For finite-valued random vectors, write and . The conditional entropy is the average entropy of the posterior distributions:
Equivalently, . Since , splitting the logarithm gives
Use 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 gives
because conditional entropy is nonnegative. Consequently
A deterministic coarsening can merge distinguishable source outcomes, but cannot create additional Shannon entropy.
Choose a most probable symbol , and let . Its binary entropy is
Since is a function of , part (a)(ii) gives . On , the concave function lies above the chord joining and . That chord has height . Therefore
The endpoint is included by continuity and corresponds to a deterministic source.
Every positive atom has probability at most , so . Averaging yields
For , the supplied inequality gives . Rearranging proves
The 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 gives
Average 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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