Linear factorization relations are derived for the matrix elements of quantum mechanical operators defined on some space ℋ = ℋ1⊕⋅2 which are diagonalizable on ℋ1. The coefficients in these relationships do not depend on the operators perse but do depend on the representations in which the operators are diagonal. The formulation is very general with regard to the nature of the ’’input’’ information in the factorization. With each choice of input information there are associated consistency conditions. The consistency conditions, in turn, give rise to a flexibility in the form of the factorization relations. These relations are examined in detail for the operators of scattering theory which are local in the internal molecular coordinates. In particular, this includes S and T matrices in the energy sudden (ES) approximation. A similar development is given for the square of the magnitude of operator matrix elements appropriately averaged over ’’symmetry classes.’’ In the ES these relations apply to transition cross sections between symmetry classes. In particular, they apply to degeneracy averaged cross sections in situations where the symmetry classes correspond to energy levels.

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In the terminology of De Pristo et al.,6 the factorization relations presented here between like quantities are called scaling relations.
9.
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10.
A WKB estimate shows that since the potential goes to infinity as the atoms of the molecule separate (the system is nonreactive), the dominant asymptotic behavior is state Independent and has a “faster than exponential” decay.9
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13.
Since φlμ satisfies a Sturm‐Liouville problem, the interior zeros must be simple. Alternatively, we may regard such points as hypersurfaces on which the function and its derivatives can not all be zero from the Cauchy—Kowalewski theorem since φlμ±0 (assuming local analyticity).
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