An example of determining the conditions of existence of the various integrals. Existence of the integrals depends upon the behavior of the singularities appearing at the edges of the region of integration.
Consider the single pair overlap integral
, where
are as in the definitions for theorem 14a, with the minor change that
contains all m indices, which may be made without loss of generality. It will be shows that the conditions for existence of this integral are
,
,
and
. Write the integral as
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That
,
, follows immediately from the fact that
exists iff
and the fact that any
may independently be near zero for this particular overlap case. Now, either
or
may also be near zero. We consider the first case, in which
is near zero, and use symmetry to supply the result for the second case. Letting
and
, rewrite equation 9.137 in a form that isolates
as

Each of the three integrals over
in equation 9.138 may be done in closed form. Do these integrals using theorem 9a and induction to find

Apply the binomial theorem in equation 9.139 to expand two of the three factors in the integrand,
and
, in series. Using these series, note that each term in the series for
will contribute the same power of x after the integration over y, while the terms of the series for
contribute increasing powers of x after the integration over y. Note also that if the lowest-power-of-x term is integrable over x in a region containing 0, then all of the terms are. Thus, the worst case occurs with the constant term from the binomial series for
. After integration over y with this constant term, and considering the small x region of integration, we are left with the integral over x given by
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where
, and C is a constant. This integral exists for
. This, symmetry, and the first condition (given by
,
) establish the result. The method for more complicated overlap structures is also indicated by this discussion.
The discussion above is of interest in another way: it provides a general method for finding multiple overlap integrals without the use of transform theory.