2010ApJ...721.1193P


Query : 2010ApJ...721.1193P

2010ApJ...721.1193P - Astrophys. J., 721, 1193-1205 (2010/October-1)

The evolution of PSR J0737-3039B and a model for relativistic spin precession.

PERERA B.B.P., McLAUGHLIN M.A., KRAMER M., STAIRS I.H., FERDMAN R.D., FREIRE P.C.C., POSSENTI A., BRETON R.P., MANCHESTER R.N., BURGAY M., LYNE A.G. and CAMILO F.

Abstract (from CDS):

We present the evolution of the radio emission from the 2.8 s pulsar of the double pulsar system PSR J0737- 3039A/B. We provide an update on the Burgay et al. analysis by describing the changes in the pulse profile and flux density over five years of observations, culminating in the B pulsar's radio disappearance in 2008 March. Over this time, the flux density decreases by 0.177 mJy/yr at the brightest orbital phases and the pulse profile evolves from a single to a double peak, with a separation rate of 2{fdg}6/yr. The pulse profile changes are most likely caused by relativistic spin precession but cannot be easily explained with a circular hollow-cone beam as in the model of Clifton & Weisberg. Relativistic spin precession, coupled with an elliptical beam, can model the pulse profile evolution well and the reappearance is expected to happen in ∼2035 with the same part of the beam or in ∼2014 if we assume a symmetric beam shape. This particular beam shape predicts geometrical parameters for the two bright orbital phases which are consistent with and similar to those derived by Breton et al. However, the observed decrease in flux over time and B's eventual disappearance cannot be easily explained by the model and may be due to the changing influence of A on B.

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Journal keyword(s): pulsars: general - stars: neutron

Simbad objects: 7

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Number of rows : 7
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 J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
2 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
3 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
4 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
5 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
6 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
7 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1

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