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Product-coordinate projections commute and contract in L2

Statement

For the product-coordinate averages of Product-coordinate averaging operators, each PJ is a well-defined self-adjoint contraction on real L2(μ), PJ2=PJ, and for all J,K⊆[d], PJPK=PJ∩K as operators on L2(μ).

Facts & Assumptions

Given: A finite product of probability spaces, f,g∈L2(μ), and subsets J,K⊆[d].

[F1]

Product-coordinate averaging operators: PJf is obtained by integrating f over the complementary coordinates, with zero assigned on exceptional sections.

[F2]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: Tonelli identifies the integral of a nonnegative product-measurable function with either iterated integral.

[F3]

Fubini's theorem for L^1 functions on a sigma-finite product: integrable functions on a product have integrable sections almost everywhere and their iterated integrals agree.

[F4]

Cauchy-Schwarz inequality for L2: L2 functions have integrable products and satisfy ∫∣uv∣≤∥u∥2∥v∥2.

Proof

Given: The objects in the Statement and facts [F1]–[F4].

1.1F1F2F3F4

Let f∈L2(μ). Tonelli applied to ∣f∣2 shows that for almost every xJ, the section z↦f(xJ,z) is square-integrable on the complementary probability space. Cauchy–Schwarz with the constant function 1 makes that section integrable, so [F1] defines its average there. If representatives f and f~ agree almost everywhere, Tonelli applied to ∣f−f~∣2 shows their sections agree almost everywhere for almost every xJ; their averages therefore define the same almost-sure class. Fubini gives measurability of the section-average function.

2.1F1F2F4step 1.1

On almost every section, Cauchy–Schwarz gives ∣PJf(xJ)∣2≤∫∣f(xJ,z)∣2 dμ−J(z) because μ−J has mass one. Integrating in xJ and using Tonelli yields ∥PJf∥22≤∥f∥22, so PJ is a contraction. Averaging a function already independent of z−J leaves it unchanged, hence PJ2=PJ.

3.1F1F3F4step 2.1

For f,g∈L2, Cauchy–Schwarz makes fg integrable. Fubini in the two groups of coordinates gives ⟨PJf,g⟩=∫EJ(PJf)(PJg) dμJ=⟨f,PJg⟩. Thus PJ is self-adjoint.

4.1F1F3step 1.1∎

Applying PK and then PJ integrates over the coordinates outside K, then over the coordinates in K∖J. Repeated finite-product Fubini permits this order and identifies the iterated integral with integration over the complement of J∩K. The equality holds almost everywhere by [F3], including when either set is empty or full, so PJPKf=PJ∩Kf in L2.

Depends on

Used by

Cited to discharge well-definedness by Product-coordinate averaging operators.

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Sources