For classical finite random variables, . Each identity follows by inserting the corresponding joint entropy into . The two orders are particularly useful when one variable is a deterministic function of the others, as in Fano's inequality via an error indicator.
If is a bijection of for every fixed , thenIn particular, translating a random variable in a finite group by a value determined by the conditioning variable does not change its conditional entropy.
Let take values in an alphabet of size , let be an estimate determined by , and put . Thenwhere is the binary entropy function. The error indicator costs at most bits, and after an error there are at most possible values of .
For a guess of a finite-alphabet variable , let and . The chain rule for conditional entropy gives . The first term is at most the binary entropy . The second is zero when the guess is right and at most when it is wrong, proving . This needs no optimality assumption on the guess.
If a uniform index has possibilities and every proposed success neighbourhood contains at most possibilities, then any estimator has failure probability at least the displayed expression. Condition on its success indicator: conditional entropy is at most . Subtract this from to bound the mutual information and rearrange. A metric Hamming ball gives approximate recovery rather than exact index decoding.
If independent random variables take values in a finite additive group, thenIndeed, , and symmetrically for . Independence is essential: taking makes the sum constant.
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Conditional entropy is a concept from information theory that quantifies the amount of uncertainty or information required to describe the outcome of a random variable, given that the value of another random variable is known. It effectively measures how much additional information is needed to describe a random variable \( Y \) when the value of another variable \( X \) is known.