A search has been made for massive resonances decaying into a quark and a vector boson, qW or qZ, or a pair of vector bosons, WW, WZ, or ZZ, where each vector boson decays to hadronic final states. This search is based on a data sample corresponding to an integrated luminosity of 5.0 fb(-1) of proton-proton collisions collected in the CMS experiment at the LHC in 2011 at a center-of-mass energy of 7 TeV. For sufficiently heavy resonances the decay products of each vector boson are merged into a single jet, and the event effectively has a dijet topology. The background from QCD dijet events is reduced using recently developed techniques that resolve jet substructure. A 95% CL lower limit is set on the mass of excited quark resonances decaying into qW (qZ) at 2.38 TeV (2.15 TeV) and upper limits are set on the cross section for resonances decaying to qW, qZ, WW, WZ, or ZZ final states. (C) 2013 CERN. Published by Elsevier B.V. All rights reserved.
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SECTION B. - ISSN 0370-2693. - 723:4-5(2013), pp. 280-301. [10.1016/j.physletb.2013.05.040]
Search for heavy resonances in the W/Z-tagged dijet mass spectrum in pp collisions at 7 TeV
Chatrchyan S; Khachatryan V; Sirunyan AM; Tumasyan A; Adam W; Aguilo E; Bergauer T; Dragicevic M; Ero J; Fabjan C; Friedl M; Fruhwirth R; Ghete VM; Hammer J; Hormann N; Hrubec J; Jeitler M; Kiesenhofer W; Knunz V; Krammer M; Kratschmer I; Liko D; Mikulec I; Pernicka M; Rahbaran B; Rohringer C; Rohringer H; Schofbeck R; Strauss J; Taurok A; Waltenberger W; Walzel G; Widl E; Wulz CE; Mossolov V; Shumeiko N; Gonzalez JS; Bansal M; Bansal S; Cornelis T; De Wolf EA; Janssen X; Luyckx S; Mucibello L; Ochesanu S; Roland B; Rougny R; Selvaggi M; Staykova Z; Van Haevermaet H; Van Mechelen P; Van Remortel N; Van Spilbeeck A; Blekman F; Blyweert S; D'Hondt J; Suarez RG; Kalogeropoulos A; Maes M; Olbrechts A; Van Doninck W; Van Mulders P; Van Onsem GP; Villella I; Clerbaux B; De Lentdecker G; Dero V; Gay APR; Hreus T; Leonard A; Marage PE; Mohammadi A; Reis T; Thomas L; Vander Marcken G; 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; Rios AAO; Ryckbosch D; Strobbe N; Thyssen F; Tytgat M; Verwilligen P; 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; Schul N; Garcia JMV; Beliy N; Caebergs T; Daubie E; Hammad GH; Alves GA; Martins MC; Martins T; Pol ME; Souza MHG; Alda WL; Carvalho W; Custodio A; Da Costa EM; Damiao DD; Martins CD; De Souza SF; Figueiredo DM; Mundim L; Nogima H; Oguri V; Da Silva WLP; Santoro A; Jorge LS; Sznajder A; Anjos TS; Bernardes CA; Dias FA; Tomei TRFP; Gregores EM; Lagana C; Marinho F; Mercadante PG; Novaes SF; Padula SS; 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 JG; Chen GM; Chen HS; Jiang CH; 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 SJ; Teng H; Wang D; Zhang L; Zou W; Avila C; Gomez JP; Moreno BG; Oliveros AFO; Sanabria JC; Godinovic N; Lelas D; Plestina R; Polic D; Puljak I; Antunovic Z; Kovac M; Brigljevic V; Duric S; Kadija K; Luetic J; Morovic S; Attikis A; Galanti M; Mavromanolakis G; Mousa J; Nicolaou C; Ptochos F; Razis PA; Finger M; Finger M; Assran Y; Elgammal S; Kamel AE; Mahmoud MA; Radi A; Kadastik M; Muntel M; Raidal M; Rebane L; Tiko A; Eerola P; Fedi G; Voutilainen M; Harkonen J; Heikkinen A; Karimaki V; Kinnunen R; Kortelainen MJ; 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; Banzuzi K; Karjalainen A; Korpela A; Tuuva T; Besancon M; Choudhury S; Dejardin M; Denegri D; Fabbro B; Faure JL; Ferri F; Ganjour S; Givernaud A; Gras P; de Monchenault GH; Jarry P; Locci E; Malcles J; Millischer L; Nayak A; Rander J; Rosowsky A; Shreyber I; Titov M; Baffioni S; Beaudette F; Benhabib L; Bianchini L; Bluj M; Broutin C; Busson P; Charlot C; Daci N; Dahms T; Dalchenko M; Dobrzynski L; de Cassagnac RG; Haguenauer M; Mine P; Mironov C; Naranjo IN; Nguyen M; Ochando C; Paganini P; Sabes D; Salerno R; Sirois Y; Veelken C; Zabi A; Agram JL; Andrea J; Bloch D; Bodin D; Brom JM; Cardaci M; Chabert EC; Collard C; Conte E; Drouhin F; Ferro C; Fontaine JC; Gele D; Goerlach U; Juillot P; Le Bihan AC; Van Hove P; Fassi F; Mercier D; Beauceron S; Beaupere N; Bondu O; Boudoul G; Chasserat J; Chierici R; Contardo D; Depasse P; El Mamouni H; Fay J; Gascon S; Gouzevitch M; Ille B; Kurca T; Lethuillier M; Mirabito L; Perries S; Sgandurra L; Sordini V; Tschudi Y; Verdier P; Viret S; Tsamalaidze Z; Anagnostou G; Autermann C; Beranek S; Edelhoff M; Feld L; Heracleous N; Hindrichs O; Jussen R; Klein K; Merz J; Ostapchuk A; Perieanu A; Raupach F; Sammet J; Schael S; Sprenger D; Weber H; Wittmer B; Zhukov V; Ata M; Caudron J; Dietz Laursonn E; Duchardt D; 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2013-01-01
Abstract
A search has been made for massive resonances decaying into a quark and a vector boson, qW or qZ, or a pair of vector bosons, WW, WZ, or ZZ, where each vector boson decays to hadronic final states. This search is based on a data sample corresponding to an integrated luminosity of 5.0 fb(-1) of proton-proton collisions collected in the CMS experiment at the LHC in 2011 at a center-of-mass energy of 7 TeV. For sufficiently heavy resonances the decay products of each vector boson are merged into a single jet, and the event effectively has a dijet topology. The background from QCD dijet events is reduced using recently developed techniques that resolve jet substructure. A 95% CL lower limit is set on the mass of excited quark resonances decaying into qW (qZ) at 2.38 TeV (2.15 TeV) and upper limits are set on the cross section for resonances decaying to qW, qZ, WW, WZ, or ZZ final states. (C) 2013 CERN. Published by Elsevier B.V. All rights reserved.
Citazione
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione.
