2021NatAs...5..145I


Query : 2021NatAs...5..145I

2021NatAs...5..145I - Nature Astronomy, 5, 145-149 (2021/February-0)

Strong toroidal magnetic fields required by quiescent X-ray emission of magnetars.

IGOSHEV A.P., HOLLERBACH R., WOOD T. and GOURGOULIATOS K.N.

Abstract (from CDS):

Magnetars are neutron stars (NSs) with extreme magnetic fields of strength 5 x 1013-1015 G. These fields are generated by dynamo action during the proto-NS phase, and are expected to have both poloidal and toroidal components, although the energy of the toroidal component could be ten times larger. Only the poloidal dipolar field can be measured directly, via NS spin-down. The magnetic field provides heating and governs how this heat flows through the crust. Magnetar thermal X-ray emission in quiescence is modulated with the rotational period of the NS, with a typical pulsed fraction 10-58%, implying that the surface temperature is substantially non-uniform despite the high thermal conductivity of the star's crust. Poloidal dipolar fields cannot explain this large pulsed fraction. Previous two-dimensional simulations have shown that a strong, large-scale toroidal magnetic field pushes a hot region into one hemisphere and increases the pulsed fraction. Here, we report three-dimensional magneto-thermal simulations of magnetars with strong, large-scale toroidal magnetic fields. These models, combined with ray propagation in curved spacetime, accurately describe the observed light curves of 10 out of 19 magnetars in quiescence and allow us to further constrain their rotational orientation. We find that the presence of a strong toroidal magnetic field is enough to explain the strong modulation of thermal X-ray emission in quiescence.

Abstract Copyright: ©

Journal keyword(s): Astrophysics - High Energy Astrophysical Phenomena

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 18

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Number of rows : 18
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 PSR J0100-7211 Psr 01 00 42.86 -72 11 33.3   17.69 17.82     B3V 101 0
2 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
3 NAME Sgr J0418+5729 gam 04 18 33.867 +57 32 22.91           ~ 244 0
4 PSR J0501+4516 Psr 05 01 06.600 +45 16 33.96           ~ 142 0
5 2E 2336 HXB 10 50 08.93 -59 53 19.9           Be 419 0
6 PSR J1119-6127 Psr 11 19 14.30 -61 27 49.5           ~ 439 1
7 PSR J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 463 1
8 PSR J1647-4552 Psr 16 47 10.18 -45 52 16.7           ~ 217 1
9 PSR J1708-4008 Psr 17 08 46.1 -40 08 56           ~ 315 0
10 [AAB2008] 1 X 17 14 05.7 -38 10 31           ~ 69 1
11 PSR J1745-2900 Psr 17 45 40.1640 -29 00 29.818           ~ 358 0
12 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
13 1WGA J1822.2-1604 X 18 22 18.32 -16 04 27.2           ~ 141 0
14 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 296 1
15 PSR J1852+0033 Psr 18 52 46.60 +00 33 20.9           ~ 51 0
16 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0
17 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
18 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1

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