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25 April 2024
 
  » arxiv » astro-ph/9903048

 Article overview



Profile instabilities of the millisecond pulsar PSR J1022+1001
M.Kramer ; K.M.Xilouris ; F.Camilo ; D.J.Nice ; D.C.Backer ; C.Lange ; D.R.Lorimer ; O.Doroshenko ; S.Sallmen ;
Date 2 Mar 1999
Subject astro-ph
Affiliation1,2), K.M.Xilouris , F.Camilo , D.J.Nice , D.C.Backer , C.Lange , D.R.Lorimer (2,3), O.Doroshenko , S.Sallmen ( Astronomy Deparment, UC Berkeley; MPI fuer Radioastronomie, Bonn; NAIC Arecibo Observatory; NRAL, Jodrell Bank; Joseph Henry Laborator
AbstractWe present evidence that the integrated profiles of some millisecond pulsars exhibit severe changes that are inconsistent with the moding phenomenon as known from slowly rotating pulsars. We study these profile instabilities in particular for PSR J1022+1001 and show that they occur smoothly, exhibiting longer time constants than those associated with moding. In addition, the profile changes of this pulsar seem to be associated with a relatively narrow-band variation of the pulse shape. Only parts of the integrated profile participate in this process which suggests that the origin of this phenomenon is intrinsic to the pulsar magnetosphere and unrelated to the interstellar medium. A polarization study rules out profile changes due to geometrical effects produced by any sort of precession. However, changes are observed in the circularly polarized radiation component. In total we identify four recycled pulsars which also exhibit instabilities in the total power or polarization profiles due to an unknown phenomenon (PSRs J1022+1001, J1730-2304, B1821-24, J2145-0750). The consequences for high precision pulsar timing are discussed in view of the standard assumption that the integrated profiles of millisecond pulsars are stable. As a result we present a new method to determine pulse times-of-arrival that involves an adjustment of relative component amplitudes of the template profile. Applying this method to PSR J1022+1001, we obtain an improved timing solution with a proper motion measurement of -17 pm 2 mas/yr in ecliptic longitude. Assuming a distance to the pulsar as inferred from the dispersion measure this corresponds to an one-dimensional space velocity of 50 km/s.
Source arXiv, astro-ph/9903048
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