2009
DOI: 10.1051/0004-6361:200811229
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Magneto-thermal evolution of neutron stars

Abstract: Context. The presence of magnetic fields in the crust of neutron stars (NSs) causes a non-spherically symmetric temperature distribution. The strong temperature dependence of the magnetic diffusivity and thermal conductivity, together with the heat generated by magnetic dissipation, couple the magnetic and thermal evolution of NSs, which can no longer be formulated as separated onedimensional problems. Aims. We study the mutual influence of thermal and magnetic evolution in a neutron star's crust in axial symm… Show more

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Cited by 273 publications
(413 citation statements)
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“…While the majority of X-ray-emitting isolated neutron stars (NSs;see, e.g., Kaspi et al 2006) exhibit thermal emission coming from the whole NS surface, no such component is required to fit our XMM-Newton spectra. Using the blackbody model, for an NS radius of 10 km and a distance of 600 pc, the 3σ upper limit on the surface temperature is 7.5×10 5 K. This low temperature fits well the behavior of old pulsars (e.g., the J0357+3205 pulsar-Morla hereafter-upper limit temperature is half this value;Marelli et al 2013): we note that the cooling mechanism is highly dependent on the magnetic field of the pulsar, so that different magnetothermal evolution paths are expected (see, e.g., Pons et al 2009). Taking into account the thermal radiation from hot spot(s), straight estimates of neutron star polar cap size based on a simple dipole magnetic field geometrygive a polar cap radius R PC =R(RΩ/c) 1 2 , where R is the neutron star radius, Ω is the angular frequency, and c is the speed of light (De Luca et al 2005).…”
Section: The Pulsarsupporting
confidence: 82%
“…While the majority of X-ray-emitting isolated neutron stars (NSs;see, e.g., Kaspi et al 2006) exhibit thermal emission coming from the whole NS surface, no such component is required to fit our XMM-Newton spectra. Using the blackbody model, for an NS radius of 10 km and a distance of 600 pc, the 3σ upper limit on the surface temperature is 7.5×10 5 K. This low temperature fits well the behavior of old pulsars (e.g., the J0357+3205 pulsar-Morla hereafter-upper limit temperature is half this value;Marelli et al 2013): we note that the cooling mechanism is highly dependent on the magnetic field of the pulsar, so that different magnetothermal evolution paths are expected (see, e.g., Pons et al 2009). Taking into account the thermal radiation from hot spot(s), straight estimates of neutron star polar cap size based on a simple dipole magnetic field geometrygive a polar cap radius R PC =R(RΩ/c) 1 2 , where R is the neutron star radius, Ω is the angular frequency, and c is the speed of light (De Luca et al 2005).…”
Section: The Pulsarsupporting
confidence: 82%
“…This transition is crucial in understanding how changes of the core magnetic field are translated to the crust. The analysis presented in this paper does, therefore, not reconcile the discrepancy between short crustal decay timescales (Pons, Miralles & Geppert 2009) and the much longer core evolution. In order to significantly reduce the latter different dissipative mechanisms have to be invoked.…”
Section: Discussioncontrasting
confidence: 65%
“…(1) it is clear that the net effect of the decay of the toroidal magnetic field, which is expected due to the combination of Ohmic and Hall effects in the neutron star interior, as it is shown in numerical simulations [see, fon instance, 23,24], is to make an initially stable prolate configuration unstable. The "more spherical" configuration has greater moment of inertia respect to the rotation axis, z in this case, and thus, in the abscense of an external torque, due to the conservation of the angular momentum, this could easily account for the sudden spin-down observed.…”
Section: The Modelmentioning
confidence: 99%