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Pooled-mixture projection and variance
Statement
Use the setup of Two-sample order-r U-statistic and first projections and suppose is antisymmetric under exchange of its two blocks and has finite second moment under every independent P/Q assignment to its positions. For put and define
Then , the first projection in the second block is , and is finite. The map is continuous on . In particular, with and ,
Facts & Assumptions
Given: A block-symmetric kernel, its antisymmetry under exchange of blocks, and finite second moments under all mixed P/Q assignments.
Two-sample order-r U-statistic and first projections defines the block kernel and its first projections.
First projections are measurable and square-integrable gives the section-integral versions and their L2 bounds.
Moments, variance, and covariance on a probability space defines the second-moment variance when .
Cauchy-Schwarz inequality for makes cross products of the finitely many square-integrable mixed-assignment section functions integrable.
Fubini's theorem for L^1 functions on a sigma-finite product supplies measurable integrable section functions and equality of iterated integrals on the mixed product probability spaces.
Proof
Given: The hypotheses in the Statement. Prove the pooled mean, sign relation, finiteness, and continuity claims.
Under , swapping the first and second blocks preserves the product law and changes to . Therefore , so it is zero.
Expand each factor in the section integral. This writes as a finite sum , where ranges over assignments of P and Q to the remaining coordinates, is a polynomial, and is the corresponding section integral. For either first-coordinate law , write for product expectation with independent coordinates having law first and the laws specified by in the remaining positions. The mixed-moment assumption gives both and . Cauchy--Schwarz [F4] also makes integrable with first-coordinate law . Fubini [F5] on that product space supplies one measurable version of , valid -almost everywhere after setting it to zero on the common exceptional set. Cauchy--Schwarz on the remaining probability product then gives for each , as in the section-integral argument of [F2]. Consequently every cross integral is finite by [F4]. Expanding now gives a finite sum of polynomial coefficients times these finite cross integrals, so it is finite and continuous in .
Holding the first coordinate of fixed and integrating the other coordinates with law defines , since the kernel mean in [F1] is zero by step 1.1. For the projection in the second block, exchange the blocks inside the integral. Antisymmetry changes the sign and the common product law is unchanged, so the second-block projection is .
Since and , step 1.2 gives , while . Multiplication by proves the displayed limit.
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