Chapter 6

Gaussian Integrals

This chapter deals with properties of exponential functions which are density functions for the distribution functions of important classes of observables. (Density function is a point function for which the distribution function is the Riemann-complete indefinite integral.)

6.1   Fresnel’s Integral

The integrals

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are well known in their familiar notation,

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The latter integrals exist as improper or extended Riemann integrals. The familiar proof of the first one runs as follows.

Lemma 10

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Proof. Let ρ > 0 and let

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By Theorem 46 (integration by substitution), the Riemann integral

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can be evaluated using polar co-ordinates (r, θ):

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Letting ρ → ∞,

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For λ = 1,2,3,… let Jλ = [−λ, λ] × [−λ, λ]. Then

If equation (6.2) is correct, it implies that βλ converges as λ → ∞, ...

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