Use integration by substitution with and the Gaussian being an even function:
The factor two from the differential exactly cancels the half-line factor in the given full-line Gaussian integral.
Retain the original PDF's full-line integration limits. For , write . Integration by parts gives
Gaussian decay dominates every power, so the endpoint term vanishes, so
This is the full-line Gaussian moment recurrence; its initial values differ from the half-line version.
The integrand for is an odd function with absolute convergence, so . For , the recurrence gives , where the supplied Gaussian integral is . Hence
The zero first moment is specific to the symmetric full-line domain.
Use integration by substitution with the reciprocal variable , so and . The endpoints become . Thus
Renaming the dummy integration variable proves the identity without evaluating either side.
The integral converges absolutely: near zero it behaves like , and at infinity like . Let its value be . The integration by substitution gives
Therefore
Absolute convergence makes this cancellation between the two ends legitimate.
The tangent half-angle substitution gives and . The endpoints become zero and one, so
Use completing the square, , and integrate:
Thus both integrals equal .

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