QCD Equation of State at nonzero baryon density in external magnetic field
arXiv:2403.07783 · doi:10.1103/PhysRevD.109.094511
Abstract
This paper is devoted to the study of QCD equation of state in external magnetic field and nonzero baryon density. Our study is carried out by means of lattice simulation with 2+1 dynamical staggered quarks at the physical masses. The simulation is conducted at imaginary baryon chemical potential what allowed us to overcome the sign problem. We expand the pressure in the baryon imaginary chemical potential and study three leading nonzero coefficients in this expansion. These coefficients were calculated for the following values of magnetic field: , , GeV with the lattice sizes , , . Using these data we take continuum limit for the coefficients. Our results indicate considerable enhancement of the expansion coefficients by the magnetic field.
8 pages, 4 figures, 3 tables; references updated; version accepted for publication in PRD
References in corpus (16)
- The Chiral Magnetic Effect
- The equation of state in (2+1)-flavor QCD
- The QCD equation of state with dynamical quarks
- The QCD transition temperature: results with physical masses in the continuum limit II.
- Equation of state and QCD transition at finite temperature
- The QCD Equation of State to from Lattice QCD
- QCD Phase Transition in a Strong Magnetic Background
- The QCD equation of state in background magnetic fields
- Chiral Properties of Strong Interactions in a Magnetic Background
- QCD equation of state with 2+1 flavors of improved staggered quarks
- Chiral properties of (2+1)-flavor QCD in strong magnetic fields at zero temperature
- Phase diagram of QCD in a magnetic background
- Fluctuations and correlations of net baryon number, electric charge and strangeness in a background magnetic field
- Chiral phase structure of three flavor QCD in a background magnetic field
- Hot perturbative QCD in a very strong magnetic background
- Cold and dense perturbative QCD in a very strong magnetic background