2023MNRAS.523.4603K


Query : 2023MNRAS.523.4603K

2023MNRAS.523.4603K - Mon. Not. R. Astron. Soc., 523, 4603-4614 (2023/August-2)

Impact of quasi-periodic and steep-spectrum timing noise on the measurement of pulsar timing parameters.

KEITH M.J. and NITU I.C.

Abstract (from CDS):

Timing noise in pulsars is often modelled with a Fourier-basis Gaussian process that follows a power law with periodic boundary conditions on the observation time, Tspan. However, the actual noise processes can extend well below 1/Tspan, and many pulsars are known to exhibit quasi-periodic timing noise. In this paper, we investigate several adaptions that try to account for these differences between the observed behaviour and the simple power-law model. First, we propose to include an additional term that models the quasi-periodic spin-down variations known to be present in many pulsars. Secondly, we show that a Fourier basis of 1/2Tspan can be more suited for estimating long-term timing parameters such as the spin frequency second derivative (F2), and is required when the exponent of the power spectrum is greater than ∼4. We also implement a Bayesian version of the generalized least-squares 'Cholesky' method which has different limitations at low frequency, but find that there is little advantage over Fourier-basis methods. We apply our quasi-periodic spin-down model to a sample of pulsars with known spin-down variations and show that this improves parameter estimation of F2 and proper motion for the most pathological cases, but in general the results are consistent with a power-law model. The models are all made available through the RUN_ENTERPRISE software package.

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

Journal keyword(s): methods: data analysis - pulsars: general

Simbad objects: 18

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Number of rows : 18
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 B0740-28 Psr 07 42 49.0730 -28 22 43.510           ~ 445 0
2 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
3 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
4 PSR B1540-06 Psr 15 43 30.1373 -06 20 45.332           ~ 131 1
5 PSR B1642-03 Psr 16 45 02.0330 -03 17 57.200           ~ 394 0
6 PSR B1714-34 Psr 17 17 20.30000 -34 25 00.3100           ~ 55 0
7 PSR B1818-04 Psr 18 20 52.5920 -04 27 37.120           ~ 230 0
8 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
9 PSR B1826-17 Psr 18 29 43.15000 -17 51 13.0000           ~ 136 0
10 PSR B1828-10 Psr 18 30 47.566 -10 59 27.90           ~ 190 1
11 PSR B1839+09 Psr 18 41 55.92100 +09 12 07.2900           ~ 134 0
12 PSR B1903+07 Psr 19 05 53.62 +07 09 19.4           ~ 43 0
13 PSR B1906+09.1 Psr 19 09 19.91 +09 12 53.7           ~ 22 0
14 PSR B1907+00 Psr 19 09 35.25200 +00 07 56.8400           ~ 91 0
15 PSR B1930+20 Psr 19 32 08.023 +20 20 46.41           ~ 87 0
16 PSR J2037+3621 Psr 20 37 27.44 +36 21 24.1           ~ 62 0
17 PSR J2043+2740 Psr 20 43 43.5 +27 40 56           ~ 137 0
18 PSR B2148+63 Psr 21 49 58.7033 +63 29 44.277           ~ 96 0

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