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Astron. Astrophys. 349, L49-L52 (1999)
4. X-rays from the Sgr A Complex
The location of SgrA* was imaged on August 24-26, 1997 for a net
exposure time of 99.5 ks. In order to study the surface brightness and
temperature profile of the diffuse emission, we extracted the MECS
counts from four annular regions with different inner and outer radii
( , , , )
centered on SgrA*. All these spectra contain several emission lines,
with the K-lines from iron
(E keV) and sulfur
(E keV) particularly bright. We
fitted them with a single temperature plasma model (MEKAL in XSPEC
v.10.00), deriving the surface brigthness and temperature profiles
shown in Fig. 2. A radial spectral variation is evident: while the
keV temperature in the three
external regions is almost constant, the emission from the inner
is significantly softer. This is
probably due to the presence, in addition to the diffuse emission, of
further contributions from the bright point sources present near the
GC (Maeda et al. 1996, Predehl & Trümper 1994, Sidoli et al.
1999b).
![[FIGURE]](img33.gif) |
Fig. 2. Surface brightness and temperature in concentric regions around the GC.
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The fit with a single temperature thermal model does not account
for all the emission lines at low energies (in particular the intense
emission from sulfur at E 2.4 keV), nor
for an excess around 6.4 keV, due to the presence of emission of
fluorescent origin. A gaussian line added at 6.4 keV accounts for
these residuals. While this line is present in all the spectra
extracted from to
, it seems to be absent within
(EW 12 eV). This is consistent with
the 6.4 keV map produced with ASCA (Maeda & Koyama 1996) where a
strong peak is visible in the region of the Radio Arc, NE to the GC.
Indeed the EW of this line increases towards the outer regions
( eV, eV,
eV). The MECS spectra extracted from
two semi-annular regions at NE and SW of the GC, confirm this
interpretation: the EWs of the 6.4 keV line are
eV (NE sector; errors are at 90%
confidence level) and eV (SW
sector).
Since the temperature profile does not show evidence of strong
spectral variations in the region from
to
, we analysed the overall spectrum by
extracting all the counts from this larger circular corona. We started
by fitting a thermal bremsstrahlung plus three gaussian lines at
1.8, 2.4 and 6.7 keV (Si, S and Fe
respectively). Their estimated equivalent widths are about 120, 190
and 1000 eV. The best fit value for the bremsstrahlung temperature is
13 keV. This temperature is too high
to be consistent with the presence of the low energy emission lines
(Kaneda et al. 1997, Fig. 2b). A possible explanation is a
multi-temperature plasma. Thus we fitted the spectrum with two thermal
emission plasma models (two "MEKAL" in XSPEC). Our best fit parameters
( =1.29, 368 d.o.f) are
NH= cm-2,
keV and
keV. A gaussian added at
6.4 keV gives an EW 120 eV. The
total unabsorbed flux (2-10 keV) is
ergs cm-
2 s-1, about one third of which is contributed
by the soft component.
To study the spatial distribution of the diffuse emission, we
extracted images in different energy bands (Fig. 3). The images
corresponding to the 2-5 keV and 7-10 keV ranges show significantly
different distributions of the diffuse emission.
![[FIGURE]](img46.gif) |
Fig. 3. 2-5 keV (left) and 5-10 keV (right) emission from the SgrA Complex. Both images have been smoothed with a gaussian with FWHM=1 arcmin. The strong source in the NE corner is 1E1743.1-2843 (Cremonesi et al. 1999). The low surface brightness in correspondence of the circle is an instrumental effect due to the absorption in the detector window support structure.
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Both the soft and hard emissions are peaked at the GC position, but
they have different spatial extents. In particular, the softer
emission has a nearly triangular shape, with a rather sharp decrease
in the south-western side, which is absent in the hard X-ray map. To
study the spatial distribution of the iron line we have also extracted
an image in the 5.5-7.5 keV band and subtracted from this map the
continuum emission interpolated from the contiguous energies. The
resulting iron line image shows a spatial distribution elongated along
the galactic plane, very similar to that of the hard X-ray map.
© European Southern Observatory (ESO) 1999
Online publication: September 2, 1999
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