2021MNRAS.503.2764F


Query : 2021MNRAS.503.2764F

2021MNRAS.503.2764F - Mon. Not. R. Astron. Soc., 503, 2764-2775 (2021/May-2)

Modelling magnetohydrodynamic equilibrium in magnetars with applications to continuous gravitational wave production.

FREDERICK S.G., THOMPSON K.L. and KUCHERA M.P.

Abstract (from CDS):

Possessing the strongest magnetic fields in our Universe, magnetars mark an extremum of physical phenomena. The strength of their magnetic fields is sufficient to deform the shape of the stellar body, and when the rotational and magnetic axes are not aligned, these deformations lead to the production of gravitational waves (GWs) via a time-varying quadrupole moment. Such gravitational radiation differs from signals presently detectable by the Laser Interferometer Gravitational-Wave Observatory. These signals are continuous rather than the momentary 'chirp' waveforms produced by binary systems during the phases of inspiral, merger, and ringdown. Here, we construct a computational model for magnetar stellar structure with strong internal magnetic fields. We implement an n = 1 polytropic equation of state (EOS) and adopt a mixed poloidal and toroidal magnetic field model constrained by the choice of EOS. We utilize fiducial values for magnetar magnetic field strength and various stellar physical attributes. Via computational simulation, we measure the deformation of magnetar stellar structure to determine upper bounds on the strength of continuous GWs formed as a result of these deformations inducing non-axisymmetric rotation. We compute predictions of upper limit GW strain values for sources in the McGill Magnetar Catalog, an index of all detected magnetars.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): gravitational waves - MHD - stars: magnetars

CDS comments: MG J0418+5372 is a probable misprint for MG J0418+5732.

Simbad objects: 21

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Number of rows : 21
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 PSR B0525-66 Psr 05 26 00.7 -66 04 35           ~ 569 1
6 2E 2336 HXB 10 50 08.93 -59 53 19.9           Be 419 0
7 PSR J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 463 1
8 PSR J1622-4950 Psr 16 22 44.80000 -49 50 54.5000           ~ 169 0
9 GRB 980618A gB 16 35 52 -47 35.2           ~ 270 0
10 PSR J1647-4552 Psr 16 47 10.18 -45 52 16.7           ~ 217 1
11 PSR J1708-4008 Psr 17 08 46.1 -40 08 56           ~ 315 0
12 [AAB2008] 1 X 17 14 05.7 -38 10 31           ~ 69 1
13 PSR J1745-2900 Psr 17 45 40.1640 -29 00 29.818           ~ 358 0
14 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2
15 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
16 1WGA J1822.2-1604 X 18 22 18.32 -16 04 27.2           ~ 141 0
17 NAME Sgr 1833-0832 gam 18 33 46.0 -08 32 13           ~ 87 0
18 PSR J1834-0845 Psr 18 34 52.1 -08 45 56           ~ 98 0
19 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 296 1
20 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0
21 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1

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