Relativistic Thomas-Fermi treatment of compressed atoms and compressed nuclear matter cores of stellar dimensions

Citations Over TimeTop 10% of 2011 papers

Abstract

The Feynman-Metropolis-Teller treatment of compressed atoms is extended to the relativistic regimes. Each atomic configuration is confined by a Wigner-Seitz cell and is characterized by a positive electron Fermi energy. The nonrelativistic treatment assumes a pointlike nucleus and infinite values of the electron Fermi energy can be attained. In the relativistic treatment there exists a limiting configuration, reached when the Wigner-Seitz cell radius equals the radius of the nucleus, with a maximum value of the electron Fermi energy $({E}_{e}^{F}){}_{\mathrm{max}}$, here expressed analytically in the ultrarelativistic approximation. The corrections given by the relativistic Thomas-Fermi-Dirac exchange term are also evaluated and shown to be generally small and negligible in the relativistic high-density regime. The dependence of the relativistic electron Fermi energies by compression for selected nuclei are compared and contrasted to the nonrelativistic ones and to the ones obtained in the uniform approximation. The relativistic Feynman-Metropolis-Teller approach here presented overcomes some difficulties in the Salpeter approximation generally adopted for compressed matter in physics and astrophysics. The treatment is then extrapolated to compressed nuclear matter cores of stellar dimensions with $A\ensuremath{\simeq}({m}_{\mathrm{Planck}}/{m}_{n}){}^{3}~{10}^{57}$ or ${M}_{\mathrm{core}}~{M}_{\ensuremath{\bigodot}}$. A new family of equilibrium configurations exists for selected values of the electron Fermi energy varying in the range $0<{E}_{e}^{F}\ensuremath{\leqslant}({E}_{e}^{F}){}_{\mathrm{max}}$. Such configurations fulfill global but not local charge neutrality. They have electric fields on the core surface, increasing for decreasing values of the electron Fermi energy reaching values much larger than the critical value ${E}_{c}={m}_{e}^{2}{c}^{3}/(e\ensuremath{\hbar})$ for ${E}_{e}^{F}=0$. We compare and contrast our results with the ones of Thomas-Fermi model in strange stars.

Related Papers

• → Kinetic energy functional for a two-dimensional electron system(2007)16 cited
• → Energy fluctuations of a finite free-electron Fermi gas(2016)6 cited
• THE RELATION BETWEEN THE MACROPROPERTIES OF ELECTRON GAS AND ITS DIMENSIONALITY(1986)
• On the relation between Fermi energy of low-dimensional electron gas and temperature(2001)