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Astron. Astrophys. 333, 583-590 (1998)
3. Galactic distribution, extinction
To extrapolate from a local X/O nova rate to a galactic population
of low mass BHB systems, one needs a distribution model. Here it is
assumed the black holes are distributed similarly to other high mass
star products at birth, namely the Galactic neutron stars. To minimize
the extrapolation to the Galactic center, the BH systems are
distributed according to the model of Johnston (1994) for the pulsar
Galactic surface density
![[EQUATION]](img64.gif)
![[EQUATION]](img65.gif)
with kpc and kpc,
which provides a good fit to the observed pulsar distribution, and
avoids a large excess inside the kpc molecular
gas ring. The thickness z of this disk is modeled as a Gaussian
distribution with pc. This model follows recent
high mass star formation; it might be argued that this under-counts
old systems produced by the bulge. For example, in Sect. 6 the
classical novae are considered, which have a significant bulge
population. These are observed to follow the distribution of light in
external galaxies, so Shafter (1997) models the Galactic population
as
![[EQUATION]](img70.gif)
![[EQUATION]](img71.gif)
The scale heights of these populations are 100pc and 200pc
respectively (Warner 1995) and, following the surface brightness
distribution, 12% of the systems are found in the bulge.
The observed low mass BHB transients are discovered in X-rays, but
confirmed via radial velocity studies in the optical. The quiescent
counterparts are generally very faint, and optical extinction is a
serious impediment to their study (Table 1). Extinction will, of
course affect their outburst magnitudes and can be a very significant
limit on detectability, even for systems with
kpc. To follow the distribution of optical extinction with l, b
and d in the Solar neighborhood, one may use the compilation of
Galactic reddening from stellar observations described in Guarinos
(1992). From this compilation of 15,500
measurements one may extract stars close to any given
and follow the increase of
with d to model the local extinction. In
practice, regions of radius were used along the
Galactic plane, and the top tercile of in each
distance bin was selected to minimize bias against rare high
lines of sight. These data allowed estimates
out to kpc in the plane. When
were needed at larger d than covered by
the data for a given line of sight, an exponential dust disk of height
100pc and mean extinction in the plane of
mag/kpc was assumed (cf. Burton and Deul 1987). There are, of course,
long interarm regions that are relatively dust free in the galaxy. To
model this 10% of the nominal disk's dust density was assigned
randomly to 0.2 of the lines of sight beyond the local 2-3 kpc. This
turned out to have a very small effect on the BHB statistics. This
extinction model was checked against a number of measured extinctions,
giving adequate estimates. While rare lines of sight through very
large molecular clouds are not followed, the
results should be reasonable for modeling of the nearby outburst
sample.
© European Southern Observatory (ESO) 1998
Online publication: April 20, 1998
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