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Microsecond Timing of PSR B1821−24 withChandraHigh Resolution Camera–S
Author(s) -
Robert E. Rutledge,
D. B. Fox,
S. R. Kulkarni,
B. A. Jacoby,
I. Cognard,
D. C. Backer,
S. S. Murray
Publication year - 2004
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/380299
Subject(s) - physics , pulsar , astrophysics , ephemeris , flux (metallurgy) , millisecond pulsar , dispersion (optics) , millisecond , noise (video) , microsecond , wavelength , pulse (music) , optics , astronomy , detector , satellite , materials science , artificial intelligence , computer science , metallurgy , image (mathematics)
We perform absolute timing of PSR B1821-24 in M28, using a 50 ksecobservation with Chandra/HRC-S. We have obtained the highest signal-to-noiseX-ray pulsed lightcurve of this source to date, detecting two X-ray pulses, aswell as significant non-pulsed emission -- a persistent X-ray flux whichcomprises 15+/-3% of the total X-ray flux of the pulsar. The Gaussian width ofthe sharp X-ray peak is 34+/-3 micro-sec in time, implying a size of the X-raybeam as it crosses the line of sight of 4.0+/-0.4 deg. We find evidence for asignificant trailing component in both X-ray peaks of the pulse profile.Including three RXTE/PCA observations in our analysis, and tying the phasestogether using a radio ephemeris obtained at Nancay, we find the absolutephases in the X-ray wander with respect to this radio ephemeris by up to 60micro-sec, likely due to the variable dispersion measure, which changes thepulse arrival time in the radio band but not the X-ray band. The presentanalysis makes clear that study of pulsar timing noise properties inmillisecond pulsars such as PSR B1821-24 -- hitherto only studied at radiowavelengths, where variable dispersion measure requires a significantcorrection -- can be studied at X-ray wavelengths, where the effect of variabledispersion measure is negligible. We also examine the known uncertainties inthe absolute Chandra/HRC-S timing accuracy, which amount to +/-12 microsec. Welimit the amount of linear drift in the relative timing accuracy of HRC-S to<3e-10 s s-1.Comment: ApJ, accepted; minor changes from original versio

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