1985
DOI: 10.1086/162780
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Vortex creep and the internal temperature of neutron stars The Crab pulsar and PSR 0525 + 21

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Cited by 47 publications
(28 citation statements)
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“…A star with viscous coupling between different internal components has to dissipate energy when it is spun up or down by an external torque. Reheating of neutron stars by energy dissipation was first considered by Alpar et al (1984Alpar et al ( , 1986 in connection with the dynamical coupling between the pinned inner crust superfluid and the crust of the neutron star. The steady state thermal luminosity supplied by energy dissipation is of the form:…”
Section: Energy Dissipationmentioning
confidence: 99%
“…A star with viscous coupling between different internal components has to dissipate energy when it is spun up or down by an external torque. Reheating of neutron stars by energy dissipation was first considered by Alpar et al (1984Alpar et al ( , 1986 in connection with the dynamical coupling between the pinned inner crust superfluid and the crust of the neutron star. The steady state thermal luminosity supplied by energy dissipation is of the form:…”
Section: Energy Dissipationmentioning
confidence: 99%
“…The recovery is characterised by time-scales between 1 and 200 days, but it is incomplete in the sense that there is a persistent and cumulative increase in the spin-down rate (Lyne et al 1993). Alpar et al (1985) successfully applied the vortex creep model to the earlier Crab glitches and PSR B0525+21. They explained the persistent shift in (2.19) 5.…”
Section: /A Itgmentioning
confidence: 99%
“…Let us start by examining the salient features of a 1.4 solar mass (MO = 2 x 1033 g) "cold" neutron star with "stiff" equation of state, shown in Fig. 1 (from Pines and Alpar 1985). Going from outside to the centre, one encounters first an atmosphere a few meters thick, followed by an outer crust, a few hun dred meters in depth and of density increasing from 7 x 106 to 4 x 101 1 g/cm3.…”
mentioning
confidence: 99%
“…For the pur poses of a first order calculation, let us assume a two component thermodyna- Pines and Alpar (1985). mic model of a one solar mass neutron star: 1) an isothermal interior starting around the density   1010 g/cm3, within which almost all of the thermal energy resides; 2) an outer envelope starting with the surface and extending to the isothermal interior along which the temperature in creases from Ts of the surface to Tc of S C the interior (see Shapiro and Teukolsky 1983, Chapter 11 for a review of neutron star cooling).…”
mentioning
confidence: 99%
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