Heat capacity of low density neutron matter: from quantum to classical regimes
arXiv:1501.03364 · doi:10.1093/mnras/stv095
Abstract
The heat capacity of neutron matter is studied over the range of densities and temperatures prevailing in neutron-star crusts, allowing for the transition to a superfluid phase at temperatures below some critical temperature and including the transition to the classical limit. Finite temperature Hartree-Fock-Bogoliubov equations (FTHFB) are solved and compared to existing approximate expressions. In particular, the formula given by Levenfish and Yakovlev is found to reproduce the numerical results with a high degree of accuracy for temperatures . In the non-superfluid phase, , the linear approximation is valid only at temperature ( being the Fermi temperature of the neutron gas) which is rarely the case in the shallow layers of the neutron star's crust. A non-perturbative interpolation between the quantal and the classical regimes is proposed here. The heat capacity, conveniently parametrized solely in terms of , , and the neutron number density , can be easily implemented in neutron-star cooling simulations.
Accepted by Monthly Notices of the Royal Astronomical Society
References in corpus (7)
- Inner crust of neutron stars with mass-fitted Skyrme functionals
- Screening Effects in Superfluid Nuclear and Neutron Matter within Brueckner Theory
- BCS-BEC crossover of neutron pairs in symmetric and asymmetric nuclear matter
- Effective contact pairing forces from realistic calculations in infinite homogeneous nuclear matter
- Unified description of neutron superfluidity in the neutron-star crust with analogy to anisotropic multi-band BCS superconductors
- Nuclear Superfluidity and Cooling Time of Neutron-Star Crust
- Neutron specific heat in the crust of neutron stars from the nuclear band theory