Write locally, with analytic and . The coefficient of in the Modified Bessel differential equation requires . If , its recurrence is , with . Hence
The analytic part is even: an odd-power term in would produce an uncancelled odd-power term under the same differential operator, and the recurrence removes all such terms. Insert a smooth even cutoff equal to one near zero. The smooth part and the exponentially decaying tails give no algebraic large-wavenumber terms after repeated integration by parts. Therefore the logarithmic singularities determine the requested terms. For ,
Thus the Fourier transform of the modified Bessel function K0 has expansion
An independent check follows from the integral representation of the modified Bessel function of the second kind. Integrating first and then setting gives , with exactly these first two terms.