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Normalization and second moments of the Gaussian matrix laws

Statement

Assume Countable Choice. The scalar and finite product densities in Standard real and normalized complex Gaussian matrix laws have total mass one. A real entry has mean zero and second moment one; a normalized complex entry has mean zero and E∣z∣2=1. The image of two independent real entries under (x,y)↦(x+iy)/2 has density π−1e−∣z∣2. These facts justify the probability laws in that definition.

Facts & Assumptions

Given: Countable Choice and the displayed density formulas in the Gaussian-law definition, initially regarded simply as functions.

[F2]

For supplied countably additive Borel length measures with these interval volumes, the real density (2π)−1/2e−x2/2 has mass one, absolutely integrable mean zero, and second moment one. Gaussian density integrals for supplied length measures

[F4]

Euclidean Lebesgue measure agrees on Borel sets with the product of its coordinate measures; Tonelli applies to nonnegative product-measurable functions on sigma-finite spaces. On Borel subsets of R^{m+n}, the product lambda_m times lambda_n agrees with lambda_{m+n} Tonelli's theorem for nonnegative measurable functions on a sigma-finite product

[F5]

Increasing nonnegative measurable functions commute with integration. Monotone convergence for the integral

Proof

1.1givenF1F2

Restrict the measures in [F1] to Borel sets in dimensions one and two. They meet exactly the supplied-measure hypotheses of [F2]. With location zero and variance one, [F2] gives real mass one, mean zero, absolute first-moment integrability, and second moment one. No normal-law result assuming full Choice is used.

2.1step 1.1F3F4algebra

The map T(x,y)=(x/2,y/2) has determinant 1/2. By [F3], the image density is 2φR(2u)φR(2v)=π−1e−(u2+v2). The integral transformation follows first for indicator functions from [F3], then for simple functions and their increasing limits. Its mass is one by step 1.1 and [F4]. By the same product integration, E∣z∣2=E(x2+y2)/2=1, and both real and imaginary means vanish; their absolute integrability follows from that of x,y.

3.1step 1.1step 2.1F4F5algebra∎

For any positive finite number of entries, repeated [F4] factors the integral of the nonnegative Borel product density into scalar integrals, each one. All coordinate spaces are sigma-finite, being countable unions of bounded boxes. Integrating over a product of Borel entry sets similarly gives the product of their scalar probabilities, which establishes independence. The integral of the density over sets defines a countably additive probability measure: for disjoint sets, the finite sums of their density-weighted indicators increase to the density times the indicator of their union, so monotone convergence, by [F5], gives countable additivity. For zero entries use the one-point space of mass one and the empty product. Thus all finite laws in the definition are justified using only the stated Countable Choice.

Depends on

Used by

Cited to discharge well-definedness by Standard real and normalized complex Gaussian matrix laws.

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Sources