• DOI:10.1103/PhysRevD.98.088503
• Corpus ID: 73664249

Comment on “Covariant Tolman-Oppenheimer-Volkoff equations. II. The anisotropic case”

@article{Isayev2018CommentO,
  title={Comment on “Covariant Tolman-Oppenheimer-Volkoff equations. II. The anisotropic case”},
  author={A. A. Isayev},
  journal={Physical Review D},
  year={2018}
}

• A. Isayev
• Published 15 August 2018
• Physics
• Physical Review D

Recently, the covariant formulation of the Tolman-Oppenheimer-Volkoff (TOV) equations for studying the equilibrium structure of a spherically symmetric compact star in the presence of the pressure anisotropy in the interior of a star was presented in Phys. Rev. D \textbf{97} (2018) 124057. It was suggested there that the anisotropic solution of these equations can be obtained by finding, first, the solution of the common TOV equations for the isotropic pressure, and then by solving the differential equation for the anisotropic pressure whose particular form was established on the basis of the covariant TOV equations. It turns out that the anisotropic pressure determined according to this scheme has a nonremovable singularity $\Pi\sim\frac{1}{r^2}$ in the center of a star, and, hence, the corresponding anisotropic solution cannot represent a physically relevant model of an anisotropic compact star. A new scheme for constructing the anisotropic solution, based on the covariant TOV equations, is suggested, which leads to the regularly behaved physical quantities in the interior of a star. A new algorithm is applied to build model anisotropic strange quark stars with the MIT bag model equation of state.