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Theorem 2.9.669D141CB2664

Theorem 2.9.6.69D141CB2664 Let $\mu $ be a finite positive Borel measure on $\mathbb R^ d$, and let $0<s<d$. Then

\[ I_ s(\mu )=b_{d,s}\int _{\mathbb R^ d}|\widehat\mu (\xi )|^2|\xi |^{s-d}\, \mathrm d\xi , \qquad b_{d,s}=\pi ^{s-d/2}\frac{\Gamma ((d-s)/2)}{\Gamma (s/2)}, \]

where $\Gamma (a)=\int _0^\infty v^{a-1}\mathrm e^{-v}\, \mathrm d v$, $a>0$, is Euler's Gamma function. Both sides may be infinite.

Proof. For $z\in \mathbb R^ d$, the substitution $v=\pi t|z|^2$ gives

\[ |z|^{-s}=\frac{\pi ^{s/2}}{\Gamma (s/2)}\int _0^\infty t^{s/2-1}\mathrm e^{-\pi t|z|^2}\, \mathrm d t, \]

and both sides are $+\infty $ when $z=0$. By lemma 2.9.2 with $t$ replaced by $1/t$, we have $\mathrm e^{-\pi t|z|^2}=t^{-d/2}\int \mathrm e^{-\pi |\xi |^2/t}\mathrm e^{-2\pi \mathrm i z\cdot \xi }\, \mathrm d\xi $. Taking $z=x-y$ and integrating with respect to $\mu \times \mu $, we obtain

\[ \iint \mathrm e^{-\pi t|x-y|^2}\, \mathrm d\mu (x)\, \mathrm d\mu (y) =t^{-d/2}\int \mathrm e^{-\pi |\xi |^2/t}|\widehat\mu (\xi )|^2\, \mathrm d\xi ; \]

Fubini's theorem applies here because the Gaussian in $\xi $ is integrable and $\mu \times \mu $ is finite. Now insert the integral formula for $|x-y|^{-s}$ into $I_ s(\mu )$. All integrands are nonnegative, so Tonelli's theorem allows us to integrate first in $(x,y)$, then use the last identity, and finally integrate in $t$ before $\xi $, even when the integrals are infinite:

\[ I_ s(\mu )=\frac{\pi ^{s/2}}{\Gamma (s/2)}\int |\widehat\mu (\xi )|^2\int _0^\infty t^{(s-d)/2-1}\mathrm e^{-\pi |\xi |^2/t}\, \mathrm d t\, \mathrm d\xi . \]

For $\xi \neq 0$, the substitution $v=\pi |\xi |^2/t$ evaluates the inner integral as

\[ \int _0^\infty t^{(s-d)/2-1}\mathrm e^{-\pi |\xi |^2/t}\, \mathrm d t =\pi ^{(s-d)/2}|\xi |^{s-d}\Gamma ((d-s)/2), \]

and the point $\xi =0$ is a Lebesgue null set. Multiplying the constants gives the formula. $\square$

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