2025MNRAS.539.3655S


Query : 2025MNRAS.539.3655S

2025MNRAS.539.3655S - Mon. Not. R. Astron. Soc., 539, 3655-3668 (2025/June-1)

Magnetar structure in non-linear electrodynamics with mixed poloidal-toroidal fields.

SUVOROV A.G. and PONS J.A.

Abstract (from CDS):

Magnetars have inferred polar field strengths in excess of the Schwinger limit, where non-linear electromagnetic effects can be significant. Their internal fields may be even stronger, suggesting that Maxwellian characterizations of hydromagnetic structure may require revision. A generalized Grad-Shafranov equation, describing static and axisymmetric fluid stars with mixed poloidal-toroidal fields, is introduced and subsequently solved in a perturbative scheme to calculate quadrupolar deformations. In the Born-Infeld theory, we show that the toroidal field has a maximum strength set by the scale parameter, b, implying an upper limit to the stellar prolateness, $|\epsilon _{\rm max}| \sim 10^{-5} \left(b/10^{16}\text{ G}\right)^2$, that is independent of field specifics. Observations of magnetar phenomena that are interpreted as evidence for ellipticity, such as precession, can thus implicitly constrain post-Maxwellian parameters in a way that complements terrestrial experiments. Toroidal ceilings also have implications for dynamo theory and gravitational waves, which we revisit together with field evolution in crusts abiding by beyond-Maxwell physics.

Abstract Copyright: © 2025 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): gravitational waves - magnetohydrodynamics - magnetic fields - stars: magnetars

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 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
2 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
3 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2
4 NAME ASKAP J1832-0911 Rad 18 32 48.4589 -09 11 15.297           ~ 13 0
5 RX J1856.6-3754 Psr 18 56 35.11 -37 54 30.5     25.7     ~ 456 0
6 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
7 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
8 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1

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