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Holevo–Schumacher–Westmoreland capacity theorem for finite cq channels
Statement
Let be a finite-input, finite-output memoryless cq channel as in Finite-input memoryless cq channel. With the average-error code convention of Finite cq block codes, average error, and capacity, its classical capacity in nats per use is For every a sequence of codes with rate tending to has average error tending to zero, and every reliable sequence has limiting upper rate at most . This theorem concerns a fixed finite classical input alphabet and does not assert a single-letter formula for general quantum-input channels.
Facts & Assumptions
Given: A finite nonempty alphabet , nonzero finite-dimensional output space , and one density operator for each input symbol.
Finite cq block codes, average error, and capacity: codes use a uniform finite message, deterministic input words, a finite decoding POVM, average block error, and rate nats/use.
The finite Holevo measurement bound: for any finite ensemble of states and any finite POVM, the classical mutual information of the input and the measurement outcome is at most the ensemble Holevo information.
Typical-projector bounds for finite quantum sources and cq ensembles: for a finite ensemble, a high-probability input typical set has conditional and global output projectors with exponentially controlled rank and operator bounds, and uniform acceptance error tending to zero.
Finite square-root measurement packing bound for cq states: projectors satisfying those four bounds give expected average decoding error at most .
Strong subadditivity of finite-dimensional quantum entropy: for every finite tripartite state, .
Continuity of finite-dimensional quantum entropy: entropy is continuous in operator norm on finite-dimensional state spaces, including at zero eigenvalues.
Finite-alphabet Fano inequality: for a finite message estimated from a finite observation with error probability , .
Finite entropy and mutual-information chain rules: for finite variables, .
Partial trace over a finite tensor factor and The partial trace is characterized by the trace pairing and is basis-independent: tracing tensor factors gives the usual marginals, is linear, and is independent of the chosen orthonormal basis.
Ordered tensor registers, their inner product, and wire permutations: the product basis is ordered factorwise and product operators act on their corresponding tensor factors.
Complex spectral theorem: a normal endomorphism of a finite-dimensional complex inner product space has an orthonormal eigenbasis, and conversely: finite-dimensional Hermitian states have orthonormal eigenbases.
Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm: the natural logarithm is additive on finite products of positive numbers.
Heine-Borel in : with the Euclidean metric a subset of is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line and A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value: the closed probability simplex in finite-dimensional Euclidean space is compact, and a continuous real function on it attains a maximum.
The operator norm is zero on the zero domain and otherwise is max_{||v||=1} ||Tv||: the operator norm is the maximum of over unit vectors .
Density operator: each output state is nonnegative and has trace one.
The partial trace is characterized by the trace pairing and is basis-independent and Trace is a linear functional on : product-state marginals and finite mixture marginals are computed by partial trace and finite linearity.
Proof
Write . The simplex is nonempty, closed, and bounded. For each state , [F12] diagonalizes it with nonnegative eigenvalues summing to one by [F16], so its action on a unit vector has norm at most one and [F15] gives . Therefore . Fix an orthonormal basis identifying unitarily with ; this preserves spectra and operator norm, so [F7] applies. Thus the first entropy term in is continuous in ; the second is a finite linear sum. Thus [F14] shows the supremum is attained, so . A point-mass input law gives by [F2], hence .
Fix and . Choose with . Let be the input typical set from [F4], with excluded probability . Since , for all sufficiently large ; for each earlier blocklength choose a fixed and use the one-message code with word and decoding POVM . Draw each large- codeword independently from conditioned on . Its mean output state is The global typical projector from [F4] therefore obeys . Each conditional projector has acceptance at least , rank at most , and the global projector accepts every conditioned codeword with at least , where and .
Consider any code with , uniform message , output states , decoding outcome , and average error . The Holevo measurement bound [F3] gives . Applying Fano [F8] and the finite mutual-information identity [F9], with , yields . For , [F2] gives , so the inequality is .
Since , choose large enough that and for every . For the finite prefix , set and use the one-message code from step 1.2. For , set and apply the packing lemma [F5] to the conditional input law on , with and . It gives expected average error at most Since for and , this tends to zero. Merge the packing POVM's failure effect into message 1: put and for . These effects are positive and sum to ; message 1's success increases by , while every other success is unchanged. Thus their average error obeys the same expectation bound, including . The codebook space is finite; order once and choose its lexicographically first codebook whose average error is at most this expectation. This defines a deterministic code for each without any choice axiom, and the finite one-message prefix does not affect .
Let and . By [F17], its th marginal is , which is a state by [F16]. For any bipartite state , tensor it with the unique state on a one-dimensional middle register : the four entropies in [F6] become , because tensoring with this factor leaves the spectrum unchanged. Thus [F6] implies ; iterating gives . Product entropy is additive: diagonalize each by [F12], so every positive product eigenvalue has logarithm equal to the sum of its coordinate logarithms by [F13]; zero eigenvalues contribute zero by [F2]. Summing these finite terms gives . Therefore
The selected codes have average error tending to zero and . If , the single-message code has zero error. When , taking a maximizing from step 1.1 proves achievability of every . When , the single-message code shows that rate zero is reliable.
Combining steps 1.3 and 2.2 gives . For any reliable sequence, divide by and let ; since , its limiting upper rate is at most . Together with step 3.1 and the capacity definition [F1], this proves the theorem.
Depends on
- Finite cq block codes, average error, and capacity
- Finite-input memoryless cq channel
- Finite classical-quantum states and Holevo information
- The finite Holevo measurement bound
- Typical-projector bounds for finite quantum sources and cq ensembles
- Finite square-root measurement packing bound for cq states
- Strong subadditivity of finite-dimensional quantum entropy
- Continuity of finite-dimensional quantum entropy
- Finite-alphabet Fano inequality
- Finite entropy and mutual-information chain rules
- Partial trace over a finite tensor factor
- The partial trace is characterized by the trace pairing and is basis-independent
- Ordered tensor registers, their inner product, and wire permutations
- Complex spectral theorem: a normal endomorphism of a finite-dimensional complex inner product space has an orthonormal eigenbasis, and conversely
- Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm
- The operator norm is zero on the zero domain and otherwise is max_{||v||=1} ||Tv||
- Density operator
- Heine-Borel in $\mathbb{R}^n$: with the Euclidean metric a subset of $\mathbb{R}^n$ is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line
- A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value
- Trace is a linear functional on $M_n(F)$
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Sources
- Mark M. Wilde, From Classical to Quantum Shannon Theory, second-edition prepublication v8, Chapters 16 and 20 (standard reference, not scraped)
- John Watrous, The Theory of Quantum Information, §8.1.2 (standard reference, not scraped)