2019
DOI: 10.1103/physrevc.99.055805
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Role of Landau-Rabi quantization of electron motion on the crust of magnetars within the nuclear energy density functional theory

Abstract: Magnetic fields of order 10 15 G have been measured at the surface of some neutron stars, and much stronger magnetic fields are expected to be present in the solid region beneath the surface.The effects of the magnetic field on the equation of state and on the composition of the crust due to Landau-Rabi quantization of electron motion are studied. Both the outer and inner crustal regions are described in a unified and consistent way within the nuclear-energy density functional theory.

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Cited by 23 publications
(46 citation statements)
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“…Making use of the completeness relations, i ϕ (q) i (r, σ ) * ϕ (q) i (r , σ ) = δ(r − r )δ σ σ , (A1) and using Eqs. (24) and (25), we can demonstrate the following identities:…”
Section: Appendix: Continuity Equationsmentioning
confidence: 88%
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“…Making use of the completeness relations, i ϕ (q) i (r, σ ) * ϕ (q) i (r , σ ) = δ(r − r )δ σ σ , (A1) and using Eqs. (24) and (25), we can demonstrate the following identities:…”
Section: Appendix: Continuity Equationsmentioning
confidence: 88%
“…Our formulas are applicable to a large class of nuclear energy-density functionals. These include the Brussels-Montreal functionals based on generalized Skyrme effective interactions for which unified equations of state for all regions of neutron stars have been calculated [21,[23][24][25], thus, paving the way for a fully consistent microscopic treatment of the dynamics of superfluid neutron stars. The formalism we have developed here in the nuclear context may also be easily transposed to the less exotic kinds of superfluids studied in terrestrial laboratories and described by similar TDHFB equations.…”
Section: Discussionmentioning
confidence: 99%
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“…where γ e is the electron Fermi energy in units of the electron mass energy m e c 2 , and ρ 6 = ρ/10 6 g cm −3 . We estimated this temperature in the different layers of the outer crust of a magnetar using the composition calculated in [21] for B = 2000 (B ≈ 8.83 × 10 16 G) and B = 3000 (B ≈ 1.32 × 10 17 G). As we show, electron captures occur at pressures well above 10 28 dyn cm −2 (densities above 10 10 g cm −3 ).…”
Section: Thermodynamic Conditionsmentioning
confidence: 99%
“…[15] by minimizing the Gibbs free energy per nucleon g at zero temperature and for a finite set of pressure values (see, e.g., Refs. [16][17][18][19]). The pressure step must be small enough to find the complete stratification, especially in the deepest region of the outer crust where even a thin layer can contain the most abundant nuclear species.…”
Section: Introductionmentioning
confidence: 99%