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Quarkonium Semiclassical Transport in Quark-Gluon Plasma: Factorization and Quantum Correction

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arxiv 2009.02408 v5 pith:O4F6DG6T submitted 2020-09-04 hep-ph nucl-th

classification hep-phnucl-th
keywords quarkoniumdistributionmomentumfunctiontransportequationgluonlines
verification ladder T0 review T1 audit T2 compute T3 formal
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We study quarkonium transport in the quark-gluon plasma by using the potential nonrelativistic QCD (pNRQCD) effective field theory and the framework of open quantum systems. We argue that the coupling between quarkonium and the thermal bath is weak using separation of scales, so the initial density matrix of the total system factorizes and the time evolution of the subsystem is Markovian. We derive the semiclassical Boltzmann equation for quarkonium by applying a Wigner transform to the Lindblad equation and carrying out a semiclassical expansion. We resum relevant interactions to all orders in the coupling constant at leading power of the nonrelativistic and multipole expansions. The derivation is valid for both weakly coupled and strongly coupled quark-gluon plasmas. We find reaction rates in the transport equation factorize into a quarkonium dipole transition function and a chromoelectric gluon distribution function. For the differential reaction rate, the definition of the momentum dependent chromoelectric gluon distribution function involves staple-shaped Wilson lines. For the inclusive reaction rate, the Wilson lines collapse into a straight line along the real time axis and the distribution becomes momentum independent. The relation between the two Wilson lines is analogous to the relation between the Wilson lines appearing in the gluon parton distribution function (PDF) and the gluon transverse momentum dependent parton distribution function (TMDPDF). The centrality dependence of the quarkonium nuclear modification factor measured by experiments probes the momentum independent distribution while the transverse momentum dependence and measurements of the azimuthal angular anisotropy may be able to probe the momentum dependent one. We discuss one way to indirectly constrain the quarkonium in-medium real potential by using the factorization formula and lattice calculations. The leading quantum correction to the semiclassical transport equation of quarkonium is also worked out. The study can be easily generalized to quarkonium transport in cold nuclear matter, which is relevant for quarkonium production in eA collisions in the future Electron-Ion Collider.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. The chromoelectric adjoint correlators in Euclidean space at next-to-leading order

    hep-ph 2025-05 conditional novelty 8.0 of 10

    The chromoelectric adjoint correlators are evaluated at next-to-leading order, revealing a Wilson-line zero-mode induced asymmetry that matches lattice data at extremely high temperatures.

  2. Lattice study of correlators of chromoelectric fields for heavy quarkonium dynamics in the quark-gluon plasma

    hep-lat 2025-05 conditional novelty 7.0 of 10

    Adjoint chromoelectric correlators relevant for quarkonium dynamics are calculated in quenched lattice QCD and found to equal the fundamental correlator times Casimir factors, confirming leading-order relations nonper...

  3. Adjoint chromoelectric correlators for heavy quarkonium diffusion

    hep-lat 2025-05 conditional novelty 4.0 of 10

    First lattice measurement of adjoint chromoelectric correlators shows they scale with the fundamental heavy-quark diffusion correlator by the perturbative factors 5/4 and 9/4.

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