is replaced by a constant diagonal matrix
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
At present the Hibridon code contains no provision for the determination of differential cross sections with the CS approximation.