- ... Chandra
- Tables 1-3 are only available in electronic form at http://www.aanda.org
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... CIAO 3.2.2
- http://cxc.harvard.edu/ciao/
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...=2.0 keV)
- http://asc.harvard.edu/ciao/download/doc/expmap_intro.ps
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
PWDetect
- See http://www.astropa.unipa.it/progetti_ricerca/PWDetect
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... XIMAGE
- http://heasarc.nasa.gov/xanadu/ximage/ximage.html
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... scales
- This effect occurred for only 3 sources at large
off-axis angles, where the PSF is particularly elongated and thus
significantly different from the symmetric PSF assumed by PWDetect. Note that,
quite obviously, this effect is also not included in the simulations of
source-free fields.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
convention
- http://cxc.harvard.edu/cdo/scipubs.html
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... XTRACT
- http://www.astro.psu.edu/xray/docs/TARA/ae_users_guide.html
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
TARA
- http://www.astro.psu.edu/xray/docs/TARA/
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
FTOOLS
- http://heasarc.gsfc.nasa.gov/docs/software/ftools/
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
hints
- http://www.astro.psu.edu/xray/docs/TARA/ae_users_guide/node35
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
arcsec
- http://www.astro.msfc.nasa.gov/Ch4/Ch4_15-03_Tsujimoto.pdf
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ...
(PIMMS
- http://heasarc.gsfc.nasa.gov/docs/software/tools/pimms.html
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... (PSC)
- See http://www.ipac.caltech.edu/2mass
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... range
- We only consider COUP sources for which mass estimates are
given by Getman et al. (2005a).
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... difference
- A direct comparison
with the results of Hillenbrand (2005) is however not possible because
her estimate of disk lifetime (i) refers to star in the
,
i.e.
less massive than the ones we observe in Cygnus OB2, (ii) is based on a
different, and more efficient, indicator of disks presence than the one we can
use here, i.e. the H-K color excess measured with respect to the photospheric
value as determined from spectral types.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... diagram
- The use of the J-band is justified because (i) in
the presence of disk excesses the J-band is the most representative of the
photospheric emission and (ii) the mass ranges in which the mass-luminosity
relationship is degenerate are narrower than for a similar relationship in the
H and K bands.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... stars
- There are
only 28 stars with masses in the
range and for which this
interval formally corresponds to the uncertainty on the mass estimate. We
therefore expect a small fraction of the 57 intermediate mass stars to lie in
the
range and to have a substantial model-predicted convective
envelope.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... types
- A number of X-ray detected
stars with no spectral type appear to be of high mass but with lower X-ray
luminosities than those with spectral types. In the discussion of
high mass stars, however, we will only consider stars with spectral types.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... 9
- One undetected B stars has an unknown
luminosity class.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... spectrum
- The temperatures reached by hydrodynamic shocks
in the winds of single stars are usually not high enough to produce significant
Fe K
emission. In wide early-type binary systems, however, stellar
winds collide with velocities close to
and are thus heated to
sufficiently high temperatures. In such cases, the cooler surrounding wind
material, excited by the high energy radiation, can produce the 6.4 keV
fluorescent Fe line. The observation of the Fe-complex can thus be a used as
diagnostic for colliding-wind binaries (Raassen et al. 2003).
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.