For every real , define . The apparent endpoint singularity at is removable, with limit , and the bound ensures integrability. Differentiation under the integral sign is justified by the integrable bound on the parameter derivative. Thus
where and the last integral is a Laplace transform. Since , integrating with respect to gives . This obtains an integral with a logarithmic denominator by differentiating away that denominator, then restoring the parameter dependence with one elementary antiderivative.

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