The azimuthal anisotropy of charged particles in Pb-Pb collisions at root S-NN = 2.76 TeV is measured with the CMS detector at the LHC over an extended transverse momentum (p(T)) range up to approximately 60 GeV/c. The data cover both the low-p(T) region associated with hydrodynamic flow phenomena and the high-p(T) region where the anisotropies may reflect the path-length dependence of parton energy loss in the created medium. The anisotropy parameter (nu(2)) of the particles is extracted by correlating charged tracks with respect to the event-plane reconstructed by using the energy deposited in forward-angle calorimeters. For the six bins of collision centrality studied, spanning the range of 0-60% most-central events, the observed nu(2) values are found to first increase with p(T), reaching a maximum around p(T) = 3 GeV/c, and then to gradually decrease to almost zero, with the decline persisting up to at least p(T) = 40 GeV/c over the full centrality range measured.
Azimuthal Anisotropy of Charged Particles at High Transverse Momenta in Pb-Pb Collisions at root S-NN=2.76 TeV / Chatrchyan, S; Khachatryan, V; Sirunyan, Am; Tumasyan, A; Adam, W; Bergauer, T; Dragicevic, M; Ero, J; Fabjan, C; Friedl, M; Fruhwirth, R; Ghete, Vm; Hammer, J; Hormann, N; Hrubec, J; Jeitler, M; Kiesenhofer, W; Krammer, M; Liko, D; Mikulec, I; Pernicka, M; Rahbaran, B; Rohringer, C; Rohringer, H; Schofbeck, R; Strauss, J; Taurok, A; Teischinger, F; Wagner, P; Waltenberger, W; Walzel, G; Widl, E; Wulz, Ce; Mossolov, V; Shumeiko, N; Gonzalez, Js; Bansal, S; Cerny, K; Cornelis, T; De Wolf, Ea; Janssen, X; Luyckx, S; Maes, T; Mucibello, L; Ochesanu, S; Roland, B; Rougny, R; Selvaggi, M; 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; Charaf, O; Clerbaux, B; De Lentdecker, G; Dero, V; Gay, Apr; Hreus, T; Leonard, A; 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[10.1103/PhysRevLett.109.022301]
Azimuthal Anisotropy of Charged Particles at High Transverse Momenta in Pb-Pb Collisions at root S-NN=2.76 TeV
Chatrchyan S; Khachatryan V; Sirunyan AM; Tumasyan A; Adam W; Bergauer T; Dragicevic M; Ero J; Fabjan C; Friedl M; Fruhwirth R; Ghete VM; Hammer J; Hormann N; Hrubec J; Jeitler M; Kiesenhofer W; Krammer M; Liko D; Mikulec I; Pernicka M; Rahbaran B; Rohringer C; Rohringer H; Schofbeck R; Strauss J; Taurok A; Teischinger F; Wagner P; Waltenberger W; Walzel G; Widl E; Wulz CE; Mossolov V; Shumeiko N; Gonzalez JS; Bansal S; Cerny K; Cornelis T; De Wolf EA; Janssen X; Luyckx S; Maes T; Mucibello L; Ochesanu S; Roland B; Rougny R; Selvaggi M; 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; Charaf O; Clerbaux B; De Lentdecker G; Dero V; Gay APR; Hreus T; Leonard A; Marage PE; Reis T; Thomas L; Vander Velde C; Vanlaer P; 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; Vanelderen L; Verwilligen P; Walsh S; Yazgan E; Zaganidis N; Basegmez S; Bruno G; 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; Beliy N; Caebergs T; Daubie E; Hammad GH; Alves GA; Martins MC; Damiao DD; Martins T; Pol ME; Souza MHG; Alda WL; Carvalho W; Custodio A; Da Costa EM; Martins CD; De Souza SF; Figueiredo DM; Mundim L; Nogima H; Oguri V; Da Silva WLP; Santoro A; Do Amaral SMS; 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 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 S; Zhu B; Zou W; Avila C; Moreno BG; Oliveros AFO; Sanabria JC; Godinovic N; Lelas D; Plestina R; Polic D; Puljak I; Antunovic Z; Dzelalija M; 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; Azzolini V; 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; 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; 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2012-01-01
Abstract
The azimuthal anisotropy of charged particles in Pb-Pb collisions at root S-NN = 2.76 TeV is measured with the CMS detector at the LHC over an extended transverse momentum (p(T)) range up to approximately 60 GeV/c. The data cover both the low-p(T) region associated with hydrodynamic flow phenomena and the high-p(T) region where the anisotropies may reflect the path-length dependence of parton energy loss in the created medium. The anisotropy parameter (nu(2)) of the particles is extracted by correlating charged tracks with respect to the event-plane reconstructed by using the energy deposited in forward-angle calorimeters. For the six bins of collision centrality studied, spanning the range of 0-60% most-central events, the observed nu(2) values are found to first increase with p(T), reaching a maximum around p(T) = 3 GeV/c, and then to gradually decrease to almost zero, with the decline persisting up to at least p(T) = 40 GeV/c over the full centrality range measured.
Citazione
Azimuthal Anisotropy of Charged Particles at High Transverse Momenta in Pb-Pb Collisions at root S-NN=2.76 TeV / Chatrchyan, S; Khachatryan, V; Sirunyan, Am; Tumasyan, A; Adam, W; Bergauer, T; Dragicevic, M; Ero, J; Fabjan, C; Friedl, M; Fruhwirth, R; Ghete, Vm; Hammer, J; Hormann, N; Hrubec, J; Jeitler, M; Kiesenhofer, W; Krammer, M; Liko, D; Mikulec, I; Pernicka, M; Rahbaran, B; Rohringer, C; Rohringer, H; Schofbeck, R; Strauss, J; Taurok, A; Teischinger, F; Wagner, P; Waltenberger, W; Walzel, G; Widl, E; Wulz, Ce; Mossolov, V; Shumeiko, N; Gonzalez, Js; Bansal, S; Cerny, K; Cornelis, T; De Wolf, Ea; Janssen, X; Luyckx, S; Maes, T; Mucibello, L; Ochesanu, S; Roland, B; Rougny, R; Selvaggi, M; 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; Charaf, O; Clerbaux, B; De Lentdecker, G; Dero, V; Gay, Apr; Hreus, T; Leonard, A; 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[10.1103/PhysRevLett.109.022301]
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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.