Sgr A*, the stationary, compact, nonthermal radio source
at the Galactic Centre (GC), appears to be coincident
with a
point-like object
(Eckart & Genzel 1996, 1997; Ghez et al. 1998; Backer & Sramek 1999; Genzel et al. 2000; Ghez et al. 2000).
It is probable that Sgr A* is associated with the accretion
of matter onto a supermassive blackhole
(for a recent review of the evidence, see Genzel & Eckart 1999).
Models for the accretion process itself vary widely,
including simplistic spherical accretion (Coker & Melia 2000; Coker & Markoff 2001),
an advective flow (Narayan et al. 1995), a convective flow (Stone et al. 1999),
a compact jet (Falcke & Markoff 2000), and a truncated power-law electron
distribution (Beckert & Duschl 1997). The true picture is
probably some combination of these various models.
Deep in the potential well of
Sgr A* and pervading the central parsec of the Milky Way,
there exists a cluster of a few dozen
early-type stars (Sellgren et al. 1990; Genzel et al. 1996),
which is dominated by the IRS 16 assemblage of probable Wolf-Rayet
(WR) stars (Najarro et al. 1997).
Numerous observations and models
(Hall et al. 1982; Allen et al. 1990; Geballe et al. 1991; Yusef-Zadeh & Melia 1992; Najarro et al. 1997; Hanson et al. 1998; Paumard et al. 2001)
provide evidence that this cluster
is producing a composite hypersonic wind of
yr-1.
Some fraction
of
will be trapped by the supermassive blackhole
located near
the middle of the stellar cluster. However, all of the above
models for Sgr A* require a mass accretion rate that is orders of magnitude less
than
.
If any of these models are correct, then for
the lifetime of the early-type cluster's winds and in the
absence of any observed large-scale outflow from Sgr A*,
some part of the cluster's winds
has been accumulating in the central parsec without being accreted by the blackhole.
It is the purpose of this letter to
investigate this gas in the light of recent X-ray observations of the GC.
Copyright ESO 2001