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@article{Khachatryan:2016:10.1103/PhysRevD.94.112009,
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 Knig, A and Krammer, M and Kratschmer, 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 Cornelis, T and De, Wolf EA and Knutsson, A and Lauwers, J and Luyckx, S 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 Keaveney, J and Lowette, S and Moortgat, S and Moreels, L and Olbrechts, A and Python, Q and Strom, D and Tavernier, S a},
doi = {10.1103/PhysRevD.94.112009},
journal = {Physical Review D},
title = {Searches for R-parity-violating supersymmetry in pp collisions at root s=8 TeV in final states with 0-4 leptons},
url = {http://dx.doi.org/10.1103/PhysRevD.94.112009},
volume = {94},
year = {2016}
}

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TY  - JOUR
AB  - Results are presented from searches for R-parity-violating supersymmetry in events produced in ppcollisions at √s=8  TeV at the LHC. Final states with 0, 1, 2, or multiple leptons are considered independently. The analysis is performed on data collected by the CMS experiment corresponding to an integrated luminosity of 19.5  fb−1. No excesses of events above the standard model expectations are observed, and 95% confidence level limits are set on supersymmetric particle masses and production cross sections. The results are interpreted in models featuring R-parity-violating decays of the lightest supersymmetric particle, which in the studied scenarios can be either the gluino, a bottom squark, or a neutralino. In a gluino pair production model with baryon number violation, gluinos with a mass less than 0.98 and 1.03 TeV are excluded, by analyses in a fully hadronic and one-lepton final state, respectively. An analysis in a dilepton final state is used to exclude bottom squarks with masses less than 307 GeV in a model considering bottom squark pair production. Multilepton final states are considered in the context of either strong or electroweak production of superpartners and are used to set limits on the masses of the lightest supersymmetric particles. These limits range from 300 to 900 GeV in models with leptonic and up to approximately 700 GeV in models with semileptonic R-parity-violating couplings.
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  - Knig,A
AU  - Krammer,M
AU  - Kratschmer,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  - Cornelis,T
AU  - De,Wolf EA
AU  - Knutsson,A
AU  - Lauwers,J
AU  - Luyckx,S
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  - Keaveney,J
AU  - Lowette,S
AU  - Moortgat,S
AU  - Moreels,L
AU  - Olbrechts,A
AU  - Python,Q
AU  - Strom,D
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  - Fasanella,G
AU  - Favart,L
AU  - Goldouzian,R
AU  - Grebenyuk,A
AU  - Karapostoli,G
AU  - Lenzi,T
AU  - Leonard,A
AU  - Maerschalk,T
AU  - Marinov,A
AU  - Randle-Conde,A
AU  - Seva,T
AU  - Vander,Velde C
AU  - Vanlaer,P
AU  - Yonamine,R
AU  - Zenoni,F
AU  - Zhang,F
AU  - Benucci,L
AU  - Cimmino,A
AU  - Crucy,S
AU  - Dobur,D
AU  - Fagot,A
AU  - Garcia,G
AU  - Gul,M
AU  - Mccartin,J
AU  - Rios,AAO
AU  - Poyraz,D
AU  - Ryckbosch,D
AU  - Salva,S
AU  - Schofbeck,R
AU  - Sigamani,M
AU  - Tytgat,M
AU  - Van,Driessche W
AU  - Yazgan,E
AU  - Zaganidis,N
AU  - Beluffi,C
AU  - Bondu,O
AU  - Brochet,S
AU  - Bruno,G
AU  - Caudron,A
AU  - Ceard,L
AU  - De,Visscher S
AU  - Delaere,C
AU  - Delcourt,M
AU  - Forthomme,L
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  - Hammad,GH
AU  - Alda,Junior WL
AU  - Alves,FL
AU  - Alves,GA
AU  - Brito,L
AU  - Correa,Martins Junior M
AU  - Hamer,M
AU  - Hensel,C
AU  - Moraes,A
AU  - Pol,ME
AU  - Teles,PR
AU  - Belchior,Batista Das Chagas E
AU  - Carvalho,W
AU  - Chinellato,J
AU  - Custodio,A
AU  - Da,Costa EM
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  - De,Souza
DO  - 10.1103/PhysRevD.94.112009
PY  - 2016///
SN  - 1550-7998
TI  - Searches for R-parity-violating supersymmetry in pp collisions at root s=8 TeV in final states with 0-4 leptons
T2  - Physical Review D
UR  - http://dx.doi.org/10.1103/PhysRevD.94.112009
UR  - http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000391016600002&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=1ba7043ffcc86c417c072aa74d649202
UR  - http://hdl.handle.net/10044/1/44846
VL  - 94
ER  -

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