Liquid-gas coexistence vs. energy minimization with respect to the density profile in the inhomogeneous inner crust of neutron stars
arXiv:1505.07030 · doi:10.1103/PhysRevC.92.015803
Abstract
We compare two approaches to describe the inner crust of neutron stars: on the one hand, the simple coexistence of a liquid (clusters) and a gas phase, and on the other hand, the energy minimization with respect to the density profile, including Coulomb and surface effects. We find that the phase-coexistence model gives a reasonable description of the densities in the clusters and in the gas, but the precision is not high enough to obtain the correct proton fraction at low baryon densities. We also discuss the surface tension and neutron skin obtained within the energy minimization.
arXiv comment7 pages, 8 figures, to be published in Phys. Rev. C
References in corpus (17)
- Physics of Neutron Star Crusts
- Inner crust of neutron stars with mass-fitted Skyrme functionals
- Nuclear pasta structures and the charge screening effect
- Structure of cold nuclear matter at subnuclear densities by Quantum Molecular Dynamics
- Warm pasta phase in the Thomas-Fermi approximation
- Low-energy collective excitations in the neutron star inner crust
- Light clusters, pasta phases and phase transitions in core-collapse supernova matter
- Symmetry energy: nuclear masses and neutron stars
- Collective excitations in the inner crust of neutron stars : supergiant resonances
- In-medium nuclear cluster energies within the Extended Thomas-Fermi approach
- A low energy theory for superfluid and solid matter and its application to the neutron star crust
- From the crust to the core of Neutron Stars on a microscopic basis
- Phase transitions in Core-Collapse Supernova Matter at sub-saturation densities
- Proton fraction in the inner neutron-star crust
- Collective excitations in the neutron star inner crust
- Ising analogue to compact-star matter
- In-medium ion mass renormalization and lattice vibrations in the neutron star crust
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- Equations of state for supernovae and compact stars
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- Unified equations of state for cold non-accreting neutron stars with Brussels-Montreal functionals. II. Pasta phases in semi-classical approximation
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- Uncertainties in the pasta-phase properties of catalysed neutron stars
- Crystallization of the inner crust of a neutron star and the influence of shell effects
- Impact of the neutron-star deformability on equation of state parameters
- Structure and composition of inner crust of neutron stars from Gogny interactions
- The effect of the energy functional on the pasta-phase properties of catalysed neutron stars
- Crustal properties of a neutron star within an effective relativistic mean-field model
- Unified equations of state for cold non-accreting neutron stars with Brussels-Montreal functionals. IV. Role of the symmetry energy in pasta phases
- Systematic analysis of inner crust composition using the extended Thomas-Fermi approximation with pairing correlations
- Long-wavelength phonons in the crystalline and pasta phases of neutron-star crusts
- Unified equations of state for cold nonaccreting neutron stars with Brussels-Montreal functionals. V. Improved parametrization of the nucleon density distributions
- Equation of state of superfluid neutron matter with low-momentum interactions
- Superfluid fraction in the slab phase of the inner crust of neutron stars
- Superfluid fraction in the rod phase of the inner crust of neutron stars
- Inner crust of neutron stars with mass-fitted Skyrme interaction
- How accurately can the Extended Thomas-Fermi method describe the inner crust of a neutron star?
- Effect of the equation of state for dilute neutron matter on the composition of the inner crust of neutron stars
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