I. Cognard et al., HIGH-PRECISION TIMING OBSERVATIONS OF THE MILLISECOND PULSAR PSR1821-24 AT NANCAY, Astronomy and astrophysics, 311(1), 1996, pp. 179-188
High-precision timing observations of the millisecond pulsar PSR 1821-
24 have been conducted on 305 individual dates at the Nancay radiotele
scope at 1.4 GHz between March 2 1989 and July 21 1993. The Time Of Ar
rival residuals after the standard fit of the pulsar parameters are ch
aracterised by a rms of 2.78 mu s. This dense and precise timing serie
s has allowed the first determination of the apparent second period de
rivative P for PSR 1821-24 and of its proper motion. We find that the
observed quasi-cubic variation (i.e. the apparent P) of the post-fit r
esiduals matches the level of low-frequency noise predicted by the emp
irical relationship of Arzoumanian et al. (1994) for the rotation irre
gularities of classical pulsars. We conclude that the millisecond puls
ar PSR 1821-24, similarly to PSR 1937+21, exhibits instrinsic rotation
irregularities, unless P is a jerk (it) induced during a close encoun
ter in the globular cluster M28. This pulsar is the youngest known mil
lisecond pulsar according to a characteristic age (1/2 P-0/P-0) of 30
x 10(6) yr. Relatively young millisecond pulsars, like PSR 1821-24 and
PSR 1937+21, might be prone to rotation irregularities while old mill
isecond pulsars like PSR 1855+09 an more stable. We find a discrepancy
between the optical proper motion of M28 and our timing proper motion
of PSR 1821-24 larger than the pulsar escape velocity in the cluster.
Reconciling these two proper motions is important for the kinematics
of M28 and the study of the gravitational potential of the Galactic di
sk and bulge. Finally, we present the daily timing observations of PSR
1821-24 conducted every year since 1989 when the solar corona interve
nes between the pulsar and the Earth at Christmas time. We have used t
hese timing observations along a single cut through the corona to fit
a spherically symmetric model of its electron density n(e) = n(0)(r/r(
0))(-alpha). With a slightly more sophisticated model for the coronal
electron density, precise timing observations of PSR 1821-24 during th
ese periods over a complete solar cycle could monitor the global flatt
ening expected for the coronal plasma at the solar minimum.