2025A&A...699A.165C


Query : 2025A&A...699A.165C

2025A&A...699A.165C - Astronomy and Astrophysics, volume 699A165 (2025/7-1)

The Chinese Pulsar Timing Array Data Release I Single pulsar noise analysis.

CHEN S., XU H., GUO Y., WANG B., CABALLERO R.N., JIANG J., XU J., XUE Z., LEE K., YUAN J., XU Y., WANG J., HAO L., LUO J., HAN J., JIANG P., SHEN Z., WANG M., WANG N., XU R., WU X., QIAN L., GUAN X., HUANG M., SUN C. and ZHU Y.

Abstract (from CDS):

The Chinese Pulsar Timing Array (CPTA) has collected observations from 57 millisecond pulsars using the Five-hundred-meter Aperture Spherical Radio Telescope (FAST) for close to three years, for the purpose of searching for gravitational waves (GWs). To robustly search for ultra-low-frequency GWs, pulsar timing arrays (PTAs) need to use models to describe the noise from the individual pulsars. We report on the results from the single pulsar noise analysis of the CPTA data release I (DR1). Conventionally, power laws in the frequency domain are used to describe pulsar red noise and dispersion measurement (DM) variations over time. Employing Bayesian methods, we found the choice of number and range of frequency bins with the highest evidence for each pulsar individually. A comparison between a dataset using DM piecewise measured (DMX) values and a power-law Gaussian process to describe the DM variations shows strong Bayesian evidence in favour of the power-law model. Furthermore, we demonstrate that the constraints obtained from four independent software packages are very consistent with each other. The short time span of the CPTA DR1, paired with the large sensitivity of FAST, has proved to be a challenge for the conventional noise model using a power law. This mainly shows in the difficulty to separate different noise terms due to their covariances with each other. Nineteen pulsars are found to display covariances between the short-term white noise and long-term red and DM noise. With future CPTA datasets, we expect that the degeneracy can be broken. Finally, we compared the CPTA DR1 results against the noise properties found by other PTA collaborations. While we can see broad agreement, there is some tension between different PTA datasets for some of the overlapping pulsars. This could be due to the differences in the methods used to obtain the constraints or the different frequency range that is probed with the CPTA DR1, which probes a higher frequency range compared to the other PTAs.

Abstract Copyright: © The Authors 2025

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

Simbad objects: 57

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Number of rows : 57
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 J0023+0923 Psr 00 23 16.890 +09 23 24.18           ~ 137 0
2 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
3 PSR J0034-05 Psr 00 34 21.8281 -05 34 36.620           ~ 201 0
4 PSR J0154+1833 Psr 01 54 36.88273 +18 33 50.7580           ~ 14 0
5 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
6 PSR J0340+41 Psr 03 40 23.2887 +41 30 45.300           ~ 91 0
7 PSR J0406+3039 Psr 04 06 32.51840 +30 39 42.4004           ~ 11 0
8 PSR J0509+08 Psr 05 09 22.23485 +08 56 25.0248           ~ 23 0
9 PSR J0605+3757 Psr 06 05 05.5444336 +37 57 35.996704           ~ 42 0
10 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
11 PSR J0621+10 Psr 06 21 22.11108 +10 02 38.7410           ~ 128 1
12 PSR J0636+5129 Psr 06 36 04.84645 +51 28 59.9625           ~ 101 0
13 PSR J0645+5158 Psr 06 45 59.08191 +51 58 14.9210           ~ 65 0
14 PSR J0732+2314 Psr 07 32 37.5156 +23 14 54.210           ~ 12 0
15 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
16 PSR J0824+0028 Psr 08 24 24.84022 +00 28 00.5670           ~ 9 0
17 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
18 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
19 PSR J1327+3423 Psr 13 27 07.54840 +34 23 37.6765           ~ 5 0
20 PSR J1453+1902 Psr 14 53 45.7175 +19 02 12.224           ~ 41 1
21 PSR J1630+3734 Psr 16 30 36.4672852 +37 34 42.101440           ~ 48 0
22 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
23 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
24 PSR J1710+4923 Psr 17 10 04.442 +49 23 11.40           ~ 10 0
25 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
26 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
27 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 122 0
28 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
29 PSR J1745+1017 Psr 17 45 33.8371 +10 17 52.523           ~ 70 0
30 PSR J1832-0836 Psr 18 32 27.589497 -08 36 55.14540           ~ 86 0
31 PSR J1843-1113 Psr 18 43 41.260405 -11 13 31.10310           ~ 86 0
32 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
33 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
34 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
35 PSR J1910+1256 Psr 19 10 09.701454 +12 56 25.48680           ~ 108 1
36 PSR J1911-11 Psr 19 11 49.2927 -11 14 22.330           ~ 87 1
37 PSR J1911+1347 Psr 19 11 55.204694 +13 47 34.38383           ~ 72 0
38 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
39 PSR J1923+2515 Psr 19 23 22.494560 +25 15 40.64360           ~ 53 0
40 PSR J1944+0907 Psr 19 44 09.32 +09 07 23.2           ~ 65 1
41 PSR J1946+3417 Psr 19 46 25.13182 +34 17 14.6770           ~ 64 0
42 PSR B1953+29 Psr 19 55 27.8680959374 +29 08 43.499227152           ~ 303 1
43 PSR J2010-1323 Psr 20 10 45.922635 -13 23 56.13270           ~ 93 0
44 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 120 1
45 PSR J2019+24 Psr 20 19 31.94900 +24 25 15.3038           ~ 145 1
46 PSR J2022+2534 Psr 20 22 33.26 +25 34 42.5           ~ 6 0
47 PSR J2033+1736 Psr 20 33 16.9140266736 +17 37 48.047177388   11.59 10.50     ~ 76 0
48 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
49 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
50 PSR J2150-0326 Psr 21 50 27.235330 -03 26 32.83180           ~ 11 0
51 PSR J2214+3000 Psr 22 14 38.8480 +30 00 38.209           ~ 136 0
52 PSR J2229+26 Psr 22 29 50.883815 +26 43 57.61393           ~ 121 1
53 PSR J2234+06 Psr 22 34 22 +06 11.0           ~ 76 0
54 PSR J2234+0944 Psr 22 34 46.856913 +09 44 30.04150           ~ 82 0
55 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0
56 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1
57 PSR J2322+2057 Psr 23 22 22.320041 +20 57 02.50080           ~ 129 1

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