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Laplace noise has its stated Lebesgue density

Statement

Assume Countable Choice. For every b>0, the probability measure Lap⁡(b) is absolutely continuous with respect to Lebesgue measure on R and has density

z⟼12be−∣z∣/b.

Facts & Assumptions

Given: b>0 and a Borel set A⊆R.

[A1]

Countable Choice is the axiom assumed by the cited exponential-law and Lebesgue change-of-variables suppliers; no full Axiom of Choice is invoked.

[F1]

Laplace distribution: Lap⁡(b)(A)=12μb(A∩(0,+∞))+12μb({x>0:−x∈A}), where μb is the exponential probability law of rate 1/b.

[F2]

Exponential-law density: for λ>0, the density is fλ(t)=λe−λt when t>0 and 0 otherwise, and it defines a probability law.

[F3]

Lebesgue change of variables: a C1 diffeomorphism T transforms nonnegative Lebesgue integrals by the absolute Jacobian; for T(x)=−x the absolute Jacobian is 1.

[F4]

Measure of a degenerate interval: a one-dimensional box with equal endpoints has Lebesgue measure 0.

Proof

1.1A1F1F2F3F4givenconstructalgebra

Put A+=A∩(0,+∞) and A−=A∩(−∞,0). By [F1] and [F2], the positive mixture half contributes 12∫A+b−1e−x/b dλ(x). Applying [F3] to reflection T(x)=−x and y↦1A−(y)b−1ey/b shows that the reflected half contributes 12∫A−b−1ey/b dλ(y). On A+, e−x/b=e−∣x∣/b; on A−, ey/b=e−∣y∣/b. The singleton at zero has Lebesgue measure zero by [F4]. Hence Lap⁡(b)(A)=∫A(2b)−1e−∣z∣/b dλ(z).

2.1step 1.1givenalgebra∎

The identity in step 1.1 holds for every Borel set A. Its integrand is nonnegative and measurable; thus every Lebesgue-null Borel set has zero Lap⁡(b) measure, and the displayed function is the claimed Radon–Nikodym density.

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Sources