# Proper heavy-quark potential from a spectral decomposition of the   thermal Wilson loop

**Authors:** A. Rothkopf, T. Hatsuda, S. Sasaki

arXiv: 0910.2321 · 2010-11-05

## TL;DR

This paper introduces a non-perturbative, gauge-invariant method to derive the heavy-quark potential at finite temperature using spectral functions of the thermal Wilson loop, validated through lattice QCD simulations.

## Contribution

It presents a novel spectral decomposition approach to define the heavy-quark potential, including its real and imaginary parts, at finite temperature in a gauge-invariant manner.

## Key findings

- Real part shows Coulombic and confining behavior below T_c.
- At high temperature, potential matches Debye screening from Polyakov-line correlations.
- Spectral structure analyzed using maximum entropy method (MEM).

## Abstract

We propose a non-perturbative and gauge invariant derivation of the static potential between a heavy-quark ($Q$) and an anti-quark ($\bar{Q}$) at finite temperature. This proper potential is defined through the spectral function (SPF) of the thermal Wilson loop and can be shown to satisfy the Schr\"{o}dinger equation for the heavy $Q\bar{Q}$ pair in the thermal medium. In general, the proper potential has a real and an imaginary part,corresponding to the peak position and width of the SPF. The validity of using a Schr\"{o}dinger equation for heavy $Q\bar{Q}$ can also be checked from the structure of the SPF. To test this idea, quenched QCD simulations on anisotropic lattices ($a_\sigma=4a_\tau=0.039\rm fm$, $N^3_\sigma \times N_{\tau} =20^2 \times (96-32)$) are performed. The real part of the proper potential below the deconfinement temperature ($T=0.78T_c$) exhibits the well known Coulombic and confining behavior. At ($T=2.33T_c$) we find that it coincides with the Debye screened potential obtained from Polyakov-line correlations in the color-singlet channel under Coulomb gauge fixing. The physical meaning of the spectral structure of the thermal Wilson loop and the use of the maximum entropy method (MEM) to extract the real and imaginary part of the proper potential are also discussed.

## Full text

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## Figures

11 figures with captions in the complete paper: https://tomesphere.com/paper/0910.2321/full.md

## References

12 references — full list in the complete paper: https://tomesphere.com/paper/0910.2321/full.md

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Source: https://tomesphere.com/paper/0910.2321