Quark and hybrid stars with renormalization group improvement of NNLO perturbative QCD

arXiv:2606.29576 · nucl-th, astro-ph.HE, hep-ph, hep-th · Submitted 2026-06-28 · Read on arXiv

nucl-th, astro-ph.HE, hep-ph, hep-th

Submitted: 2026-06-28

Updated: 2026-10-07

Comments: 21 pages, 9 figures, 4 tables

License: http://creativecommons.org/licenses/by/4.0/

The gist: Recently, the NNLO perturbative QCD pressure of cold and dense symmetric matter, with arbitrary quark masses, has been resummed within the renormalization-group-optimized perturbation theory (RGOPT)

Terminology

Abstract

Recently, the NNLO perturbative QCD pressure of cold and dense symmetric matter, with arbitrary quark masses, has been resummed within the renormalization-group-optimized perturbation theory (RGOPT) framework. By being imbued with renormalization group properties, the resulting pressure is less sensitive to renormalization scale (X mu B/3) variations than the NNLO perturbative QCD pressure. Here, we extend this by considering beta-equilibrium and charge neutrality to evaluate the corresponding equation of state (EoS). We provide a compact ``pocket" fitting formula for the EoS for N f=2+1 massive quarks at different renormalization scale parameter (X) values. We describe pure quark stars as well as hybrid stars with quark-cores. Pure quark stars compatible with astrophysical observations were obtained with X=3.08-3.58, whereas a larger value (4.10) is needed if the low mass object of the observation GW190814 represents a neutron star. Hybrid stars were built considering three representative hadron models based on a relativistic mean-field description, and chosen to produce soft and stiff EoSs. Stable hybrid stars with masses compatible with the massive pulsar PSR J0740+6620 were obtained considering X of the order of 2 to 2.60-2.98, the largest scale giving rise to hybrid stars with a large quark core with a radius of 5 to 8 km, and the smallest to a small quark core at the center of the star.

Sources

Related papers