Prompt charmonia production and polarization at the LHC in the NRQCD with kT-factorization. III. J/Ψ meson

被引:22
作者
Baranov, S. P. [1 ]
Lipatov, A. V. [2 ,3 ]
机构
[1] PN Lebedev Phys Inst, Moscow 119991, Russia
[2] Lomonosov Moscow State Univ, Skobeltsyn Inst Nucl Phys, Moscow 119991, Russia
[3] Joint Inst Nucl Res, Dubna 141980, Moscow Region, Russia
关键词
SMALL-X PHENOMENOLOGY; HEAVY-QUARK PRODUCTION; INELASTIC PHOTOPRODUCTION; QCD COHERENCE; J-PSI; FRAGMENTATION; DISTRIBUTIONS; UPSILON;
D O I
10.1103/PhysRevD.96.034019
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
In the framework of the k(T)-factorization approach, the production and polarization of prompt J/Psi mesons at the LHC energies is studied. Our consideration is based on the nonrelativistic QCD formalism for bound states and off-shell amplitudes for hard partonic subprocesses. Both the direct production mechanism and feed-down contributions from chi(c) and Psi(2S) decays are taken into account. The transverse momentum dependent (or unintegrated) gluon densities in a proton were derived from Ciafaloni-Catani-Fiorani-Marchesini evolution equation or, alternatively, were chosen in accordance with Kimber-Martin-Ryskin prescription. The nonperturbative color-octet matrix elements were first deduced from the fits to the latest CMS data on J/Psi transverse momentum distributions and then applied to describe the ATLAS and LHCb data on J/Psi production and polarization at root s = 7, 8 and 13 TeV. We perform an estimation of polarization parameters lambda(theta), lambda(phi), and lambda(theta phi) which determine J/Psi spin density matrix and demonstrate that treating the soft gluon emission as a series of explicit color-electric dipole transitions within NRQCD leads to unpolarized J/Psi production at high transverse momenta, that is in qualitative agreement with the LHC data.
引用
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页数:13
相关论文
共 58 条
[1]  
A Kuraev E., 1977, Sov. Phys. JETP, V45, P199
[2]  
A Kuraev E., 1976, Sov. Phys. JETP, V44, P443
[3]  
Aad G, 2014, J HIGH ENERGY PHYS, P1, DOI 10.1007/JHEP05(2014)071
[4]  
Aaij R, 2015, J HIGH ENERGY PHYS, DOI 10.1007/JHEP10(2015)172
[5]  
Aaij R, 2014, EUR PHYS J C, V74, DOI 10.1140/epjc/s10052-014-2872-9
[6]  
Aaij R, 2013, EUR PHYS J C, V73, DOI 10.1140/epjc/s10052-013-2631-3
[7]  
Aaij R., 2016, JHEP, V10, DOI 10.1007/JHEP10(2016)030
[8]   Small-x phenomenology -: Summary of the 3rd Lund small-x workshop in 2004 [J].
Andersen, J. R. ;
Baranov, S. ;
Bartels, J. ;
Barnafoldi, G. G. ;
Chachamis, G. ;
Collins, J. ;
Grindhammer, G. ;
Gustafson, G. ;
Hansson, M. ;
Ingelman, G. ;
Jung, H. ;
Jonsson, L. ;
Knutsson, A. ;
Kowalski, H. ;
Kutak, K. ;
Kyrieleis, A. ;
Levai, P. ;
Lipatov, A. ;
Lonnblad, L. ;
Lublinsky, M. ;
Marchesini, G. ;
Milcewicz, I. ;
Risler, C. ;
Sabio-Vera, A. ;
Sjodahl, M. ;
Stasto, A. ;
Turnau, J. ;
Watt, G. ;
Zotov, N. .
EUROPEAN PHYSICAL JOURNAL C, 2006, 48 (01) :53-105
[9]   Small-x phenomenology -: summary and status 2002 [J].
Andersen, JR ;
Baranov, S ;
Collins, J ;
Dokshitzer, Y ;
Goerlich, L ;
Grindhammer, G ;
Gustafson, G ;
Jönsson, L ;
Jung, H ;
Kwiecinski, J ;
Levin, E ;
Lipatov, A ;
Lonnblad, L ;
Lublinsky, M ;
Maul, M ;
Milcewicz, I ;
Miu, G ;
Nowak, G ;
Sjöstrand, T ;
Stasto, A ;
Tîmneanu, N ;
Turnau, J ;
Zotov, N .
EUROPEAN PHYSICAL JOURNAL C, 2004, 35 (01) :67-98
[10]   Small x phenomenology:: summary and status [J].
Andersson, B ;
Baranov, S ;
Bartels, J ;
Ciafaloni, M ;
Collins, J ;
Davidsson, M ;
Gustafson, G ;
Jung, H ;
Jönsson, L ;
Karlsson, M ;
Kimber, M ;
Kotikov, A ;
Kwiecnski, J ;
Lönnblad, L ;
Miu, G ;
Salam, G ;
Seymour, MH ;
Sjöstrand, T ;
Zotov, N .
EUROPEAN PHYSICAL JOURNAL C, 2002, 25 (01) :77-101