2016
DOI: 10.1093/mnras/stw751
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Diffusive heat blanketing envelopes of neutron stars

Abstract: We construct new models of outer heat blanketing envelopes of neutron stars composed of binary ion mixtures (H -He, He -C, C -Fe) in and out of diffusive equilibrium. To this aim, we generalize our previous work on diffusion of ions in isothermal gaseous or Coulomb liquid plasmas to handle non-isothermal systems. We calculate the relations between the effective surface temperature T s and the temperature T b at the bottom of heat blanketing envelopes (at a density ρ b ∼ 10 8 − 10 10 g cm −3 ) for diffusively e… Show more

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Cited by 36 publications
(63 citation statements)
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References 185 publications
(479 reference statements)
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“…The curves are calculated using the approximate analytic expressions [13] for a 1.4 M star. The stars of age t 10-100 yr are thought to be thermally relaxed inside with a noticeable temperature gradient remaining only in a thin surface layer called the heat blanketing envelope (e.g., [14][15][16]). The stars with t 10 5 yr (including the Vela pulsar) are believed to be cooling predominantly via the neutrino emission from their superdense cores.…”
Section: Introductionmentioning
confidence: 99%
“…The curves are calculated using the approximate analytic expressions [13] for a 1.4 M star. The stars of age t 10-100 yr are thought to be thermally relaxed inside with a noticeable temperature gradient remaining only in a thin surface layer called the heat blanketing envelope (e.g., [14][15][16]). The stars with t 10 5 yr (including the Vela pulsar) are believed to be cooling predominantly via the neutrino emission from their superdense cores.…”
Section: Introductionmentioning
confidence: 99%
“…An interesting effect, first noticed by Beznogov et al (2016), is that the replacement of H by 4 He increases the photon luminosity. This effect is caused by the different mass to charge ratio of H, which results in the discontinuity of ρ and is related to the lower opacities of He at high T and fixed ρ, revealed in both op and opal tables.…”
Section: Accreted Envelopesmentioning
confidence: 93%
“…All the fits are obtained for an envelope with surface gravity g s,0 = 2.4271 × 10 14 cm s −2 but can be scaled for any g s using Y = (T s /1MK)(g s,0 /g s ) 1/4 (Gudmundsson et al 1983). We use an adapted version of the analytic functions (Equation A1) presented by Beznogov et al (2016).…”
Section: Appendix A: Analytic T S -T B Relationsmentioning
confidence: 99%