J/{psi} polarization in photoproduction up to the next-to-leading order of QCD

We investigate the J/{psi} polarization in photoproduction at the Hadron Electron Ring Accelerator (HERA) up to the next-to-leading order of QCD. The results show that the transverse momentum p{sub t} and energy fraction z distributions of J/{psi} production do not agree with the observed ones very...

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Veröffentlicht in:Physical review. D, Particles and fields Particles and fields, 2009-08, Vol.80 (3)
Hauptverfasser: Chang Chaohsi, Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing, 100080, Theoretical Physics Center for Science Facilities, Chinese Academy of Sciences, Beijing, 100049, Li Rong, Wang Jianxiong
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container_title Physical review. D, Particles and fields
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creator Chang Chaohsi
Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing, 100080
Theoretical Physics Center for Science Facilities, Chinese Academy of Sciences, Beijing, 100049
Li Rong
Wang Jianxiong
description We investigate the J/{psi} polarization in photoproduction at the Hadron Electron Ring Accelerator (HERA) up to the next-to-leading order of QCD. The results show that the transverse momentum p{sub t} and energy fraction z distributions of J/{psi} production do not agree with the observed ones very well. The theoretical uncertainties for the z distributions of the J/{psi} polarization parameters with respect to various choices of the renormalization and factorization scales are too large to give a definite predication. The uncertainties for the p{sub t} distributions of these parameters are small when p{sub t}>3 GeV and the obtained p{sub t} distributions cannot describe the experimental data even in this region.
doi_str_mv 10.1103/PHYSREVD.80.034020
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subjects ELECTRON-RING ACCELERATORS
FACTORIZATION
GEV RANGE 01-10
HERA STORAGE RING
J PSI-3097 MESONS
PHOTOPRODUCTION
PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
POLARIZATION
QUANTUM CHROMODYNAMICS
RENORMALIZATION
TRANSVERSE MOMENTUM
title J/{psi} polarization in photoproduction up to the next-to-leading order of QCD
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