2026ApJ...999..156S


Query : 2026ApJ...999..156S

2026ApJ...999..156S - Astrophys. J., 999, 156 (2026/March-2)

The NANOGrav 15 yr Dataset: Improved Timing Precision with Very Long Baseline Interferometry Astrometric Priors.

SOSA FISCELLA S.V., LAM M.T., AGAZIE G., ANUMARLAPUDI A., ARCHIBALD A.M., ARZOUMANIAN Z., BAKER P.T., BROOK P.R., CROMARTIE H.T., CROWTER K., DE BIASI M.S., DECESAR M.E., DEMOREST P.B., DOLCH T., FERRARA E.C., FIORE W., FONSECA E., FREEDMAN G.E., GARVER-DANIELS N., GENTILE P.A., GLASER J., GOOD D.C., HAZBOUN J.S., JENNINGS R.J., JONES M.L., KAPLAN D.L., KERR M., LORIMER D.R., LUO J., LYNCH R.S., McEWEN A., McLAUGHLIN M.A., McMANN N., MEYERS B.W., NG C., NICE D.J., PENNUCCI T.T., PERERA B.B.P., POL N.S., RADOVAN H.A., RANSOM S.M., RAY P.S., SCHMIEDEKAMP A., SCHMIEDEKAMP C., SHAPIRO-ALBERT B.J., STAIRS I.H., STOVALL K., SUSOBHANAN A., SWIGGUM J.K. and WAHL H.M.

Abstract (from CDS):

Accurate pulsar astrometric estimates are essential to almost all high-precision pulsar timing experiments. Traditional pulsar timing techniques refine these estimates by including them as free parameters when fitting a model to observed pulse time-of-arrival measurements. However, reliable submilliarcsecond astrometric estimations require years of observations. Even then, power from red noise can be inadvertently absorbed into astrometric parameter fits. This effect biases the resulting estimates and reduces the sensitivity to red noise processes, including gravitational waves (GWs). In this work, we seek to mitigate these shortcomings by using pulsar astrometric estimates derived from very long baseline interferometry (VLBI) as priors for the timing fit. First, we used VLBI and timing astrometric estimates of 18 millisecond pulsars to calibrate a rotation between the reference frames used in timing and VLBI, with a precision of ∼0.7 mas. Through this frame tie, we combined timing- and VLBI-based probabilities to obtain a maximum-posterior astrometric solution. We found offsets between our results and the timing-based astrometric solutions, which, if real, would lead to the absorption of spectral power at the frequencies of interest for single-source GW searches. However, we do not find significant power absorption due to astrometric fitting at the low-frequency domain of the GW background.

Abstract Copyright: © 2026. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Pulsars - Astrometry - Very long baseline interferometry

Simbad objects: 23

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Number of rows : 23
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 Z 538-57 Sy1 02 23 11.41124925 +42 59 31.3853324   15.71 14.81     ~ 582 2
3 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
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 J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
7 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
8 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
9 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
10 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
11 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
12 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
13 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
14 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
15 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
16 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
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 J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
22 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
23 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1

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