2022ApJ...932..105J


Query : 2022ApJ...932..105J

2022ApJ...932..105J - Astrophys. J., 932, 105-105 (2022/June-3)

Gravitational-wave Statistics for Pulsar Timing Arrays: Examining Bias from Using a Finite Number of Pulsars.

JOHNSON A.D., VIGELAND S.J., SIEMENS X. and TAYLOR S.R.

Abstract (from CDS):

Recently, many different pulsar timing array (PTA) collaborations have reported strong evidence for a common stochastic process in their data sets. The reported amplitudes are in tension with previously computed upper limits. In this paper, we investigate how using a subset of a set of pulsars biases Bayesian upper limit recovery. We generate 500 simulated PTA data sets, based on the NANOGrav 11 yr data set with an injected stochastic gravitational-wave background (GWB). We then compute the upper limits by sampling the individual pulsar likelihoods, and combine them through a factorized version of the PTA likelihood to obtain upper limits on the GWB amplitude, using different numbers of pulsars. We find that it is possible to recover an upper limit (95% credible interval) below the injected value, and that it is significantly more likely for this to occur when using a subset of pulsars to compute the upper limit. When picking pulsars to induce the maximum possible bias, we find that the 95% Bayesian upper limit recovered is below the injected value in 10.6% of the realizations (53 of 500). Further, we find that if we choose a subset of pulsars in order to obtain a lower upper limit than when using the full set of pulsars, the distribution of the upper limits obtained from these 500 realizations is shifted to lower-amplitude values.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Astronomy data analysis

Simbad objects: 22

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Number of rows : 22
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 J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
3 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
4 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
5 PSR J1455-3300 Psr 14 55 47.976991 -33 30 46.40280           ~ 165 1
6 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
7 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
8 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
9 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
10 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
11 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
12 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 122 0
13 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
14 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
15 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
16 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
17 PSR J1910+1256 Psr 19 10 09.701454 +12 56 25.48680           ~ 108 1
18 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
19 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
20 PSR J2010-1323 Psr 20 10 45.922635 -13 23 56.13270           ~ 93 0
21 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
22 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1

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