2013MNRAS.431.1136C


Query : 2013MNRAS.431.1136C

2013MNRAS.431.1136C - Mon. Not. R. Astron. Soc., 431, 1136-1142 (2013/May-2)

On the evolution of the radio pulsar PSR J1734-3333.

CALISKAN S., ERTAN U., ALPAR M.A., TRUMPER J.E. and KYLAFIS N.D.

Abstract (from CDS):

Recent measurements showed that the period derivative of the `high-B' radio pulsar PSR J1734-3333 is increasing with time. For neutron stars evolving with fallback discs, this rotational behaviour is expected in certain phases of the long-term evolution. Using the same model as employed earlier to explain the evolution of anomalous X-ray pulsars (AXPs) and soft gamma-ray repeaters, we show that the period, the first and second period derivatives and the X-ray luminosity of this source can simultaneously acquire the observed values for a neutron star evolving with a fallback disc. We find that the required strength of the dipole field that can produce the source properties is in the range 1012-1013G on the pole of the neutron star. When the model source reaches the current state properties of PSR J1734-3333, accretion on to the star has not started yet, allowing the source to operate as a regular radio pulsar. Our results imply that PSR J1734-3333 is at an age of ∼ 3 x 104-2x105yr. Such sources will have properties like the X-ray dim isolated neutron stars or transient AXPs at a later epoch of weak accretion from the diminished fallback disc.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): accretion, accretion discs - stars: neutron - pulsars: individual: PSR J1734-3333

Simbad objects: 5

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Number of rows : 5
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 J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
2 NAME Sgr J0418+5729 gam 04 18 33.867 +57 32 22.91           ~ 244 0
3 PSR B1731-33.5 Psr 17 34 26.6 -33 33 22           ~ 104 1
4 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
5 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1

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