2001MNRAS.327..639I


Query : 2001MNRAS.327..639I

2001MNRAS.327..639I - Mon. Not. R. Astron. Soc., 327, 639-662 (2001/October-3)

Magnetic deformation of magnetars for the giant flares of the soft gamma-ray repeaters.

IOKA K.

Abstract (from CDS):

We present one possible mechanism for the giant flares of the soft gamma-ray repeaters (SGRs) within the framework of the magnetar (superstrongly magnetized neutron star) model, motivated by the positive period increase associated with the August 27 event from SGR 1900+14. From second-order perturbation analysis of the equilibrium of the magnetic polytrope, we find that there exist different equilibrium states separated by the energy of the giant flares and the shift in the moment of inertia to cause the period increase. This suggests that, if we assume that global reconfiguration of the internal magnetic field of {formmu14} suddenly occurs, the positive period increase {formmu15} as well as the energy ≳1044erg of the giant flares may be explained. The moment of inertia can increase with a release of energy, because the star shape deformed by the magnetic field can be prolate rather than oblate. In this mechanism, since oscillation of the neutron star will be excited, a ∼ms-period pulsation of the burst profile and an emission of gravitational waves are expected. The gravitational waves could be detected by planned interferometers such as LIGO, VIRGO and LCGT.

Abstract Copyright: The Royal Astronomical Society

Journal keyword(s): gravitation - gravitational waves - stars: magnetic fields - stars: neutron - gamma-rays: bursts - gamma-rays: theory

Simbad objects: 5

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Number of rows : 5
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 B0525-66 Psr 05 26 00.7 -66 04 35           ~ 569 1
2 GRB 980618A gB 16 35 52 -47 35.2           ~ 270 0
3 NAME Sgr 1801-23 gam 18 00 58.9 -22 56 48           ~ 40 0
4 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2
5 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0

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