Results are presented from a search for a narrow, spin-2 resonance decaying into a pair of Z bosons, with one Z-boson decaying into leptons (e(+)e(-) or mu(+)mu(-)) and the other into jets. An example of such a resonance is the Kaluza-Klein graviton, G(KK), predicted in Randall-Sundrum models. The analysis is based on a 4.9 fb(-1) sample of proton-proton collisions at a center-of-mass energy of 7 TeV, collected with the CMS detector at the LHC. Kinematic and topological properties including decay angular distributions are used to discriminate between signal and background. No evidence for a resonance is observed, and upper limits on the production cross sections times branching fractions are set. In two models that predict Z-boson spin correlations in graviton decays, graviton masses are excluded lower than a value which varies between 610 and 945 GeV, depending on the model and the strength of the graviton couplings. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved.
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SECTION B. - ISSN 0370-2693. - 718:4-5(2013), pp. 1208-1228. [10.1016/j.physletb.2012.11.063]
Search for a narrow, spin-2 resonance decaying to a pair of Z bosons in the q(q)over-barl(+)l(-) final state
Chatrchyan S; Khachatryan V; Sirunyan AM; Tumasyan A; Adam W; Aguilo E; Bergauer T; Dragicevic M; Eroe J; Fabjan C; Friedl M; Fruehwirth R; Ghete VM; Hammer J; Hormann N; Hrubec J; Jeitler M; Kiesenhofer W; Knuenz 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 R; 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 R; 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; Damiao DDJ; Martins T; Pol ME; Souza MHG; Alda WL; Carvalho W; Custodio A; Da Costa EM; Martins CDO; 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 R; 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 R; 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 S; Guo Y; Li W; Liu S; Mao Y; Qian SJ; Teng H; Wang D; Zhang L; Zhu B; 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; Khalil S; 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; Chariot C; Daci N; Dahms T; 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; Sordini V; Tschudi Y; Verdier P; Viret S; Tsamalaidze Z; Anagnostou G; Beranek S; Edelhoff M; Feld L; Heracleous N; Hindrichs O; Jussen R; Klein K; Merz J; Ostapchuk A; Perieanu A; Raupach E; Sammet J; Schael S; Sprenger D; Weber H; Wittmer B; Zhukov V; Ata M; Caudron J; Dietz Laursonn E; Duchardt D; Erdmann M; Fischer R; Guth A; Hebbeker T; Heidemann C; Hoepfner K; Klingebiel D; Kreuzer P; Magass C; Merschmeyer M; Meyer A; Olschewski M; Papacz P; Pieta H; Reithler H; Schmitz SA; Sonnenschein L; Steggemann J; Teyssier D; Weber M; Bontenackels M; Cherepanov V; Erdogan Y; Flugge G; Geenen H; Geisler M; Ahmad WH; Hoehle F; Kargoll B; Kress T; Kuessel Y; Nowack A; Perchalla L; Pooth O; Sauerland P; Stahl A; Martin MA; Behr J; Behrenhoff W; Behrens U; Bergholz M; Bethani A; Borras K; Burgmeier A; Cakir A; Calligaris L; Campbell A; Castro E; Costanza E; Dammann D; Pardos CD; Eckerlin G; Eckstein D; Flucke G; Geiser A; Glushkov I; Gunnellini P; Habib S; Hauk J; Hellwig G; Jung H; Kasemann M; Katsas P; Kleinwort C; Kluge H; Knutsson A; Kramer M; Krucker D; Kuznetsova E; Lange W; Lohmann W; Lutz B; Mankel R; Marfin I; Marienfeld M; Melzer Pellmann IA; Meyer AB; Mnich J; Mussgiller A; Naumann Emme S; Olzem J; Perrey H; Petrukhin A; Pitzl D; Raspereza A; Cipriano PMR; Riedl C; Ron E; Rosin M; Salfeld Nebgen J; 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2013-01-01
Abstract
Results are presented from a search for a narrow, spin-2 resonance decaying into a pair of Z bosons, with one Z-boson decaying into leptons (e(+)e(-) or mu(+)mu(-)) and the other into jets. An example of such a resonance is the Kaluza-Klein graviton, G(KK), predicted in Randall-Sundrum models. The analysis is based on a 4.9 fb(-1) sample of proton-proton collisions at a center-of-mass energy of 7 TeV, collected with the CMS detector at the LHC. Kinematic and topological properties including decay angular distributions are used to discriminate between signal and background. No evidence for a resonance is observed, and upper limits on the production cross sections times branching fractions are set. In two models that predict Z-boson spin correlations in graviton decays, graviton masses are excluded lower than a value which varies between 610 and 945 GeV, depending on the model and the strength of the graviton couplings. (C) 2012 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. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.