Bourbaki

Lemma 1

Tag 09SB, permanent. Cite it as [Bourbaki, Tag 09SB].

Integration, IX, p. 77, § 6. Promeasures and measures on a locally convex space

For every integer n⩾0n \geqslant 0,

∫R∣x∣ne−x2/2dx=2n+12Γ(n+12) \int_{\mathbf{R}} |x|^n e^{-x^2/2} dx = 2^{n+1 \over 2} \Gamma \left( {n+1 \over 2} \right)
(6)

∫Rx2ne−x2/2dx=(2π)1/2(2n)!2nn! \int_{\mathbf{R}} x^{2n} e^{-x^2/2} dx = (2\pi)^{1/2} \frac{(2n)!}{2^n n!}
(7)

∫Rx2n+1e−x2/2dx=0. \int_{\mathbf{R}} x^{2n+1} e^{-x^2/2} dx = 0.
(8)

Recall the formula

Γ(s)=∫0∞us−1e−udu \Gamma(s) = \int_0^\infty u^{s-1} e^{-u} du
(9)

valid for every real number s>0s > 0 (FRV, VII, §1, No. 3, Prop. 3). On making the change of variable x=(2u)1/2x = (2u)^{1/2}, it follows from (9) that

∫0∞xne−x2/2dx=∫0∞(2u)n/2e−u1221/2u−1/2du=2n−12Γ(n+12), \int_0^\infty x^n e^{-x^2/2} dx = \int_0^\infty (2u)^{n/2} e^{-u} {1 \over 2} 2^{1/2} u^{-1/2} du = 2^{n-1 \over 2} \Gamma \left( {n+1 \over 2} \right),

whence the formula (6) since

∫R∣x∣ne−x2/2dx=2∫0∞xne−x2/2dx. \int_{\mathbf{R}} |x|^n e^{-x^2/2} dx = 2 \int_0^\infty x^n e^{-x^2/2} dx.

The formula (7) follows from (6) and the relation

Γ(n+12)=π1/2(2n)!22nn!. \Gamma \left( n + \frac{1}{2} \right) = \pi^{1/2} \frac{(2n)!}{2^{2n} n!}.
(10)

For n=0n = 0, this relation reduces to Γ(12)=π1/2\Gamma(\frac{1}{2}) = \pi^{1/2}, that is, to the formula (21) of FRV, VII, §1, No. 3. The general case then follows by induction on nn, on taking into account the relation Γ(x+1)=x⋅Γ(x)\Gamma(x+1) = x \cdot \Gamma(x) (loc. cit., §1, No. 1).

Finally, the formula (8) follows from the fact that the function x↦x2n+1e−x2/2x \mapsto x^{2n+1} e^{-x^2/2} is odd.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

Cited by

Cites

  • FRV, VII, §1, No. 3 not yet on this site: FVR VII
  • FRV, VII, §1, No. 3, Prop. 3 not yet on this site: FVR VII
  • §1, No. 1
Transcribed from the printed volume. Not translated.