The previous discovery of an X-ray halo around the edge-on galaxy NGC
891 prompted this effort to better understand the structure of the hot
halo by deep observations with the X-ray satellite telescopes ROSAT a
nd ASCA. The ROSAT HRI image (FWHM of 5'') reveals four point sources
in the disk and one in the halo that was confused with diffuse emissio
n in the previous ROSAT PSPC image. At 5'' angular resolution, the hal
o emission remains diffuse, rather than becoming an ensemble of filame
nts and point sources. There is an indication of X-ray absorption in t
he midplane on the same angular scale as the optical extinction by dus
t (a width of 10''-20''). The PSPC observations (FWHM of 25''-30'') sh
ow that the diffuse emission along the disk closely follows the tracer
s of star formation, such as CO line and 1.3 mm continuum observations
. This would be expected if massive stars led to the production of hot
gas, such as through supernovae. The maximum vertical extent of the h
ot gas, approximate to 2', is similar to that of optical emission line
gas, except the X-ray scale height is much larger. The halo gas densi
ty can be fit with the functional form n(e)(x, z) = n(o) exp (-x/h) ex
p (-z(2)/l(2)), where n(0) = 0.026 cm(-3), the radial length scale h =
85'' (4.1 kpc), and the vertical scale height l = 72'.4 (3.5 kpc). Th
e mean temperature of the gaseous component is 3.5 x 10(6) K, so for a
filing factor of unity, the characteristic pressure is p/k similar to
10(5) K cm(-3), comparable to that of the molecular gas in the disk.
The total gas mass is 4.0 x 10(7) M-circle dot, the bolometric X-ray l
uminosity is 3.9 x 10(39) ergs s(-1), and the mass cooling rate is 0.0
87 M-circle dot yr(-1).