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Heavy quarkonium fragmentation functions from a heavy quark pair. I.Swave

2013/11/30 by Yan-Qing Ma, Jian-Wei Qiu, Hong Zhang · 3 citations
Mathematics · Physics and Astronomy · #Algorithm #Factorization #High-Energy Particle Collisions Research #Mathematics #Particle physics #Particle physics theoretical and experimental studies #Parton #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum mechanics #Quark #Quarkonium #Wave function #hep-ph #nucl-th

paper · pdf · doi:10.1103/physrevd.89.094029

published as Phys. Rev. D 89, 094029 (2014) · 42 pages, 4 figures, typos corrected, references added, version accepted by Journal

arxiv created 2014/05/14 · openalex publication_date 2014/05/29 · arxiv updated 2014/06/11 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/06

Abstract

A QCD factorization formalism was recently proposed for evaluating heavy quarkonium production at large pT at collider energies. With systematically calculated short-distance partonic hard parts and evolution kernels of fragmentation functions (FFs), the predictive power of this factorization approach relies on our knowledge of a large number of universal FFs at an input factorization scale \ensuremathμ0\ensuremath\gtrsim2mQ with heavy quark mass mQ. With the large heavy quark mass, the relative motion of the heavy quark pair inside a heavy quarkonium is effectively nonrelativistic. We evaluate these universal input FFs using nonrelativistic QCD (NRQCD) factorization and express the large number of FFs in terms of a few universal NRQCD long-distance matrix elements with perturbatively calculated coefficients. We derive complete contributions to the single-parton FFs at both O(\ensuremathαs) and O(\ensuremathαs2) and the heavy quark-pair FFs at O(\ensuremathαs). We present detailed derivation for all contributions involving long-distance matrix elements of S-wave NRQCD QQ states (P-wave contributions in a companion paper, Y.-Q. Ma, J.-W. Qiu, and H. Zhang, arXiv:1401.0524 [Phys. Rev. D (to be published)]). Our results bridge the gap between the QCD factorization formalism and its phenomenological applications.

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