Swift/XRT localization of SLX 1746-331
ATel #1237; J. A. Kennea (PSU), D. Steeghs (Warwick/CfA), M. A.P. Torres (CfA), J. Homan (MIT) and J. M. Miller (Michigan)
on 12 Oct 2007; 21:18 UT
Distributed as an Instant Email Notice Transients
Credential Certification: Jamie A. Kennea (kennea@astro.psu.edu)
Subjects: X-ray, Black Hole, Transient
We report on a target of opportunity observation of SLX 1746-331 taken by
Swift/XRT on Oct 12th, 2007 at 15:13UTÂ for 2ks. SLX 1746-331 is a black
hole candidate and recurrent transient source which has recently been reported
to have returned to an active state (Markwardt & Swank 2007, ATEL #1235).
Photon Counting mode data was taken to ensure that an accurate localization of
this transient could be found. Analysis of XRT data reveals a very bright point
source at the following coordinates:
RA(J2000) = 17h 49m 49.0s,
Dec(J2000) = -33d 12m 14.9s,
with an estimated uncertainty of 4 arcseconds radius (90% confidence). This
position lies 29 arcseconds away from the initial position of this source
reported by Skinner et al (1990, MNRAS, 243, 72), inside of their reported 35
arcsecond error radius and lies 7.2 arcseconds from the ROSAT survey source 1RXS
J174948.4−331215, which has an 8 arcsecond error circle. We therefore conclude
that the bright source we detect is SLX 1746-331 in outburst and, as suggested
by Motch et al (1996, AASS, 132, 341), 1RXS J174948.4−331215 is SLX 1746-331.
We note that the XRT error circle contains two 2MASS point sources, 2MASS
17494887-3312152 and 2MASS 17494929-3312123 2.5 and 3.4 arcseconds from the XRT
position respectively, however the crowded nature of this field means that
infrared/optical identification of the source will require follow-up
observations.
Due to the source brightness, the PC mode data is highly piled up making
spectral analysis difficult. However by fitting the PSF wings we find the
following spectral parameters utilizing a thermal bremsstrahlung model: kT = 3.4
+/- 0.2 keV, NH = (1.0 +/- 0.1) x 1022 cm-2. We
note that this spectral fit is considerably harder than the kT=1.5 keV
temperature reported by Skinner et al. (1990). A bremsstrahlung model is favored
for these data compared to a power-law model (reduced Chi^2 = 1.0 and 1.7 for
the thermal and power-law models respectively with 76 degrees of freedom). A
disk blackbody model is also a good fit to the spectrum with Tin =
1.26 +/- 0.04 keV and NH = (0.71 +/- 0.04) x 1022
cm-2 (reduced Chi^2 = 0.95 for 76 degrees of freedom), supporting the
idea that this source is most likely a black hole transient. We note that with
the disk blackbody model, the NH value is approximately double the
expected Galactic absorption of 3.9 x 1021 cm-2. Fixing
the absorption to the expected galactic value results in a poor spectral
fit.
The XRT measured flux of this source is 5 x 10-9 erg/s/cm2
(1-10 keV), uncorrected for absorption, although we note that this value most
likely has a large uncertainty due to the high degree of pile up in the XRT
data.