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Conditional block law factors across IID coordinates

Statement

Let Zt=(X1,t,…,Xk,t) be a finite-alphabet IID multisource with joint law P. For nonempty S⊆[k], put C=Sc. If (xSn,xCn) is supported under P⊗n, then the conditional block probability obtained from its joint and complement marginal satisfies P⊗n(xSn∣xCn)=∏t=1nPXS∣XC(xS,t∣xC,t).

Facts & Assumptions

Given: The finite-alphabet IID multisource, a nonempty S⊆[k], and supported blocks (xSn,xCn).

[F1]

Finite-alphabet IID multisource: the joint letter law is P, and P⊗n(zn)=∏t=1nP(zt).

[F2]

Finite conditional entropy: for PXS,XC(s,c)>0, the conditional probability is PXS∣XC(s∣c)=PXS,XC(s,c)/PXC(c).

[F3]

Marginals and positive-mass conditionals of a finite joint law are probability vectors: finite joint-law marginals are probability vectors; positive-mass conditional vectors are well-defined probability vectors.

Proof

1.1F1F3algebra

For each coordinate t, support gives PXS,XC(xS,t,xC,t)>0, and the finite marginal sum PXC(xC,t)=∑xSPXS,XC(xS,xC,t) is therefore positive by [F3]. Summing the finite product law over all xSn and distributing the finite sums gives PXCn⊗n(xCn)=∑xSn∏t=1nPXS,XC(xS,t,xC,t)=∏t=1nPXC(xC,t)>0. Thus the conditional block probability is defined by dividing its joint mass by this positive complement marginal.

2.1F1F2step 1.1algebra∎

Using [F1] for the numerator and step 1.1 for the denominator, that ratio is ∏t=1nPXS,XC(xS,t,xC,t)∏t=1nPXC(xC,t)=∏t=1nPXS,XC(xS,t,xC,t)PXC(xC,t)=∏t=1nPXS∣XC(xS,t∣xC,t), where each final factor is the conditional probability in [F2]. This proves the factorization.

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