2020A&A...644A.153D


Query : 2020A&A...644A.153D

2020A&A...644A.153D - Astronomy and Astrophysics, volume 644A153-153 (2020/12-1)

Dispersion measure variability for 36 millisecond pulsars at 150 MHz with LOFAR.

DONNER J.Y., VERBIEST J.P.W., TIBURZI C., OSLOWSKI S., KUNSEMOLLER J., BAK NIELSEN A.-S., GRIESSMEIER J.-M., SERYLAK M., KRAMER M., ANDERSON J.M., WUCKNITZ O., KEANE E., KONDRATIEV V., SOBEY C., McKEE J.W., BILOUS A.V., BRETON R.P., BRUGGEN M., CIARDI B., HOEFT M., VAN LEEUWEN J. and VOCKS C.

Abstract (from CDS):


Context. Radio pulses from pulsars are affected by plasma dispersion, which results in a frequency-dependent propagation delay. Variations in the magnitude of this effect lead to an additional source of red noise in pulsar timing experiments, including pulsar timing arrays (PTAs) that aim to detect nanohertz gravitational waves.
Aims. We aim to quantify the time-variable dispersion with much improved precision and characterise the spectrum of these variations.
Methods. We use the pulsar timing technique to obtain highly precise dispersion measure (DM) time series. Our dataset consists of observations of 36 millisecond pulsars, which were observed for up to 7.1yr with the LOw Frequency ARray (LOFAR) telescope at a centre frequency of ∼150MHz. Seventeen of these sources were observed with a weekly cadence, while the rest were observed at monthly cadence.
Results. We achieve a median DM precision of the order of 10–5cm–3pc for a significant fraction of our sources. We detect significant variations of the DM in all pulsars with a median DM uncertainty of less than 2x10–4cm–3pc. The noise contribution to pulsar timing experiments at higher frequencies is calculated to be at a level of 0.1-10µs at 1.4GHz over a timespan of a few years, which is in many cases larger than the typical timing precision of 1µs or better that PTAs aim for. We found no evidence for a dependence of DM on radio frequency for any of the sources in our sample.
Conclusions. The DM time series we obtained using LOFAR could in principle be used to correct higher-frequency data for the variations of the dispersive delay. However, there is currently the practical restriction that pulsars tend to provide either highly precise times of arrival (ToAs) at 1.4GHz or a high DM precision at low frequencies, but not both, due to spectral properties. Combining the higher-frequency ToAs with those from LOFAR to measure the infinite-frequency ToA and DM would improve the result.

Abstract Copyright: © J. Y. Donner et al 2020

Journal keyword(s): gravitational waves - pulsars: general - ISM: structure

Simbad objects: 40

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Number of rows : 40
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 J0407+16 Psr 04 07 54.939 +16 07 16.40           ~ 35 1
5 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
6 PSR J0621+10 Psr 06 21 22.11108 +10 02 38.7410           ~ 128 1
7 PSR J0645+5158 Psr 06 45 59.08191 +51 58 14.9210           ~ 65 0
8 PSR J0712-68 Psr 07 11 54.153093 -68 30 47.23387           ~ 120 1
9 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
10 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
11 PSR J0952-0607 Psr 09 52 08.319 -06 07 23.49           ~ 103 0
12 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
13 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
14 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
15 PSR J1125+7819 Psr 11 25 59.851 +78 19 48.70           ~ 36 0
16 PSR B1257+12 Psr 13 00 03.1075 +12 40 55.155           ~ 546 1
17 PSR J1400-1431 Psr 14 00 37.00370 -14 31 47.0422           ~ 49 0
18 PSR J1544+4937 Psr 15 44 04.166 +49 37 57.45           ~ 89 1
19 PSR J1552+5437 Psr 15 52 53.33117 +54 37 05.7866           ~ 27 0
20 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
21 PSR J1658+36 Psr 16 58 26.5198 +36 30 30.095           ~ 14 0
22 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
23 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
24 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
25 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
26 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
27 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
28 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
29 PSR J1911-11 Psr 19 11 49.2927 -11 14 22.330           ~ 87 1
30 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
31 PSR J1923+2515 Psr 19 23 22.494560 +25 15 40.64360           ~ 53 0
32 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
33 PSR J1944+0907 Psr 19 44 09.32 +09 07 23.2           ~ 65 1
34 PSR B1953+29 Psr 19 55 27.8680959374 +29 08 43.499227152           ~ 303 1
35 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
36 V* LY Aqr Psr 20 51 07.52058 -08 27 37.6100           ~ 236 2
37 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
38 PSR J2222-0137 Psr 22 22 06.00015 -01 37 15.7827           ~ 78 0
39 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0
40 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1

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