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The QCD equation of state in background magnetic fields (1406.0269v2)

Published 2 Jun 2014 in hep-lat, hep-ph, hep-th, and nucl-th

Abstract: We determine the equation of state of 2+1-flavor QCD with physical quark masses, in the presence of a constant (electro)magnetic background field on the lattice. To determine the free energy at nonzero magnetic fields we develop a new method, which is based on an integral over the quark masses up to asymptotically large values where the effect of the magnetic field can be neglected. The method is compared to other approaches in the literature and found to be advantageous for the determination of the equation of state up to large magnetic fields. Thermodynamic observables including the longitudinal and transverse pressure, magnetization, energy density, entropy density and interaction measure are presented for a wide range of temperatures and magnetic fields, and provided in ancillary files. The behavior of these observables confirms our previous result that the transition temperature is reduced by the magnetic field. We calculate the magnetic susceptibility and permeability, verifying that the thermal QCD medium is paramagnetic around and above the transition temperature, while we also find evidence for weak diamagnetism at low temperatures.

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Summary

The QCD Equation of State in Background Magnetic Fields

This paper presents a paper of the equation of state (EoS) for Quantum Chromodynamics (QCD) with 2+1 flavors in the presence of background magnetic fields. The research is conducted using lattice QCD simulations, leveraging a newly developed method to compute thermodynamic quantities over a range of temperatures and magnetic fields.

Overview and Methodology

The primary aim is to determine the EoS for QCD matter near the crossover transition temperature under varying magnetic fields. This involves calculating key thermodynamic observables such as pressure, energy density, entropy density, magnetization, and the interaction measure. The paper introduces a novel approach, termed the generalized integral method, which circumvents the challenges posed by magnetic flux quantization in lattice simulations.

The generalized integral method allows derivation of the magnetic field's influence on thermodynamic properties by integrating condensate differences over quark masses, from their physical values up to asymptotically large values. This approach offers computational advantages, particularly for larger magnetic fields, where direct computation would be infeasible.

Numerical Results

Several noteworthy numerical findings are presented:

  • Transition Temperature: There is a reduction in the QCD transition temperature as the magnetic field increases, corroborating previous results that the crossover transition line shifts to lower temperatures with stronger fields.
  • Paramagnetic Behavior: The QCD medium exhibits paramagnetic characteristics around and above the transition temperature. This behavior is verified by calculations of magnetic susceptibility and permeability, with a weak diamagnetic tendency observed at lower temperatures due to pion contributions.
  • Pressure Anisotropy: The external magnetic field induces anisotropy in the pressure, with longitudinal and transverse components diverging. This anisotropy is crucial for accurately modeling scenarios like heavy-ion collisions where such anisotropic pressures can be observed.

Implications and Significance

The results have direct implications for systems under strong interactions and external fields, such as the quark-gluon plasma in heavy-ion collisions and strongly magnetized neutron stars. Understanding the EoS shifts with magnetic fields informs the evaluation of the QGP's evolution and offers insights into the early universe where such magnetic fields were prevalent.

Moreover, the paramagnetic and diamagnetic transitions impact the modeling of transport properties in these systems, with potential applications in cosmology and astrophysics.

Future Directions

Future research could extend these findings by:

  • Incorporating more refined lattice simulations to explore higher magnetic field limits and temperature ranges.
  • Developing more comprehensive models integrating lattice QCD data with perturbative techniques for broader applicability.
  • Examining the effects of finite quark densities in conjunction with magnetic fields to better simulate real-world conditions like neutron stars.

Overall, this paper significantly enhances our understanding of QCD under magnetic fields, providing a robust framework to accurately model the EoS and its thermodynamic characteristics in such conditions.

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