Abstract

The propagation of long-wavelength gluons through a dense QCD medium at high baryon chemical potential μB is qualitatively modified by the effects of screening, arising from scatterings off the high-momentum quarks in the medium. This same screening phenomenon also impacts gluons occurring in loop corrections to the pressure of cold quark matter, leading to contributions from the parametric scale αs1/2μB, starting at next-to-next-to-leading order (N2LO) in the strong coupling constant αs. At next-to-next-to-next-to-leading order (N3LO), interactions between these long-wavelength gluonic modes contribute to the pressure. These interaction corrections have recently been computed in Ref [1, 2], and the inclusion of these interactions slightly improves the convergence of the equation of state of cold quark matter. In these proceedings, we present these results and provide details summarizing how this lengthy calculation was performed.

Highlights

  • In recent years, the cold quark-matter (QM) equation of state (EoS)has been used as a nontrivial high-density limit [3] to constrain the EoS of neutron-star (NS) matter at much lower baryon densities nB [4,5,6]

  • This cold-QM EoS can only be used at densities nB & 40n0, with n0 ⇡ 0.16 fm−3 corresponding to nuclear saturation density, where calculations in perturbative Quantum chromodynamics [1, 2, 4, 7] show a small renormalization-scale dependence and are under perturbative control

  • In calculations at high density, one typically chooses the renormalization scale ⇤ ̄ to be proportional to the baryon chemical potential

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Summary

Introduction

The lack of a clear split between the hard and soft modes leads to an ambiguous semisoft range of energies and momenta mE ⌧ !, |k| ⌧ μB in which resummations are not necessary, but one may still use the kinematic simplifications of the HTL theory. This means that each loop integral in the diagram is divergent in the UV, leading to each of the above HTL graphs contributing terms to the pressure at orders 1/✏2, 1/✏, and

Results
Conclusion

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