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The capacity of the noisy quantum channel
Quantum Physics · Submitted 19 Apr 1996
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim An upper limit is given to the amount of quantum information that can be transmitted reliably down a noisy, decoherent quantum channel.
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The abstract, sentence by sentence
An upper limit is given to the amount of quantum information that can be transmitted reliably down a noisy, decoherent quantum channel. A class of quantum error-correcting codes is presented that allow the information transmitted to attain this limit. The result is the quantum analog of Shannon's bound and code for the noisy classical channel.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | An upper limit is given to the amount of quantum information that can be transmitted reliably down a noisy, decoherent quantum channel. | result 0.86 | 0.86 | 0.59 | asserted 1.00 |
| s1 | A class of quantum error-correcting codes is presented that allow the information transmitted to attain this limit. | contribution 0.86 | 0.91 | 0.31 | asserted 1.00 |
| s2 | The result is the quantum analog of Shannon's bound and code for the noisy classical channel. | interpretation 0.98 | 0.50 | 0.21 | asserted 1.00 |
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The paper
Original abstract
An upper limit is given to the amount of quantum information that can be transmitted reliably down a noisy, decoherent quantum channel. A class of quantum error-correcting codes is presented that allow the information transmitted to attain this limit. The result is the quantum analog of Shannon's bound and code for the noisy classical channel.
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References
How later papers used it
125 later papers cite it
1 later paper by other authors is listed below: 1 used its method or tool.
Uses its method or tool 1 of 3 papers with this label
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We quantify this information using the coherent information [ref] .
Markovian to non-Markovian phase transition in the operator dynamics of a mobile impurity (2024) · Echo protocol · 0.94
How the literature uses it
26 arXiv papers cite this in 33 sentences
Papers citing it · 14 sentences without a confident label
Builds on it 1 paper
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This kind of task was defined and developed in [ref] , albeit with the assistance of a particular kind of $k$-extendible channel and only the case $k=2$ was considered there, generalizing the usual notion of entanglement distillation and quantum communication protocols from [ref] .
Extendibility limits the performance of quantum processors · Introduction · 0.85
Cites it as background 17 papers
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The quantum capacity characterizes the ability of a quantum channel for this task in the absence of additional resources [ref] [equation] where $^(1)() = max_ϕ^AA'^(1)(,ϕ^AA')$ is the coherent information of a quantum channel.
Non-convexity of private capacity and classical environment-assisted capacity of a quantum channel · Communication tasks · 0.88
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It has been known for some time [ref] that the quantum capacity is given by a regularised expression—the optimisation of an entropic quantity (the coherent information) in the limit of arbitrarily many uses of the channel: [equation] (Here, $Q^(n)()$ is the coherent information $$ maximised over a joint input $ρ^(n)$ for $n$ uses of the channel $$.) However, the regularisation renders computing the quantum capacity infeasible; it involves an optimisation over an infinite parameter space.
Unbounded number of channel uses are required to see quantum capacity · Introduction · 0.98
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The quantum capacity is known to be lower bounded by the coherent information [ref] : Q(N)≥I_c(A⟩B) :=max_ρ(S(B)_σ-S(E)_σ), where the von Neumann entropies are evaluated on $σ_BE = U ρU^†$, with $U : A ↦BE$ the isometry associated to the channel $N$ as follows: $N(ρ) = tr_E(U ρU^y)$.
When does noise increase the quantum capacity? · Introduction · 0.92
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