Abstract

We explore the in-medium properties of heavy-quarkonium states at finite baryo-chemical potential and finite transverse momentum based on a modern complex-valued potential model. Our starting point is a novel, rigorous derivation of the generalized Gauss law for in-medium quarkonium, combining the non-perturbative physics of the vacuum bound state with a weak coupling description of the medium degrees of freedom. Its relation to previous models in the literature is discussed. We show that our approach is able to reproduce the complex lattice QCD heavy quark potential even in the non-perturbative regime, using a single temperature dependent parameter, the Debye mass $m_D$. After vetting the Gauss-law potential with state-of-the-art lattice QCD data, we extend it to the regime of finite baryon density and finite velocity, currently inaccessible to first principles simulations. In-medium spectral functions computed from the Gauss-law potential are subsequently used to estimate the $\psi'/J/\psi$ ratio in heavy-ion collisions at different beam energies and transverse momenta. We find qualitative agreement with the predictions from the statistical model of hadronization for the $\sqrt{s_{NN}}$ dependence and a mild dependence on the transverse momentum.

Highlights

  • Heavy quarkonium, the bound states of a charm or bottom quark, and its antiquark have matured into a high precision tool for the study of strongly interacting matter under extreme conditions in the context of relativistic heavy-ion collisions [1,2]

  • From a theory standpoint the heavy mass of the constituent quarks opens the door to the powerful effective field theory (EFT) framework [6] that allow us to simplify the description of theirequilibrium behavior

  • We find that our ansatz, as expected, reproduces the well-known hard-thermal loop (HTL) result [17,37] given in Eq (2), ReVCðrÞ

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Summary

INTRODUCTION

The bound states of a charm or bottom quark, and its antiquark (ccor bb ) have matured into a high precision tool for the study of strongly interacting matter under extreme conditions in the context of relativistic heavy-ion collisions [1,2]. From a theory standpoint the heavy mass of the constituent quarks opens the door to the powerful effective field theory (EFT) framework [6] that allow us to simplify the description of their (non)equilibrium behavior These techniques have led to progress both in direct lattice QCD studies of equilibrated quarkonium and in formulating realtime descriptions of their nonequilibrium evolution. This information is only accessible in potential based computations, where a Schrödinger equation for the spectral functions is solved in the presence of a nonperturbatively defined in-medium potential Important progress in this regard has been made using an EFT based definition of the in-medium potential between two static quarks based on the real-time evolution of the QCD Wilson loop, VðrÞ. Landau damping dominates and the potential reads

HTL ðrÞ
THE GAUSS LAW POTENTIAL MODEL
Constructing the in-medium model
Consistent treatment of string breaking
Comparison to other models
Vetting with lattice QCD data
Extension to a running coupling
Extension to finite velocity
Continuum corrections
In-medium spectral functions
APPLICATIONS TO HEAVY-ION COLLISIONS
Finite μB phenomenology
Finite transverse momentum
Findings
CONCLUSION
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