  The accretion of hot slowly rotating gas onto a supermassive black hole is
considered. Rotation velocities at the Bondi radius r_B are small in comparison
with speed of sound c_s. The centrifugal barrier at a depth r_c = l^2/G M_BH <<
r_B hinders supersonic accretion. We take into account saturated electron
thermal conductivity and Bremsstrahlung energy losses of two temperature plasma
for density and temperature near the Bondi radius similar to those observed in
M87 galaxy. Joint action of electron thermal conductivity and free-free
radiation leads to the effective cooling of accreting plasma and formation of
the subsonic settling of accreting gas above the zone of a centrifugal barrier.
A toroidal condensation and a hollow funnel that separates the torus from the
black hole emerge near the barrier. The barrier divides the flow into two
regions: (1) the settling zone with slow subKeplerian rotation and (2) the zone
with rapid supersonic nearly Keplerian rotation. Existence of the centrifugal
barrier leads to significant decrease of the accretion rate dM/dt in comparison
with the critical Bondi solution for gamma=5/3. Shear instabilities in the
torus and related friction cause the gas to spread slowly in the equatorial
plane in two directions. As a result, outer (r>r_c) and inner (r<r_c) disks are
formed. The gas enters the zone of the internal ADAF flow along the accretion
disk (r<r_c). Since the angular momentum is conserved, the outer disk removes
outward an excess of angular momentum along with part of the matter falling
into the torus. Such outer Keplerian disk was observed by Hubble Space
Telescope around the nucleus of the M87 galaxy in the optical emission lines.
Turbulence causes rotation. We discuss the characteristic times during which
the turbulence should lead to the changes in the orientation of the torus,
accretion disk and, possibly, of the jet.
