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Astron. Astrophys. 332, 55-70 (1998)
7. Summary
We analyzed the keV and
keV ROSAT all-sky-survey data and
evaluated the photoelectric absorption of the neutral matter traced by
H I gas as given by the Leiden/Dwingeloo survey.
The main results are:
- At high latitudes near
the temperature
of the distant X-ray MK plasma is kT = 0.13-0.14 keV
(Sect. 3.2), a value in agreement with other published X-ray
temperatures obtained towards different directions of the galactic
sky. Hence, we found that the thermal X-ray component is, in a first
approximation, isothermal.
- The photoelectric-absorption-corrected
keV
count rate decreases with increasing latitude and towards the galactic
anticenter, (Sect. 3.5), indicating that a significant fraction
of the galactic keV emission originates in the
halo.
- We modelled an isothermal flattened X-ray halo based on
hydrostatic equilibrium considerations (Sect. 4.1). An X-ray halo
component with a scale height of
and a radial
scale length of in addition to an
extragalactic power-law ( ) component - both
absorbed by galactic neutral matter - can reproduce the
keV RASS data down to its data accuracy limit
(Sect. 4.2).
- The RASS
keV large-scale intensity
distribution is consistent with this X-ray plasma halo model
(Sect. 6).
(Since our analysis is restricted to latitudes above
and to directions away from the galactic
bulge, we note that our results are largely restricted to information
contributed from a volume within about 4 kpc from the Sun.)
Finally, assuming that the X-ray halo model is valid for the entire
Galaxy, we obtain a total halo X-ray luminosity of
. This value is comparable to luminosities
found for the X-ray halos of M51 and NGC1566 by Ehle (1996). This may
be an indication of a common X-ray halo-producing mechanism, as for
example a galactic fountain by stellar activity (e.g. Bregman 1980),
where hot material is transported up and radially outward, reproducing
the X-ray parameters determined.
© European Southern Observatory (ESO) 1998
Online publication: March 10, 1998
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