2012ApJ...761..117P


Query : 2012ApJ...761..117P

2012ApJ...761..117P - Astrophys. J., 761, 117 (2012/December-3)

XMM-Newton observation of the very old pulsar J0108-1431.

POSSELT B., ARUMUGASAMY P., PAVLOV G.G., MANCHESTER R.N., SHANNON R.M. and KARGALTSEV O.

Abstract (from CDS):

We report on an X-ray observation of the 166 Myr old radio pulsar J0108-1431 with XMM-Newton. The X-ray spectrum can be described by a power-law model with a relatively steep photon index Γ ~ 3 or by a combination of thermal and non-thermal components, e.g., a power-law component with fixed photon index Γ = 2 plus a blackbody component with a temperature of kT = 0.11 keV. The two-component model appears more reasonable considering different estimates for the hydrogen column density NH. The non-thermal X-ray efficiency in the single power-law model is ηPL1–10keV = LPL1–10keV/{dot}E ∼ 0.003, higher than in most other X-ray-detected pulsars. In the case of the combined model, the non-thermal and thermal X-ray efficiencies are even higher, ηPL1–10keV ∼ ηbbPC ∼ 0.006. We detected X-ray pulsations at the radio period of P ~ 0.808 s with significance of ~7σ. The pulse shape in the folded X-ray light curve (0.15-2 keV) is asymmetric, with statistically significant contributions from up to five leading harmonics. Pulse profiles at two different energy ranges differ slightly: the profile is asymmetric at low energies, 0.15-1 keV, while at higher energies, 1-2 keV, it has a nearly sinusoidal shape. The radio pulse peak leads the 0.15-2 keV X-ray pulse peak by φ = 0.06±0.03.

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Journal keyword(s): pulsars: individual: PSR J0108-1431 - stars: neutron - X-rays: stars

Simbad objects: 16

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Number of rows : 16
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 J0108-1431 Psr 01 08 08.29 -14 31 48.5           ~ 113 0
2 PSR J0538+2813 Psr 05 38 25.06 +28 17 11.0           ~ 224 1
3 PSR B0628-28 Psr 06 30 49.35000 -28 34 42.1000           ~ 313 1
4 PSR J0633+1746 Psr 06 33 54.153 +17 46 12.91           ~ 1308 0
5 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
6 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 541 1
7 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
8 PSR B0943+10 Psr 09 46 07.31 +09 51 57.3           ~ 364 1
9 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
10 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
11 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
12 PSR B1451-68 Psr 14 56 00.0175876848 -68 43 40.034742348           ~ 203 0
13 PSR B1813-36 Psr 18 17 05.8883476416 -36 18 04.776876972           ~ 62 0
14 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
15 PSR J2144-3939 Psr 21 44 12.01000 -39 33 58.4000           ~ 145 0
16 PSR B2223+65 Psr 22 25 52.8627 +65 35 36.371           ~ 342 0

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