2020ApJ...893....9Z


Query : 2020ApJ...893....9Z

2020ApJ...893....9Z - Astrophys. J., 893, 9-9 (2020/April-2)

Magnetars from neutron star-white dwarf mergers: application to fast radio bursts.

ZHONG S.-Q. and DAI Z.-G.

Abstract (from CDS):

It is widely believed that magnetars could be born in core-collapse supernovae (SNe), binary neutron star (BNS) or binary white dwarf (BWD) mergers, or accretion-induced collapse (AIC) of white dwarfs. In this paper, we investigate whether magnetars could also be produced from neutron star-white dwarf (NSWD) mergers, motivated by FRB 180924-like fast radio bursts (FRBs) possibly from magnetars born in BNS/BWD/AIC channels suggested by Margalit et al. (2019). By a preliminary calculation, we find that NSWD mergers with unstable mass transfer could result in the NS acquiring an ultra-strong magnetic field via the dynamo mechanism due to differential rotation and convection or possibly via the magnetic flux conservation scenario of a fossil field. If NSWD mergers can indeed create magnetars, then such objects could produce at least a subset of FRB 180924-like FRBs within the framework of flaring magnetars, since the ejecta, local environments, and host galaxies of the final remnants from NSWD mergers resemble those of BNS/BWD/AIC channels. This NSWD channel is also able to well explain both the observational properties of FRB 180924-like and FRB 180916.J0158+65-like FRBs within a large range in local environments and host galaxies.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Compact binary stars - Gravitational waves - Magnetars - Radio bursts

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 FRB 20180916B rB 01 58 00.750 +65 43 00.30           ~ 457 0
2 [BTS2017] CDF-S XT2 G 03 32 18.38112 -27 52 23.8692   26.509     24.598 ~ 46 0
3 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
4 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
5 FRB 180924 rB 21 44 25.255 -40 54 00.10           ~ 140 0
6 FRB 181112 rB 21 49 23.630 -52 58 15.39           ~ 131 0
7 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
8 FRB 171019 rB 22 17.5 -08 40           ~ 52 0

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