For finite-valued random vectors, write and . The conditional entropy is the average entropy of the posterior distributions:Equivalently, . Since , splitting the logarithm givesUse the usual convention and omit conditionals at zero-probability outputs. The same identities hold for countable alphabets whenever the entropy sums are well-defined, without subtracting two infinite quantities.
Set . Given , the value of is certain, so . Applying the entropy identity in the two orders givesbecause conditional entropy is nonnegative. ConsequentlyA deterministic coarsening can merge distinguishable source outcomes, but cannot create additional Shannon entropy.
Choose a most probable symbol , and let . Its binary entropy isSince is a function of , part (a)(ii) gives . On , the concave function lies above the chord joining and . That chord has height . ThereforeThe endpoint is included by continuity and corresponds to a deterministic source.
Every positive atom has probability at most , so . Averaging yieldsFor , the supplied inequality gives . Rearranging provesThe two regimes combine into the entropy lower bound from the largest atom, valid for every finite probability distribution.
Given an output of positive probability, the ideal observer chooses a symbol maximizing the posterior:Ties may be broken arbitrarily, and the choice at an impossible output does not matter. This is maximum a posteriori decoding. It minimizes conditional error at each , because a deterministic decision is correct with probability ; a randomized decision is a weighted average of these success probabilities and cannot exceed their maximum.
Write . Then . Applying the two cases from part (b) to the posterior distribution givesAverage with respect to the output law to obtain the conditional entropy upper bound on minimum decoding error:This is an upper bound on the optimum error probability; it does not hold for arbitrary deliberately poor decoding rules.
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