Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory

Haque N, Andersen JO, Mustafa MG, Strickland M, Su N (2014)
Physical Review D 89(6).

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We present results of a three-loop hard-thermal-loop perturbation theory calculation of the thermodynamical potential of a finite temperature and baryon chemical potential system of quarks and gluons. We compare the resulting pressure and diagonal quark susceptibilities with available lattice data. We find reasonable agreement between our analytic results and lattice data at both zero and finite chemical potential.
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Haque N, Andersen JO, Mustafa MG, Strickland M, Su N. Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory. Physical Review D. 2014;89(6).
Haque, N., Andersen, J. O., Mustafa, M. G., Strickland, M., & Su, N. (2014). Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory. Physical Review D, 89(6).
Haque, N., Andersen, J. O., Mustafa, M. G., Strickland, M., and Su, N. (2014). Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory. Physical Review D 89.
Haque, N., et al., 2014. Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory. Physical Review D, 89(6).
N. Haque, et al., “Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory”, Physical Review D, vol. 89, 2014.
Haque, N., Andersen, J.O., Mustafa, M.G., Strickland, M., Su, N.: Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory. Physical Review D. 89, (2014).
Haque, Najmul, Andersen, Jens O., Mustafa, Munshi G., Strickland, Michael, and Su, Nan. “Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory”. Physical Review D 89.6 (2014).
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