For a finite probability distribution with largest atom , its base-two Shannon entropy satisfies . If , coarsen the distribution to the indicator of a largest atom: Shannon entropy cannot increase under a deterministic function, so . The concavity of binary entropy places it above the chord from to , giving . If , every nonzero probability has , so . The function vanishes at and has negative derivative on , proving the same bound. Equality in the combined bound occurs for a point mass or a distribution uniform on two points.
Fix the channel matrix . The mixed input induces the mixed output . The concavity of information entropy implies
For completeness, the difference is by Gibbs inequality, including zero coordinates with the usual conventions.
On the other hand, conditional output entropy is linear in the input law:
Subtracting gives the concavity of mutual information in the input distribution:
This makes maximizing mutual information over the input probability simplex a concave optimization problem: a local maximum is global. It also justifies averaging input distributions over channel symmetries when searching for an optimum, since symmetry averaging cannot lower the achieved mutual information. The channel itself is held fixed throughout.
Choose noise values , giving exactly the outputs . The transition matrix, in that column order, is
An input probability mass function makes outputs equiprobable, so and . Hence bit per use, as required for comparison with the four-output case.
There is a strict improvement, which can also be computed exactly. Reflection of the input labels , accompanied by output reflection , leaves mutual information unchanged. Concavity of information entropy makes mutual information a concave function of the input probability mass function for a fixed transition matrix. Averaging an input law with its reflection therefore cannot decrease it. It suffices to consider
The outputs whose labels are even integers have total mass and conditional probability mass function , with information entropy . The outputs whose labels are odd integers have mass and conditional probability mass function , with information entropy one. Splitting first by output parity using the chain rule for information entropy yields
Its derivative is , and its second derivative is negative. The unique maximum occurs at , giving
This additional optimization explains the collision pattern: outputs identify input , outputs identify the two extreme inputs, and only output is ambiguous.
Figure 1.
Three original additive-noise channel diagrams: increasing noise separation changes output collisions and channel capacity
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Introduce a selector with Bernoulli distribution of parameter , and construct by taking its conditional law given to be , and its conditional law given to be . No prescribed joint law of is needed. Summing over the selector gives the desired mixture probability mass function. The conditional entropy is
Since conditioning cannot increase information entropy,
This proves the concavity of information entropy. The argument also covers infinite information entropies with the convention that a zero mixing weight contributes zero. At or , the mixture is the corresponding original law and equality is immediate.
Draw uniformly from and let be uniform on independently. Then
If denotes the marginal law of , this also says . Since is uniform on ,
Subadditivity of information entropy followed by concavity of information entropy gives
Exponentiating proves .
Let be the marginal probability distribution of . Subadditivity of information entropy and the concavity of information entropy give
For each ,
so .
Suppose one row of a finite discrete memoryless channel is a convex combination of other rows: . Deleting input leaves the channel capacity unchanged. Given any input law with mass on , move that mass to the other symbols in proportions . The output law stays the same. By the concavity of information entropy, , so this replacement cannot increase conditional entropy and cannot decrease mutual information. Taking maxima proves the claim; the smaller channel is also trivially a restriction of the original one. If the entropy inequality is strict, every positive use of the redundant row is strictly suboptimal compared with its redistribution.
Let the input alphabet be and let the output be , where independent noise is uniform on two distinct integers. Translating the output alphabet reduces the noise to , . The reachable output alphabet has size : it is the union of two three-element intervals shifted by .
For , every row of the transition matrix has conditional information entropy one bit, so . Input probabilities make the output uniform and attain one bit per use. For , the two translated input alphabets are disjoint and every output identifies its input. A uniform input then attains bits per use.
For , reflection symmetry and concavity of information entropy permit restricting to input probabilities . Conditional on output parity, outputs whose labels are even integers have probabilities and outputs whose labels are odd integers have probabilities . Consequently . Its strictly negative second derivative and stationary equation give and channel capacity . All three values follow from overlap of translated input alphabets, rather than from output alphabet size alone.