2024MNRAS.527.2297K


Query : 2024MNRAS.527.2297K

2024MNRAS.527.2297K - Mon. Not. R. Astron. Soc., 527, 2297-2302 (2024/January-2)

How different is the magnetic field at the core-crust interface from that at the neutron star surface? The range allowed in magnetoelastic equilibrium.

KOJIMA Y. and YOSHIDA S.

Abstract (from CDS):

This study was focused on the investigation of a magnetic field penetrating from the core of a neutron star to its surface. The range of possible field configurations in the intermediate solid crust is less limited owing to the elastic force acting on the force balance. When the Lorentz force is excessively strong, the magnetoelastic equilibrium does not hold, and thus, the magnetic field becomes constrained. By numerically solving for the magnetoelastic equilibrium in a thin crust, the range of the magnetic field at the core-crust interface was determined, while assuming the exterior to be fixed as a dipole in vacuum. The results revealed that the toroidal component should be smaller than the poloidal component at the core-crust interface for the surface dipole, B0 > 2.1 × 1014 G. Consequently, a strong toroidal field, for example, B ∼ 1016 G, as suggested by free precession of magnetars should be confined to a deep interior core and should be reduced to B ∼ 1014 G at the bottom of the crust. The findings of this study provide insights into the interior field structure of magnetars. Further investigations on more complicated geometries with higher multipoles and exterior magnetosphere are necessary.

Abstract Copyright: © 2023 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): stars: magnetars - stars: magnetic field - stars: neutron

Simbad objects: 3

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Number of rows : 3
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 PSR J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 463 1
3 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0

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