2016MNRAS.457.4421C


Query : 2016MNRAS.457.4421C

2016MNRAS.457.4421C - Mon. Not. R. Astron. Soc., 457, 4421-4440 (2016/April-3)

The noise properties of 42 millisecond pulsars from the European Pulsar Timing Array and their impact on gravitational-wave searches.

CABALLERO R.N., LEE K.J., LENTATI L., DESVIGNES G., CHAMPION D.J., VERBIEST J.P.W., JANSSEN G.H., STAPPERS B.W., KRAMER M., LAZARUS P., POSSENTI A., TIBURZI C., PERRODIN D., OSLOWSKI S., BABAK S., BASSA C.G., BREM P., BURGAY M., COGNARD I., GAIR J.R., GRAIKOU E., GUILLEMOT L., HESSELS J.W.T., KARUPPUSAMY R., LASSUS A., LIU K., McKEE J., MINGARELLI C.M.F., PETITEAU A., PURVER M.B., ROSADO P.A., SANIDAS S., SESANA A., SHAIFULLAH G., SMITS R., TAYLOR S.R., THEUREAU G., VAN HAASTEREN R. and VECCHIO A.

Abstract (from CDS):

The sensitivity of Pulsar Timing Arrays to gravitational waves (GWs) depends on the noise present in the individual pulsar timing data. Noise may be either intrinsic or extrinsic to the pulsar. Intrinsic sources of noise will include rotational instabilities, for example. Extrinsic sources of noise include contributions from physical processes which are not sufficiently well modelled, for example, dispersion and scattering effects, analysis errors and instrumental instabilities. We present the results from a noise analysis for 42 millisecond pulsars (MSPs) observed with the European Pulsar Timing Array. For characterizing the low-frequency, stochastic and achromatic noise component, or 'timing noise', we employ two methods, based on Bayesian and frequentist statistics. For 25 MSPs, we achieve statistically significant measurements of their timing noise parameters and find that the two methods give consistent results. For the remaining 17 MSPs, we place upper limits on the timing noise amplitude at the 95 per cent confidence level. We additionally place an upper limit on the contribution to the pulsar noise budget from errors in the reference terrestrial time standards (below 1 per cent), and we find evidence for a noise component which is present only in the data of one of the four used telescopes. Finally, we estimate that the timing noise of individual pulsars reduces the sensitivity of this data set to an isotropic, stochastic GW background by a factor of >9.1 and by a factor of >2.3 for continuous GWs from resolvable, inspiralling supermassive black hole binaries with circular orbits.

Abstract Copyright: © 2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

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

Simbad objects: 42

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Number of rows : 42
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 J0034-05 Psr 00 34 21.8281 -05 34 36.620           ~ 201 0
3 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
4 PSR J0610-2100 Psr 06 10 13.602953 -21 00 27.74435           ~ 116 0
5 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
6 PSR J0621+10 Psr 06 21 22.11108 +10 02 38.7410           ~ 128 1
7 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
8 PSR J0900-3144 Psr 09 00 43.95220 -31 44 30.8722           ~ 68 0
9 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
10 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
11 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
12 PSR J1455-3300 Psr 14 55 47.976991 -33 30 46.40280           ~ 165 1
13 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
14 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
15 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
16 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
17 PSR J1721-2457 Psr 17 21 05.50008 -24 57 06.2260           ~ 37 0
18 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
19 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
20 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
21 PSR J1751-2857 Psr 17 51 32.686848 -28 57 46.57130           ~ 65 1
22 PSR J1801-1417 Psr 18 01 51.064902 -14 17 34.54980           ~ 45 0
23 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
24 PSR J1804-27 Psr 18 04 21.13307 -27 17 31.3370           ~ 87 1
25 PSR J1843-1113 Psr 18 43 41.260405 -11 13 31.10310           ~ 86 0
26 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
27 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
28 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
29 PSR J1910+1256 Psr 19 10 09.701454 +12 56 25.48680           ~ 108 1
30 PSR J1911-11 Psr 19 11 49.2927 -11 14 22.330           ~ 87 1
31 PSR J1911+1347 Psr 19 11 55.204694 +13 47 34.38383           ~ 72 0
32 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
33 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
34 PSR B1953+29 Psr 19 55 27.8680959374 +29 08 43.499227152           ~ 303 1
35 PSR J2010-1323 Psr 20 10 45.922635 -13 23 56.13270           ~ 93 0
36 PSR J2019+24 Psr 20 19 31.94900 +24 25 15.3038           ~ 145 1
37 PSR J2033+1736 Psr 20 33 16.9140266736 +17 37 48.047177388   11.59 10.50     ~ 76 0
38 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
39 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
40 PSR J2229+26 Psr 22 29 50.883815 +26 43 57.61393           ~ 121 1
41 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1
42 PSR J2322+2057 Psr 23 22 22.320041 +20 57 02.50080           ~ 129 1

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