is replaced by a constant diagonal matrix
(
+ 1) ,
(2)
where
(designated L-bar) is some average orbital angular momentum, then the
CC equations become block-diagonal in the index
which is the body-frame
projection of J. Equivalently, the block diagonalization can
be achieved by neglecting all Coriolis coupling in a body-frame expansion of the
total scattering wavefunction, and, in addition, approximating the diagonal
terms in the body-frame expansion of the orbital angular momentum
Because the computer time required for solution of the CC equations scales as Nch3, this block diagonalization leads to a substantial reduction in the total time required in a scattering calculation. Moreover, for problems in which the potential is not long-ranged, many tests have shown the the CS approximation is remarkably accurate.
where
ki is the wavevector of the initial state and the sum
runs over:

all values of the projection quantum number
such that
| .le. min { Ji, Jf }
and
. Since the S matrix
is independent of the sign of
, the summation in Eq. (3)
can be further restricted to positive, definite values of

At present the Hibridon code contains no provision for the determination of differential cross sections with the CS approximation.