  - 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.
AU  - Khachatryan,V
AU  - Sirunyan,AM
AU  - Tumasyan,A
AU  - Adam,W
AU  - Asilar,E
AU  - Bergauer,T
AU  - Brandstetter,J
AU  - Brondolin,E
AU  - Dragicevic,M
AU  - Eroe,J
AU  - Flechl,M
AU  - Friedl,M
AU  - Fruehwirth,R
AU  - Ghete,VM
AU  - Hartl,C
AU  - Hoermann,N
AU  - Hrubec,J
AU  - Jeitler,M
AU  - Koenig,A
AU  - Kraetschmer,I
AU  - Liko,D
AU  - Matsushita,T
AU  - Mikulec,I
AU  - Rabady,D
AU  - Rad,N
AU  - Rahbaran,B
AU  - Rohringer,H
AU  - Schieck,J
AU  - Strauss,J
AU  - Treberer-Treberspurg,W
AU  - Waltenberger,W
AU  - Wulz,C-E
AU  - Mossolov,V
AU  - Shumeiko,N
AU  - Gonzalez,JS
AU  - Alderweireldt,S
AU  - De,Wolf EA
AU  - Janssen,X
AU  - Lauwers,J
AU  - Van,De Klundert M
AU  - Van,Haevermaet H
AU  - Van,Mechelen P
AU  - Van,Remortel N
AU  - Van,Spilbeeck A
AU  - Abu,Zeid S
AU  - Blekman,F
AU  - D'Hondt,J
AU  - Daci,N
AU  - De,Bruyn I
AU  - Deroover,K
AU  - Heracleous,N
AU  - Lowette,S
AU  - Moortgat,S
AU  - Moreels,L
AU  - Olbrechts,A
AU  - Python,Q
AU  - Tavernier,S
AU  - Van,Doninck W
AU  - Van,Mulders P
AU  - Van,Parijs I
AU  - Brun,H
AU  - Caillol,C
AU  - Clerbaux,B
AU  - De,Lentdecker G
AU  - Delannoy,H
AU  - Fasanella,G
AU  - Favart,L
AU  - Goldouzian,R
AU  - Grebenyuk,A
AU  - Karapostoli,G
AU  - Lenzi,T
AU  - Leonard,A
AU  - Luetic,J
AU  - Maer-Schalk,T
AU  - Marinov,A
AU  - Randle-Conde,A
AU  - Seva,T
AU  - Velde,CV
AU  - Vanlaer,P
AU  - Yonamine,R
AU  - Zenoni,F
AU  - Zhang,F
AU  - Cimmino,A
AU  - Cornelis,T
AU  - Dobur,D
AU  - Fagot,A
AU  - Garcia,G
AU  - Gul,M
AU  - Poyraz,D
AU  - Salva,S
AU  - Schofbeck,R
AU  - Sharma,A
AU  - Tytgat,M
AU  - Van,Driessche W
AU  - Yazgan,E
AU  - Zaganidis,N
AU  - Bakhshiansohi,H
AU  - Beluffi,C
AU  - Bondu,O
AU  - Brochet,S
AU  - Bruno,G
AU  - Caudron,A
AU  - De,Visscher S
AU  - Delaere,C
AU  - Delcourt,M
AU  - Francois,B
AU  - Giammanco,A
AU  - Jafari,A
AU  - Jez,P
AU  - Komm,M
AU  - Lemaitre,V
AU  - Magitteri,A
AU  - Mertens,A
AU  - Musich,M
AU  - Nuttens,C
AU  - Piotrzkowski,K
AU  - Quertenmont,L
AU  - Selvaggi,M
AU  - Marono,MV
AU  - Wertz,S
AU  - Beliy,N
AU  - Alda,Junior WL
AU  - Alves,FL
AU  - Alves,GA
AU  - Brito,L
AU  - Hensel,C
AU  - Moraes,A
AU  - Pol,ME
AU  - Rebello,Teles P
AU  - Belchior,Batista Das Chagas E
AU  - Chinellato,J
AU  - Custodio,A
AU  - Da,Costa EM
AU  - Da,Silveira GG
AU  - De,Jesus Damiao D
AU  - De,Oliveira Martins C
AU  - Fonseca,De Souza S
AU  - Huertas,Guativa LM
AU  - Malbouisson,H
AU  - Matos,Figueiredo D
AU  - Mora,Herrera C
AU  - Mundim,L
AU  - Nogima,H
AU  - Prado,Da Silva WL
AU  - Santoro,A
AU  - Sznajder,A
AU  - Tonelli,Manganote EJ
AU  - Vilela,Pereira A
AU  - Ahuja,S
AU  - Bernardes,CA
AU  - Dogra,S
AU  - Fernandez,Perez Tomei TR
AU  - Gregores,EM
AU  - Mercadante,PG
AU  - Moon,CS
AU  - Novaes,SF
AU  - Padula,SS
AU  - Romero,Abad D
AU  - Ruiz,Vargas JC
AU  - Al
DO  - 10.1007/JHEP04(2017)018
PY  - 2017///
SN  - 1029-8479
TI  - Search for electroweak production of charginos in final states with two T leptons in pp collisions at root s=8 TeV
T2  - JOURNAL OF HIGH ENERGY PHYSICS
UR  - http://dx.doi.org/10.1007/JHEP04(2017)018
UR  - http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000398449400010&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=1ba7043ffcc86c417c072aa74d649202
UR  - http://hdl.handle.net/10044/1/48100
VL  - 2017
ER  -

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