2017MNRAS.464L..65H


Query : 2017MNRAS.464L..65H

2017MNRAS.464L..65H - Mon. Not. R. Astron. Soc., 464, L65-L69 (2017/January-1)

Ejector and propeller spin-down: how might a superluminous supernova millisecond magnetar become the 6.67 h pulsar in RCW 103.

HO W.C.G. and ANDERSSON N.

Abstract (from CDS):

The X-ray source 1E 161348-5055 in the supernova remnant RCW 103 recently exhibited X-ray activity typical of magnetars, i.e. neutron stars with magnetic fields >= 1014-1015 G. However, 1E 161348-5055 has an observed period of 6.67 h, in contrast to magnetars which have a spin period of seconds. Here we describe a simple model which can explain the spin evolution of 1E 161348-5055, as well as other magnetars, from an initial period of milliseconds that would be required for dynamo generation of magnetar-strength magnetic fields. We propose that the key difference between 1E 161348-5055 and other magnetars is the persistence of a remnant disc of small total mass. This disc caused 1E 161348-5055 to undergo ejector and propeller phases in its life, during which strong torques caused a rapid increase of its spin period. By matching its observed spin period and ≃1-3 kyr age, we find that 1E 161348-5055 has the (slightly) highest magnetic field of all known magnetars, with B ∼ 5 x 1015 G, and that its disc had a mass of ∼1024 g, comparable to that of the asteroid Ceres.

Abstract Copyright: © 2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): accretion, accretion discs - stars: individual: 1E 161348-5055 - RCW 103 - stars: magnetars - stars: magnetic field - stars: neutron - supernovae: general - supernovae: general

Simbad objects: 4

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Number of rows : 4
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 J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
2 AJG 44 Psr 16 17 33.000 -51 02 00.00           ~ 552 3
3 2E 3623 X 16 17 36.30 -51 02 26.6           ~ 126 1
4 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2

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