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A perturbative study of the QCD phase diagram for heavy quarks at nonzero chemical potential: two-loop corrections

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arxiv 1710.01930 v1 pith:U6W6VV45 submitted 2017-10-05 hep-ph hep-lathep-th

classification hep-phhep-lathep-th
keywords potentialtwo-loopchemicalcorrectionsdiagramphaseresultsbackground
verification ladder T0 review T1 audit T2 compute T3 formal

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We extend a previous investigation of the QCD phase diagram with heavy quarks in the context of background field methods by including the two-loop corrections to the background field effective potential. The nonperturbative dynamics in the pure-gauge sector is modeled by a phenomenological gluon mass term in the Landau-DeWitt gauge-fixed action, which results in an improved perturbative expansion. We investigate the phase diagram at nonzero temperature and (real or imaginary) chemical potential. Two-loop corrections yield an improved agreement with lattice data as compared to the leading-order results. We also compare with the results of nonperturbative approaches. We further study the equation of state as well as the thermodynamic stability of the system at two-loop order. Finally, we show, using simple thermodynamic arguments, that the behavior of the Polyakov loops as functions of the chemical potential complies with their interpretation in terms of quark and anti-quark free energies.

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Cited by 2 Pith papers

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

  1. Lee Yang edge singularities of QCD in association with Roberge-Weiss phase transition and chiral phase transition

    hep-ph 2025-04 conditional novelty 6.0 of 10

    Including a confining background field in Dyson-Schwinger equations makes Lee-Yang edge singularities terminate at the Roberge-Weiss line, mu_i = pi T / 3, above T = 0.235 GeV, while leaving the critical exponent unchanged.

  2. Nonrelativistic meson masses from the Curci-Ferrari model

    hep-ph 2025-09 conditional novelty 5.0 of 10

    A potential model built from the Curci-Ferrari massive-gluon action fits charm and bottom meson spectra, and the fit prefers a nonzero gluon mass.

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