Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density

Haque N, Andersen JO, Mustafa MG, Strickland M, Su N (2014)
Phys. Rev. D 89.

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We present results of a three-loop hard-thermal-loop perturbation theorycalculation of the thermodynamical potential of a finite temperature and baryonchemical potential system of quarks and gluons. We compare the resultingpressure and diagonal quark susceptibilities with available lattice data. Wefind reasonable agreement between our analytic results and lattice data at bothzero and finite chemical potential.
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Haque N, Andersen JO, Mustafa MG, Strickland M, Su N. Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density. Phys. Rev. D. 2014;89.
Haque, N., Andersen, J. O., Mustafa, M. G., Strickland, M., & Su, N. (2014). Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density. Phys. Rev. D, 89.
Haque, N., Andersen, J. O., Mustafa, M. G., Strickland, M., and Su, N. (2014). Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density. Phys. Rev. D 89.
Haque, N., et al., 2014. Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density. Phys. Rev. D, 89.
N. Haque, et al., “Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density”, Phys. Rev. D, vol. 89, 2014.
Haque, N., Andersen, J.O., Mustafa, M.G., Strickland, M., Su, N.: Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density. Phys. Rev. D. 89, (2014).
Haque, Najmul, Andersen, Jens O., Mustafa, Munshi G., Strickland, Michael, and Su, Nan. “Three-loop HTLpt Pressure and Susceptibilities at Finite Temperature and Density”. Phys. Rev. D 89 (2014).
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