Dimensionally regularized Polyakov loop correlators in hot QCD
Nov, 200938 pages
Published in:
- JHEP 01 (2010) 054,
- JHEP 01 (2013) 180 (erratum)
e-Print:
- 0911.3480 [hep-ph]
Report number:
- BI-TP-2009-20
View in:
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Abstract: (arXiv)
A popular observable in finite-temperature lattice QCD is the so-called singlet quark-antiquark free energy, conventionally defined in Coulomb gauge. In an effort to interpret the existing numerical data on this observable, we compute it at order O(alpha_s^2) in continuum, and analyze the result at various distance scales. At short distances (r << 1/pi T) the behaviour matches that of the gauge-independent zero-temperature potential/ on the other hand at large distances (r >> 1/pi T) the singlet free energy appears to have a gauge-fixing related power-law tail. At infinite distance the result again becomes physical in the sense that it goes over to a gauge-independent disconnected contribution, the square of the expectation value of the trace of the Polyakov loop/ we recompute this quantity at O(alpha_s^2), finding for pure SU(Nc) a different non-logarithmic term than in previous literature, and adding for full QCD the quark contribution. We also discuss the value of the singlet free energy in a general covariant gauge, as well as the behaviour of the cyclic Wilson loop that is obtained if the singlet free energy is made gauge-independent by inserting straight spacelike Wilson lines into the observable. Comparisons with lattice data are carried out where possible.Note:
- 38 pages. v2: reference added, published version. v3: erratum added for sec.5, main results unchanged
- Thermal Field Theory
- NLO Computations
- Heavy Quark Physics
- Lattice QCD
- Polyakov loop: correlation function
- regularization: dimensional
- gauge: covariance
- free energy
- quantum chromodynamics
- Wilson loop
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