Alphabeta Math
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Coefficient and factorial-effect variances under equal replication

Statement

Let r≥1 be an integer. For every run x∈Xk and replicate s∈{1,…,r}, suppose Yx,s=∑B⊆[k]βBxB+ϵx,s, where the coefficients βB are fixed and the errors are mutually independent real random variables on one probability space, with E[ϵx,s2]<∞ and common variance σ2<∞. Define Y‾x=r−1∑s=1rYx,s and β^A=2−k∑x∈XkxAY‾x. Then for every A⊆[k], Var⁡(β^A)=σ2r2k. For nonempty A, define τ^A as the difference of the mean run responses Y‾x over GA,+ and GA,− from Two-level full factorial designs and coded effects. Then τ^A=2β^A,Var⁡(τ^A)=4σ2r2k.

The variance calculation assumes equal replication at every run and independence across all run-replicate errors. It requires neither Gaussian errors nor zero interactions. A zero-mean assumption is additionally needed if βB is to denote coefficients of the mean response; it is not needed for these variance identities.

Facts & Assumptions

Given: The full factorial design and coefficient convention in Two-level full factorial designs and coded effects, the model and error hypotheses in the Statement, and the contrast identity in Orthogonality of the full two-level factorial contrasts.

[F1]

Two-level full factorial designs and coded effects: each column is xA=∏j∈Axj, and the normalized coefficient of a response table y is 2−k∑xxAyx; for nonempty A, the factorial effect is the difference of the two xA group means.

[F2]

Orthogonality of the full two-level factorial contrasts: 2−k∑xxAxB=1 when A=B and 0 otherwise.

[F3]

Random elements and real random variables: a real random variable is a measurable map from a probability space to R with its Borel sigma-algebra.

[F4]

Independent random elements: a family of random elements on one probability space is independent when their generated sigma-algebras are independent.

[F5]

Expectation of a nonnegative or integrable random variable: for a nonnegative measurable random variable U, E[U]=∫U dP.

[F6]

Moments, variance, and covariance on a probability space: for a square-integrable real random variable Z, Var⁡(Z)=E[(Z−EZ)2].

[F7]

Variance and covariance identities for random variables: covariance is symmetric and bilinear on finite linear combinations of square-integrable real random variables.

[F8]

Variance adds for every finite pairwise-independent family: the variance of a finite sum of pairwise-independent square-integrable real random variables is the sum of their variances.

Proof

technique · isolate each coefficient by the contrast Gram identity, then add the variances of the signed independent errors
1.1givenF1F2algebra

Substitute the model and the run averages into the definition of β^A. This gives β^A=∑B⊆[k]βB(2−k∑x∈XkxAxB)+1r2k∑x∈Xk∑s=1rxAϵx,s. By [F2], the parenthesized factor is 1 for B=A and 0 otherwise. Thus β^A−βA=(r2k)−1∑x,sxAϵx,s.

1.2givenF3F4F5F6F7algebra

Fix A and put Zx,s=xAϵx,s. Each xA is +1 or −1, so multiplication by xA is a Borel bijection whose inverse is itself; consequently σ(Zx,s)=σ(ϵx,s). By [F3] and [F4] these variables remain mutually, hence pairwise, independent. Their second moments are finite by the hypothesis, and 2∣z∣≤1+z2 gives E∣Zx,s∣<∞, so their variances are defined. By [F6], variance is covariance with both arguments equal; then [F7] gives Var⁡(Zx,s)=xA2Var⁡(ϵx,s)=σ2.

2.1F7F8step 1.1step 1.2algebra

There are r2k variables Zx,s. By [F8], their sum has variance r2kσ2. Applying the scalar rule from [F7] to step 1.1 yields Var⁡(β^A)=(r2k)−2r2kσ2=σ2/(r2k).

3.1F1F7step 2.1choosealgebra∎

For nonempty A, choose j∈A. Reversing coordinate xj bijects GA,+ with GA,−, so each group has 2k−1 runs. The difference of their run-average means is therefore 21−k∑xxAY‾x=2β^A by [F1]. Its variance is four times the coefficient variance from step 2.1, giving 4σ2/(r2k).

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