Measurement of quarkonium production at forward rapidity in Formula: see text collisions at Formula: see textTeV

The inclusive production cross sections at forward rapidity of [Formula: see text], [Formula: see text], [Formula: see text](1S) and [Formula: see text](2S) are measured in [Formula: see text] collisions at [Formula: see text] with the ALICE detector at the LHC. The analysis is based on a data sampl...

Full description

Saved in:
Bibliographic Details
Published inThe European physical journal. C, Particles and fields Vol. 74; no. 8; p. 2974
Main Authors Aggarwal, M M, Ahammed, Z, Alexandre, D, Alici, A, Aronsson, T, Bach, M, Badalà, A, Barbera, R, Baumann, C, Berenyi, D, Bhat, I R, Blau, D, Bock, F, Buesching, H, Cai, X, Carena, W, Castillo Castellanos, J, Ceballos Sanchez, C, Chapeland, S, Cunqueiro, L, D'Erasmo, G, De Gruttola, D, Dordic, O, Evans, D, Ferreiro, E G, Festanti, A, Foka, P, Ghosh, S K, Guber, F, Gulkanyan, H, Gupta, A, Hess, B A, Hristov, P, Kharlov, Y, Kim, S, Knichel, M L, Kondratiev, V, Kovalenko, V, Koyithatta Meethaleveedu, G, Kramer, F, Krus, M, Legrand, I, Lindal, S, Loginov, V, Luzzi, C, Ma, R, Maire, A, Manceau, L, Margagliotti, G V, Martinengo, P, Miake, Y, Milosevic, J, Moreira De Godoy, D A, Moretto, S, Mudnic, E, Muhuri, S, Nappi, E, Nikulin, S, Oeschler, H, Oleniacz, J, Onderwaater, J, Paić, G, Pant, D, Parmar, S, Petran, M, Pospisil, V, Prasad, S K, Preghenella, R, Putschke, J, Razazi, V, Riggi, F, Ryabinkin, E, Šafařík, K, Segato, G, Seo, J, Serradilla, E, Shabetai, A, Shangaraev, A, Skjerdal, K, Soltz, R, Song, M, Sorensen, S, Steinpreis, M, Stenlund, E, Steyn, G, Susa, T, Telesca, A, Timmins, A R, Tsuji, T, Usai, G L, Van Hoorne, J W, Vechernin, V, Vernet, R, Virgili, T, Viyogi, Y P, Vranic, D, Vulpescu, B, Watanabe, D, Winn, M, Zhigareva, N
Format Journal Article
LanguageEnglish
Published 01.01.2014
Online AccessGet full text

Cover

Loading…
More Information
Summary:The inclusive production cross sections at forward rapidity of [Formula: see text], [Formula: see text], [Formula: see text](1S) and [Formula: see text](2S) are measured in [Formula: see text] collisions at [Formula: see text] with the ALICE detector at the LHC. The analysis is based on a data sample corresponding to an integrated luminosity of 1.35 pb[Formula: see text]. Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the [Formula: see text] invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum [Formula: see text] and rapidity [Formula: see text], over the ranges [Formula: see text] GeV/c for [Formula: see text], [Formula: see text] GeV/c for all other resonances and for [Formula: see text]. The measured cross sections integrated over [Formula: see text] and [Formula: see text], and assuming unpolarized quarkonia, are: [Formula: see text] [Formula: see text]b, [Formula: see text] [Formula: see text]b, [Formula: see text] nb and [Formula: see text] nb, where the first uncertainty is statistical and the second one is systematic. The results are compared to measurements performed by other LHC experiments and to theoretical models.The inclusive production cross sections at forward rapidity of [Formula: see text], [Formula: see text], [Formula: see text](1S) and [Formula: see text](2S) are measured in [Formula: see text] collisions at [Formula: see text] with the ALICE detector at the LHC. The analysis is based on a data sample corresponding to an integrated luminosity of 1.35 pb[Formula: see text]. Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the [Formula: see text] invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum [Formula: see text] and rapidity [Formula: see text], over the ranges [Formula: see text] GeV/c for [Formula: see text], [Formula: see text] GeV/c for all other resonances and for [Formula: see text]. The measured cross sections integrated over [Formula: see text] and [Formula: see text], and assuming unpolarized quarkonia, are: [Formula: see text] [Formula: see text]b, [Formula: see text] [Formula: see text]b, [Formula: see text] nb and [Formula: see text] nb, where the first uncertainty is statistical and the second one is systematic. The results are compared to measurements performed by other LHC experiments and to theoretical models.
Bibliography:ObjectType-Article-1
SourceType-Scholarly Journals-1
content type line 23
ObjectType-Feature-2
ISSN:1434-6044
DOI:10.1140/epjc/s10052-014-2974-4