2013MNRAS.429.2493C


Query : 2013MNRAS.429.2493C

2013MNRAS.429.2493C - Mon. Not. R. Astron. Soc., 429, 2493-2499 (2013/March-1)

The extended X-ray emission around RRAT J1819-1458.

CAMERO-ARRANZ A., REA N., BUCCIANTINI N., McLAUGHLIN M.A., SLANE P., GAENSLER B.M., TORRES D.F., STELLA L., DE ONA E., ISRAEL G.L., CAMILO F. and POSSENTI A.

Abstract (from CDS):

We present new imaging and spectral analysis of the recently discovered extended X-ray emission around the high magnetic field rotating radio transient RRAT J1819-1458. We used two Chandra observations performed for this object in 2008 May 31 and 2011 May 28, respectively. The diffuse X-ray emission was detected with a significance of ∼ 19σ in the image obtained by combining the two observations. Neither long-term spectral nor timing variability has been observed from the source or the nebula. RRAT J1819-1458 shows an unusual high X-ray efficiency of η_X ≡L_X(0.3-5 keV)/\skew4{dot}E_rot ∼0.15 at converting spin-down power into X-ray luminosity. The most favourable scenario for the origin of this extended X-ray emission is either a pulsar wind nebula or a scattering halo. A magnetically powered scenario for the extended emission is viable only in the case of a Compton nebula, while it can be tentatively disfavoured in the case of synchrotron emission.

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

Journal keyword(s): stars: magnetic field - stars: neutron - pulsars: individual: RRAT J1819-1458 - X-rays: stars

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 J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 463 1
2 2MASS J18193233-1457584 * 18 19 32.3415727968 -14 57 58.513705272           ~ 1 0
3 PSR J1819-1458 Psr 18 19 34.173 -14 58 03.57           ~ 136 0
4 2MASS J18193491-1457472 EB* 18 19 34.9158166704 -14 57 47.735514540           ~ 2 0
5 PSR J1834-0845 Psr 18 34 52.1 -08 45 56           ~ 98 0

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