2011MNRAS.411.1917W


Query : 2011MNRAS.411.1917W

2011MNRAS.411.1917W - Mon. Not. R. Astron. Soc., 411, 1917-1934 (2011/March-1)

The glitch-induced identity changes of PSR J1119-6127.

WELTEVREDE P., JOHNSTON S. and ESPINOZA C.M.

Abstract (from CDS):

Rotation-powered radio pulsars are generally observed to pulse regularly in the radio band, but this is not the case for so-called rotating radio transients (RRATs) which emit only sporadic bursts of radio emission. We demonstrate that the high-magnetic field pulsar J1119-6127 exhibits three different types of behaviour in the radio band. Trailing the `normal' profile peak there is an `intermittent' peak and these components are flanked by two additional components showing very erratic `RRAT-like' emission. Both the intermittent and RRAT-like events are extremely rare and are preceded by a large amplitude glitch in the spin-down parameters. The post-glitch relaxation occurs on two different time-scales (∼20 and ∼210 d) and the post-glitch spin-down rate is smaller than the pre-glitch rate. This type of relaxation is also seen in an earlier, smaller glitch and is very unusual for the pulsar population as a whole, but is observed in the glitch recovery of an RRAT. The abnormal emission behaviour in PSR J1119-6127 was observed up to three months after the epoch of the large glitch, suggestive of changes in the magnetospheric conditions during the fast part of the recovery process. We argue that both the anomalous recoveries and the emission changes could be related to reconfigurations of the magnetic field. Apart from the glitches, the spin-down of PSR J1119-6127 is relatively stable, allowing us to refine the measurement of the braking index (n= 2.684±0.002) using more than 12 yr of timing data.

The properties of this pulsar are discussed in light of the growing evidence that RRATs do not form a distinct class of pulsar, but rather are a combination of different extreme emission types seen in other neutron stars. Different sub-classes of the RRATs can potentially be separated by calculating the lower limit on the modulation index of their emission. Unlike other quantities, this parameter is independent of observation duration allowing a direct comparison with other emission phenomena. We speculate that if the abnormal behaviour in PSR J1119-6127 is indeed glitch induced then there might exist a population of neutron stars which only become visible in the radio band for a short duration in the immediate aftermath of glitch activity. These neutron stars will be visible in the radio band as sources that only emit a cluster of pulses once every few years.


Abstract Copyright: 2010 The Authors Monthly Notices of the Royal Astronomical Society2010 RAS

Journal keyword(s): polarization - radiation mechanisms: non-thermal - pulsars: general - pulsars: individual: J1119-6127

Simbad objects: 25

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Number of rows : 25
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 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
3 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
4 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
5 PSR J0627+16 Psr 06 27 13 +16 12.0           ~ 9 0
6 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
7 NAME Vela SNR 08 34.0 -45 50           ~ 1331 2
8 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
9 PSR J1014-5719 Psr 10 15 37.96 -57 19 12.8           ~ 44 0
10 PSR B1046-58 Psr 10 48 13.10000 -58 32 03.0000           ~ 293 0
11 PSR J1105-6107 Psr 11 05 26.1400 -61 07 48.940           ~ 129 0
12 PSR J1119-6127 Psr 11 19 14.30 -61 27 49.5           ~ 439 1
13 SNR G292.2-00.5 SNR 11 19.3 -61 28           ~ 98 1
14 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
15 PSR J1420-6048 Psr 14 20 08.190 -60 48 14.85           ~ 214 0
16 PSR J1623-4950 Psr 16 23.0 -49 50           ~ 2 0
17 SNR G343.1-02.3 SNR 17 08.0 -44 16           ~ 82 1
18 PSR B1706-44 Psr 17 09 42.62000 -44 29 12.0000     13.30     ~ 670 1
19 PSR B1737-30.2 Psr 17 40 33.98000 -30 15 22.0000           ~ 236 0
20 PSR B1800-21 Psr 18 03 51.40000 -21 37 07.0000           ~ 278 1
21 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
22 PSR J1819-1458 Psr 18 19 34.173 -14 58 03.57           ~ 136 0
23 PSR J1846-0258 Psr 18 46 24.75 -02 58 29.6           ~ 388 2
24 PSR J1933+2421 Psr 19 33 37.83 +24 36 39.6           ~ 157 0
25 PSR B2334+61 Psr 23 37 05.779 +61 51 01.69           ~ 206 1

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