2015MNRAS.454.3674Y


Query : 2015MNRAS.454.3674Y

2015MNRAS.454.3674Y - Mon. Not. R. Astron. Soc., 454, 3674-3678 (2015/December-3)

The evolution of the magnetic inclination angle as an explanation of the long term red timing-noise of pulsars.

YI S.-X. and ZHANG S.-N.

Abstract (from CDS):

We study the possibility that the long term red timing-noise in pulsars originates from the evolution of the magnetic inclination angle χ. The braking torque under consideration is a combination of the dipole radiation and the current loss. We find that the evolution of χ can give rise to extra cubic and fourth-order polynomial terms in the timing residuals. These two terms are determined by the efficiency of the dipole radiation, the relative electric-current density in the pulsar tube and χ. The following observation facts can be explained with this model: (a) young pulsars have positive 1; (b) old pulsars can have both positive and negative 1; (c) the absolute values of 1 are proportional to -{dot}ν; (d) the absolute values of the braking indices are proportional to the characteristic ages of pulsars. If the evolution of χ is purely due to rotation kinematics, then it cannot explain the pulsars with braking index less than 3, and thus the intrinsic change of the magnetic field is needed in this case. Comparing the model with observations, we conclude that the drift direction of χ might oscillate many times during the lifetime of a pulsar. The evolution of χ is not sufficient to explain the rotation behaviour of the Crab pulsar, because the observed χ and {dot}χ are inconsistent with the values indicated from the timing residuals using this model.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): Pulsars: General

Simbad objects: 10

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Number of rows : 10
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 PSR J0007+7303 Psr 00 07 00.6000137 +73 03 06.849976           ~ 171 1
2 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5263 0
3 PSR J1023-5746 Psr 10 23 02.84 -57 46 06.9           ~ 61 0
4 PSR J1418-6058 Psr 14 18 42.725 -60 58 01.89           ~ 120 0
5 PSR B1509-58 Psr 15 13 55.52 -59 08 08.8     13.06     ~ 845 1
6 PSR B1620-26 Psr 16 23 38.2218 -26 31 53.769     21.30     ~ 295 2
7 PSR J1824-2452A Psr 18 24 32.009 -24 52 11.10           ~ 501 2
8 NAME Sgr 1833-0832 gam 18 33 46.0 -08 32 13           ~ 80 0
9 PSR B1937+21 Psr 19 39 39.6 +21 37 22           ~ 1068 2
10 PSR B2334+61 Psr 23 37 05.779 +61 51 01.69           ~ 190 1

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