2023MNRAS.519.1080G


Query : 2023MNRAS.519.1080G

2023MNRAS.519.1080G - Mon. Not. R. Astron. Soc., 519, 1080-1097 (2023/February-2)

Precession of magnetars: dynamical evolutions and modulations on polarized electromagnetic waves.

GAO Y., SHAO L., DESVIGNES G., JONES D.I., KRAMER M. and YIM G.

Abstract (from CDS):

Magnetars are conjectured to be highly magnetized neutron stars (NSs). Strong internal magnetic field and elasticity in the crust may deform the stars and lead to free precession. We study the precession dynamics of triaxially deformed NSs incorporating the near-field and the far-field electromagnetic torques. We obtain timing residuals for different NS geometries and torques. We also investigate the polarized X-ray and radio signals from precessing magnetars. The modulations on the Stokes parameters are obtained for thermal X-rays emitted from the surface of magnetars. For radio signals, we apply the simple rotating vector model (RVM) to give the modulations on the position angle (PA) of the polarization. Our results are comprehensive, ready to be used to search for magnetar precession with timing data and polarizations of X-ray and radio emissions. Future observations of precessing magnetars will give us valuable information on the geometry and the strength of the strong magnetic fields, the emission geometry, as well as the equation of state of NSs.

Abstract Copyright: © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): polarization - methods: analytical - stars: magnetars - X-rays: general

Simbad objects: 6

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Number of rows : 6
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 2E 3623 X 16 17 36.30 -51 02 26.6           ~ 126 1
4 PSR B1828-10 Psr 18 30 47.566 -10 59 27.90           ~ 190 1
5 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0
6 PSR J1933+2421 Psr 19 33 37.83 +24 36 39.6           ~ 157 0

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