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Renormalization in Self-Consistent Approximations schemes at Finite Temperature I: Theory

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arxiv hep-ph/0107200 v2 pith:GNTBMXT2 submitted 2001-07-18 hep-ph cond-matnucl-th

classification hep-phcond-matnucl-th
keywords renormalizedself-consistentequationsschemestheoryconsistencyderivablefinite
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Within finite temperature field theory, we show that truncated non-perturbative self-consistent Dyson resummation schemes can be renormalized with local counter-terms defined at the vacuum level. The requirements are that the underlying theory is renormalizable and that the self-consistent scheme follows Baym''s $\Phi$-derivable concept. The scheme generates both, the renormalized self-consistent equations of motion and the closed equations for the infinite set of counter terms. At the same time the corresponding 2PI-generating functional and the thermodynamical potential can be renormalized, in consistency with the equations of motion. This guarantees the standard $\Phi$-derivable properties like thermodynamic consistency and exact conservation laws also for the renormalized approximation schemes to hold. The proof uses the techniques of BPHZ-renormalization to cope with the explicit and the hidden overlapping vacuum divergences.

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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. Consistent Thermal Resummation and Phase Transitions with 2PI Methods

    hep-ph 2026-08 conditional novelty 6.0 of 10

    A 2PI-Hartree effective potential for two mixing scalars is renormalized and used to show that self-consistent thermal resummation can substantially alter predicted phase transition strengths and gravitational wave spectra.

  2. Emergent chiral spin symmetry, non-perturbative dynamics and thermoparticles in hot QCD

    hep-ph 2025-12 unverdicted novelty 3.0 of 10

    Lattice data indicate hot QCD features an intermediate phase with emergent chiral spin symmetry and thermoparticles as thermal constituents, differing from perturbative expectations.

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