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Finite-IID rate-distortion mutual-information converse

Statement

Let S1,…,Sk be IID with law PS on a finite nonempty alphabet S, let S^ be finite nonempty, and let d:S×S^→[0,∞) be finite-valued. For any joint law of Sk and S^k, put Dk:=Edk(Sk,S^k), using the normalized block distortion of Single-letter and block distortion. If R(D) is the finite-alphabet information rate-distortion function in bits from Finite-alphabet information rate-distortion function, then

ln⁡2 R(Dk)≤1kI(Sk;S^k),

where mutual information on the right is in nats. The test channel induced by the joint law is feasible at distortion Dk, so the rate-distortion minimum is attained there by Attainment of finite-alphabet rate-distortion minima.

Facts & Assumptions

Given: A finite IID source, finite reproduction alphabet, finite nonnegative distortion, and any joint distribution of Sk,S^k.

[A1]

S1,…,Sk are IID with common law PS; hence each coordinate has law PS and is independent of its predecessors.

[F1]

Finite-alphabet information rate-distortion function and Attainment of finite-alphabet rate-distortion minima: R(D) is the minimum finite mutual information in bits over test channels with source law PS and expected distortion at most D; every feasible minimum is attained.

[F2]

Single-letter and block distortion: dk(sk,s^k)=k−1∑i=1kd(si,s^i).

[F3]

Finite mutual information and Finite entropy and mutual-information chain rules: finite mutual information has the chain rule, including I(U;V,Z)=I(U;Z)+I(U;V∣Z).

[F4]

Finite conditional mutual information identities and equality: finite conditional mutual information is nonnegative.

[F5]

Finite information quantities convert by the logarithm base: information in bits equals information in nats divided by ln⁡2.

Proof

1.1A1F1F2givenconstruct

Let T be uniform on [k], independent of (Sk,S^k), and put (S,S^)=(ST,S^T). By [A1], S has law PS; by [F2], Ed(S,S^)=k−1∑iEd(Si,S^i)=Dk. For each s with PS(s)>0, the conditional law of S^ given S=s is a probability vector; choose any probability-vector row for zero-mass s. This gives a finite test channel with source law PS and distortion Dk, so it is feasible in [F1].

1.2A1F3F4givenalgebra

The chain rule [F3] gives I(Sk;S^k)=∑i=1kI(Si;S^k∣Si−1). Since I(Si;Si−1)=0 by [A1], the chain rule gives I(Si;S^k∣Si−1)=I(Si;S^k,Si−1). Write Ui=(S^k,Si−1); its coordinate S^i is a function of Ui, so I(Si;Ui,S^i)=I(Si;Ui). Expanding the left side by [F3] and using [F4] yields I(Si;Ui)=I(Si;S^i)+I(Si;Ui∣S^i)≥I(Si;S^i). Summing proves ∑iI(Si;S^i)≤I(Sk;S^k).

2.1F1F3F4F5step 1.1step 1.2algebra∎

By the chain rule, I(S;S^∣T)=k−1∑iI(Si;S^i). Since S and T are independent, I(S;S^,T)=I(S;S^∣T); also I(S;S^,T)=I(S;S^)+I(S;T∣S^)≥I(S;S^) by [F3]–[F4]. Thus I(S;S^)≤k−1∑iI(Si;S^i)≤k−1I(Sk;S^k) by step 1.2. The test channel in step 1.1 is feasible, so [F1] gives R(Dk)≤I2(S;S^), where the subscript denotes bits. Multiply by ln⁡2 and use [F5] to obtain the claimed nats inequality.

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