2012MNRAS.425.2487V


Query : 2012MNRAS.425.2487V

2012MNRAS.425.2487V - Mon. Not. R. Astron. Soc., 425, 2487-2492 (2012/October-1)

Central compact objects and the hidden magnetic field scenario.

VIGANO D. and PONS J.A.

Abstract (from CDS):

Central compact objects (CCOs) are X-ray sources lying close to the centre of supernova remnants, with inferred values of the surface magnetic fields significantly lower (≲1011G) than those of standard pulsars. In this paper, we revise the hidden magnetic field scenario, presenting the first 2D simulations of the submergence and re-emergence of the magnetic field in the crust of a neutron star. A post-supernova accretion stage of about 10–4–10–3M☉ over a vast region of the surface is required to bury the magnetic field into the inner crust. When accretion stops, the field re-emerges on a typical time-scale of 1–100 kyr, depending on the submergence conditions. After this stage, the surface magnetic field is restored close to its birth values. A possible observable consequence of the hidden magnetic field is the anisotropy of the surface temperature distribution, in agreement with observations of several of these sources. We conclude that the hidden magnetic field model is viable as an alternative to the antimagnetar scenario, and it could provide the missing link between CCOs and the other classes of isolated neutron stars.

Abstract Copyright: © 2012 The Authors Monthly Notices of the Royal Astronomical Society © 2012 RAS

Journal keyword(s): stars: magnetic field - stars: neutron - pulsars: general

Simbad objects: 8

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Number of rows : 8
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Sgr J0418+5729 gam 04 18 33.867 +57 32 22.91           ~ 244 0
2 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
3 PSR J0821-4300 Psr 08 21 58.2 -43 00 22           ~ 129 2
4 NAME Pup A SNR 08 24 07 -42 59.8           ~ 636 1
5 SNR G295.5+09.7 SNR 12 09 40 -52 25.0           ~ 301 1
6 PSR J1210-5226 Psr 12 10 00.88 -52 26 28.4           ~ 230 1
7 SNR G033.6+00.1 SNR 18 52 29.000 +00 38 42.00           ~ 302 2
8 PSR J1852+0040 Psr 18 52 38.5963516169 +00 40 20.164383034           ~ 98 1

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