For finite random variables , let be the error probability of maximum a posteriori decoding of from . Then when conditional entropy is measured in bits. At each positive-probability output , the optimum success probability is the largest posterior atom , so its conditional error is . Apply the entropy lower bound from the largest atom to that posterior to get , then average over . An arbitrary decoder need not satisfy this bound; it uses the optimum conditional decision rule.
Fano's inequality Created 2026-09-29 Updated 2026-10-14
Fano's inequality turns remaining uncertainty into a constraint on decision errors. If an observation leaves many plausible answers, a decoder cannot usually recover the answer reliably. Its elegant idea is to separate two uncertainties: whether the guess was wrong, and which alternative was correct when it was wrong.
Let be discrete random variables, with taking values in a finite alphabet of cardinality . Choose any deterministic decoder whose output lies in , and define its average error probability . With base-two logarithms, Fano's inequality states
Here is conditional entropy and is binary entropy, with at the endpoints. Both sides are measured in bits; using natural logarithms throughout gives the same inequality in nats. No uniform source, independence of , or optimality of the decoder is assumed. Requiring its output to belong to the same alphabet is what leaves at most alternatives after an error.[ref]
For an exact toy example, give the discrete uniform distribution on . A channel reports with probability and reports each of the other three symbols with probability , where . Use the decoder . The output is uniform, and the conditional probabilities after any report are
Thus and direct calculation of the conditional entropy gives
This is equality in Fano's inequality for every . At , each report leaves probabilities , up to their order, and bits. The two contributions are bits for the error flag and bits for identifying the correct alternative after an error. These are theoretical probabilities, not measured data.
Figure 1.
A symmetric four-symbol toy channel makes every step of Fano's bound an equality
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The identity decoder in this example minimizes error only for : its guessed symbol has the largest posterior probability exactly when . At , are independent random variables and all four guesses tie. For , guessing any one of the three other symbols has error probability . Equality in Fano's inequality therefore does not certify an optimal decoder.
For usefulness, combine with to obtain the simpler consequence
For a uniform , , so this becomes . This connects mutual information to unavoidable decision error in channel coding or classification in statistical learning; it can rule out reliable recovery regardless of the chosen decoder.[ref]
The sharper right-hand side increases from zero to on , then decreases: in the interior, . When interpreting the inequality by inverting a curve, use its increasing branch to obtain a lower error threshold. A decoder that chooses a largest posterior probability, as in maximum a posteriori decoding, always has , since the largest of conditional probabilities is at least . Arbitrary decoders can have larger error. In particular, low conditional entropy does not force every decoder to work well: with a fair binary and , the rule has even though . Fano's inequality supplies a constraint, not an exact error prediction for each rule.
Min-entropy Created 2026-09-28 Updated 2026-10-14
For a discrete random variable with a finite or countable alphabet and probability mass function , define . Its min-entropy, using base-two logarithms, is
The unit is the bit. This is the smallest information content of any possible outcome: it records the easiest outcome to predict, whereas Shannon entropy averages information content over all outcomes. A normalized countable probability mass function has an attained positive maximum, so is finite even when Shannon entropy is infinite. Outcomes of zero probability cannot minimize the surprise and are omitted from the minimum; including extra impossible symbols changes neither quantity.[ref]
Suppose someone knows the probability mass function but receives no observation correlated with , and must name exactly one outcome. Naming succeeds with probability , so naming a most likely outcome is optimal:
Tied maxima give equally good guesses. Randomizing independently among guesses cannot improve success: if the guess has probability mass function , its success probability is . This is the simplest instance of maximum a posteriori decoding. The identity gives min-entropy an operational meaning: bits means every single guess succeeds with probability at most , under these information assumptions.[ref]
For an exact analytical example on symbols , compare the two probability mass functions
Under , each possible outcome has information content bits; under , has information content bit and each other outcome has bits. Consequently their Shannon entropies agree exactly,
but and bits. A best single guess therefore succeeds with probability under and under . The same average surprise can hide a factor of two in immediate predictability. The zero entry in contributes zero to Shannon entropy, using .
Figure 1.
Two exact probability models have the same average surprise but different best single guesses
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For the discrete uniform distribution on possible outcomes, bits and the best single guess succeeds with probability . A certain outcome has and success probability one. Thus min-entropy is useful when a common outcome could defeat an attempt to make outputs unpredictable, even if rare alternatives raise Shannon entropy.
For cryptography, this unconditional calculation alone does not certify security: an observer might know already. If a report reveals a uniform four-outcome source, its unconditional min-entropy remains bits but guessing after the report succeeds with probability one. For finite classical reports, the appropriate success calculation uses conditional probabilities and maximum a posteriori decoding:
The conditional entropy instead averages remaining surprise. A security argument must specify the observer's information and the protocol's required guarantee; neither unconditional min-entropy nor Shannon entropy supplies those assumptions.
Maximum a posteriori decoding chooses an input with the largest posterior probability given the received word. By Bayes' theorem this maximizes over candidate codewords, minimizing the average probability of a decoding error.
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.
The ideal observer performs maximum a posteriori decoding: for received word , it maximizes , equivalently . Maximum-likelihood decoding maximizes the latter conditional likelihood alone. Minimum-distance decoding minimizes the Hamming distance . Ties may be resolved arbitrarily among maximizers.
For independent errors in a binary symmetric channel,
For , its ratio on increasing the distance by one is . Thus maximum-likelihood decoding and minimum-distance decoding select exactly the same codewords. At the allowed endpoint , they agree on a possible observation ; impossible observations have zero likelihood for every codeword, so an arbitrary maximum-likelihood tie rule need not agree with minimum distance. This qualification is needed for the literal assumption .
For the specified observation, the Hamming distances from 000 and 111 are two and one. Their likelihoods are and , respectively. After multiplying by the priors, their joint probabilities are and , so their posterior probabilities are and . Therefore