2006MNRAS.369.1502H


Query : 2006MNRAS.369.1502H

2006MNRAS.369.1502H - Mon. Not. R. Astron. Soc., 369, 1502-1520 (2006/July-1)

High-precision baseband timing of 15 millisecond pulsars.

HOTAN A.W., BAILES M. and ORD S.M.

Abstract (from CDS):

We describe extremely precise timing experiments performed on five solitary and 10 binary millisecond pulsars during the past 3 yr, with the Caltech Parkes Swinburne Recorder (CPSR2) coherent dedispersion system at the Parkes 64-m radio telescope. 12 of our sources have rms timing residuals below 1.5µs and four are below 200ns. The quality of our data allows us to measure eight parallaxes and nine proper motions, from which we conclude that models of galactic electron density still have limited predictive power for individual objects. We derive a mean transverse velocity of 87+31/-14km/s for these pulsars, in good agreement with previous authors. We demonstrate that unless multifrequency observations are made, typical variations in dispersion measure (DM) could introduce an additional drift in arrival times of ∼1µs per year at 20-cm wavelengths. Our high timing precision means that Shapiro delay can be used to constrain the inclination angles and component masses of all but two of the selected binary systems. The signature of annual orbital parallax is detected in the timing of PSR J0437-4715 and PSR J1713+0747, providing additional geometric constraints. The timing of PSR J1909-3744 is used to demonstrate that the DE405 ephemeris is a better model of the Solar system than the earlier DE200. In addition, we show that pulsar astrometric parameters measured using DE200 and DE405 often differ significantly. In order to use pulsars to search for a cosmological gravitational wave background, it is desirable to time them against each other to eliminate Earth-based time standards. We demonstrate that PSR J1909-3744 can be used as a reference against which we obtain a very small rms residual of 133ns for PSR J1713+0747. Although the gain of the Parkes antenna is small compared to other telescopes involved in precision timing, we obtain some of the lowest rms residuals ever measured, highlighting the importance of good instrumentation such as CPSR2 and good analysis software.

Abstract Copyright: 2006 The Authors. Journal compilation © 2006 RAS

Journal keyword(s): pulsars: individual: J0437-4715 - pulsars: individual: J0613-0200 - pulsars: individual: J0711-6830 - pulsars: individual: J1022+1001 - pulsars: individual: J1024-0719 - pulsars: individual: J1045-4509

Simbad objects: 20

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Number of rows : 20
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 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
2 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
3 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
4 PSR J0712-68 Psr 07 11 54.153093 -68 30 47.23387           ~ 120 1
5 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
6 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
7 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
8 PSR J1045-45 Psr 10 45 50.179671 -45 09 54.05686           ~ 154 1
9 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
10 PSR J1604-72 Psr 16 03 35.670781 -72 02 32.82328           ~ 142 0
11 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
12 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
13 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 948 1
14 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
15 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
16 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
17 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
18 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
19 PSR J2129-5718 Psr 21 29 22.781548 -57 21 14.33356           ~ 122 1
20 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0

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