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Entropy Rate

Definition (Entropy Rate)

The entropy rate of a source {Xi}i=1∞\{X_{i}\}^{\infty}_{i=1} with alphabet X\mathcal{X} is denoted by H(X)H(\mathcal{X}) and defined by H(X):=lim⁡n→∞1nH(Xn)H(\mathcal{X}):=\lim_{n\to\infty} \frac{1}{n}H(X^{n})provided that the limit exists.

Remark

If source {Xi}i=1∞\{X_{i}\}^{\infty}_{i=1} is a DMS (i.e. iid), then H(X)=lim⁡n→∞1nH(X1,⋯ ,Xn)=lim⁡n→∞1n(nH(X1))=H(X1)H(\mathcal{X})=\lim_{n\to\infty} \frac{1}{n}H(X_{1},\cdots,X_{n})=\lim_{n\to\infty} \frac{1}{n}(nH(X_{1}))=H(X_{1})

Lemma

For a stationary source {Xi}i=1∞\{X_{i}\}^{\infty}_{i=1}, the sequence of conditional entropies {H(Xi∣Xi−1)}i=1∞\{H(X_{i}|X^{i-1})\}^{\infty}_{i=1} is decreasing in ii and has a limit denoted by H~(X):=lim⁡i→∞H(Xi∣Xi−1)\tilde H(\mathcal{X}):=\lim_{i\to\infty}H(X_{i}|X^{i-1})

Theorem

For a stationary source {Xi}i=1∞\{X_{i}\}^{\infty}_{i=1}, its entropy rate H(X)H(\mathcal{X}) always exists and is equal to H~(X)\tilde H(\mathcal{X}): H(X)=H~(X)=lim⁡n→∞H(Xn∣Xn−1)H(\mathcal{X})=\tilde H(\mathcal{X})=\lim_{n\to\infty}H(X_{n}|X^{n-1})

Remark

  • Since H~(X)=H(X)\tilde H(\mathcal{X})=H(\mathcal{X}) and H(Xn∣Xn−1)↓H~(X)H(X_{n}|X^{n-1})\downarrow\tilde H(\mathcal{X}) by lemma 1, then we have H(X)≤H(Xn∣Xn−1) ∀n≥1H(\mathcal{X})\le H(X_{n}|X^{n-1}) \ \forall n\ge 1
  • Can also be shown that 1nH(Xn)\frac{1}{n}H(X^{n}) is decreasing in nn H(X)≤1nH(Xn) ∀n≥1H(\mathcal{X})\le \frac{1}{n}H(X^{n}) \ \forall n\ge1

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