- ... band
- All the count rates
listed here and hereafter have already been corrected for
the enclosed energy fraction and the vignetting.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... observations
- This source was not
discussed in Soria & Kong (2002) because in that paper
we focussed only on transient sources newly detected by XMM
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... AGN
- Two
candidate "ultra-luminous'' sources in the field of nearby galaxies
have recently been recognised as background AGN
(Masetti et al. 2003; Foschini et al. 2002). The possibility that
CXOU J13651.1+154547 is a background object was discussed
by Krauss et al. (2003), but considered unlikely
in the absence of any radio or optical counterpart.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... bmc
- The bmc model (Shrader & Titarchuk 1999)
describes the thermal or bulk motion
Comptonization of a blackbody seed-photon component.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... comptt
- Comptt (Titarchuk 1994)
approximates the seed-photon input spectrum
with the Wien tail of the blackbody spectrum. Thus, it is simpler but less
accurate than the bmc model.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... detector
- The conversion
between the XMM-Newton and Chandra count rates in the three bands
depends of course on the assumed spectral model and absorption,
but these variations are small for the range of column densities
and temperatures considered in Table 2. We converted the colours
using the correct response matrices generated by the CIAO
and SAS software, rather than the default
(pre-launch) responses from PIMMS.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... 1252
- The GCN archive is at
http://gcn.gsfc.nasa.gov/gcn3_archive.html.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.