S. Garciaburillo et M. Guelin, THE DISTORTED KINEMATICS OF MOLECULAR GAS IN THE CENTER OF NGC-891, Astronomy and astrophysics, 299(3), 1995, pp. 657-670
The center of the edge-on spiral galaxy NGC 891 has been mapped in the
J=2-1 and J=1-0 transitions of (CO)-C-12 using the IRAM 30m telescope
, with spatial resolutions of 13'' and 21'' respectively. The kinemati
cs of molecular gas in the inner regions of the galaxy is particularly
distorted. The position-velocity diagram (p-v) taken along the kinema
tical major axis of NGC 891 is strikingly similar to the Galaxy's long
itude-velocity plot (I-v). As in our Galaxy, we have detected in NGC 8
91 molecular gas circulating at velocities 'forbidden' by a law based
only on circular rotation. Following the work of Binney et al. (1991)
on the interpretation of our Galaxy's CO I-v diagram, we have develope
d a model on the gas kinematics of the inner regions of NGC 891 that e
xplains satisfactorily the major features of the CO p-v diagram. In ou
r model, the flow of molecular gas is driven by a bar that has corotat
ion at r similar to 3 kpc and that is viewed at an angle alpha similar
to 45 degrees from its major axis. Molecular clouds circulate along x
(2) orbits (elliptical orbits perpendicular to the bar) between the tw
o Inner Linblad Resonances (ILR), and partly populate x(1) orbits (ell
ipses parallel to the bar) in the outer regions (from the outer ILR up
to the corotation circle). We can also explain the radial distributio
n of molecular gas: the great ring of molecular material at r similar
to 4.5-6 kpc might be associated with the Outer Linblad Resonance of t
he bar (OLR) and the adjacent hole of molecular gas inside this radius
, with the corotation circle. The observed kinematics of molecular gas
in the center of the edge-on spiral NGC 5907, as well as a number of
other galaxies, could be also interpreted in terms of highly elliptica
l orbits driven by bars or triaxial potentials.