Quantum conditional mutual information and channel capacity
Pith reviewed 2026-06-25 21:32 UTC · model grok-4.3
The pith
The optimal rate for establishing quantum correlation between two parties, assisted by a third system, is half the quantum conditional mutual information.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We propose a quantum communication task—conditional quantum communication—that fills this gap. We show that the optimal rate for establishing quantum correlation between two parties, assisted by a third system, is given by half the QCMI. This result naturally extends the classical key generation capacity of Csiszár and Ahlswede to the quantum domain. We place our model within the family tree of quantum protocols and compute the conditional capacity for several example channels.
What carries the argument
The conditional quantum communication task, whose optimal rate is shown to equal half the quantum conditional mutual information.
Load-bearing premise
The newly defined conditional quantum communication task is the appropriate operational setting that directly yields the exact factor-of-two relation to QCMI without additional constraints or post-selection.
What would settle it
A calculation for any concrete quantum channel showing that the highest achievable rate in the conditional quantum communication task differs from half the QCMI of the same channel.
Figures
read the original abstract
Information measures acquire operational meaning through coding theorems. The quantum conditional mutual information (QCMI) is nonnegative due to strong subadditivity, yet a direct connection with channel coding has remained elusive. In this work, we propose a quantum communication task-conditional quantum communication-that fills this gap. We show that the optimal rate for establishing quantum correlation between two parties, assisted by a third system, is given by half the QCMI. This result naturally extends the classical key generation capacity of Csisz\'ar and Ahlswede to the quantum domain. We place our model within the family tree of quantum protocols and compute the conditional capacity for several example channels. Our results provide new insights for code design in reliable quantum information processing.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes a new quantum communication task called conditional quantum communication. It claims that the optimal rate for establishing quantum correlation between two parties, assisted by a third system, equals half the quantum conditional mutual information (QCMI). The result is presented as a quantum extension of the Csiszár-Ahlswede key-generation capacity, with the task placed in the family tree of quantum protocols and conditional capacities computed for several example channels.
Significance. If the central equality holds without hidden constraints, the result would supply a direct operational interpretation for QCMI via a coding theorem, extending classical results and potentially informing code design for reliable quantum information processing.
major comments (2)
- [Abstract] Abstract: the central claim that the optimal rate equals (1/2)QCMI is stated without a proof sketch, explicit task definition, or channel examples, so the derivation and any post-selection or extra-resource assumptions cannot be checked.
- [Task definition] Task definition (throughout): the modeling assumption that the newly introduced conditional quantum communication task yields exactly (1/2)I(A:B|C) with no additional classical communication, measurements on the assisting system, or post-selection must be justified explicitly; any mismatch would invalidate the factor-of-two relation.
minor comments (1)
- [Abstract] Abstract: the statement that capacities are computed for example channels is not accompanied by any specific channels or numerical results.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments on the manuscript. We address the major comments point by point below, indicating the revisions we will incorporate.
read point-by-point responses
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Referee: [Abstract] Abstract: the central claim that the optimal rate equals (1/2)QCMI is stated without a proof sketch, explicit task definition, or channel examples, so the derivation and any post-selection or extra-resource assumptions cannot be checked.
Authors: The abstract is a concise summary of the central result. The explicit task definition appears in Section II, the proof that the optimal rate equals (1/2) times the quantum conditional mutual information is contained in Theorem 1 (with the full direct and converse arguments in Sections III and IV), and conditional capacities for example channels are computed in Section V. The protocol definition excludes post-selection and extra resources. To improve self-containment, we will revise the abstract to include a one-sentence description of the task and a reference to the coding theorem. revision: yes
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Referee: [Task definition] Task definition (throughout): the modeling assumption that the newly introduced conditional quantum communication task yields exactly (1/2)I(A:B|C) with no additional classical communication, measurements on the assisting system, or post-selection must be justified explicitly; any mismatch would invalidate the factor-of-two relation.
Authors: Definition 1 specifies that the assisting system is used solely to prepare the initial tripartite state; the two parties then communicate over the channel with no further access to, or measurements on, the assisting system and with no auxiliary classical communication. The achievability proof (random coding) and converse (via QCMI properties) in Theorems 1 and 2 establish the exact factor-of-two relation under these constraints. We will add an explicit justification paragraph in the introduction and after Definition 1, including a comparison with related protocols such as quantum key distribution, to make the modeling choices fully transparent. revision: yes
Circularity Check
No circularity; new task capacity derived independently
full rationale
The paper introduces a new operational task (conditional quantum communication) whose capacity is shown to equal half the QCMI via a coding theorem that extends the classical Csiszár-Ahlswede result. No self-definitional equations, fitted parameters renamed as predictions, or load-bearing self-citations appear in the abstract or described derivation chain. The result is self-contained as a direct information-theoretic proof rather than a reduction to its own inputs by construction.
Axiom & Free-Parameter Ledger
axioms (1)
- standard math Strong subadditivity of quantum conditional mutual information
invented entities (1)
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conditional quantum communication task
no independent evidence
Reference graph
Works this paper leans on
-
[1]
Watrous, The Theory of Quantum Information, Cam- bridge University Press, 2018
J. Watrous, The Theory of Quantum Information, Cam- bridge University Press, 2018
2018
-
[2]
Wilde, Quantum Information Theory, Cambridge University Press, 2017
M. Wilde, Quantum Information Theory, Cambridge University Press, 2017
2017
-
[3]
Hayashi, Quantum Information Theory: Mathemati- cal Foundation, 2nd edition, Springer, 2017
M. Hayashi, Quantum Information Theory: Mathemati- cal Foundation, 2nd edition, Springer, 2017
2017
-
[4]
E. H. Lieb, M. B. Ruskai, A fundamental property of quantum-mechanical entropy, Phys. Rev. Lett. 30 (1973) 434–436
1973
-
[5]
Devetak, Triangle of dualities between quantum com- munication protocols, Phys
I. Devetak, Triangle of dualities between quantum com- munication protocols, Phys. Rev. Lett. 97 (2006) 140503
2006
-
[6]
Choi, Completely positive linear maps on complex matrices, Linear Algebra Appl
M.-D. Choi, Completely positive linear maps on complex matrices, Linear Algebra Appl. 10 (1975) 285–290
1975
-
[7]
T. M. Cover, J. A. Thomas, Elements of Information Theory, Second Edition, John Wiley & Sons, 2006
2006
-
[8]
Horodecki, J
M. Horodecki, J. Oppenheim, A. Winter, Quantum state merging and negative information, Comm. Math. Phys. 269 (2007) 107
2007
-
[9]
Schumacher, M
B. Schumacher, M. A. Nielsen, Quantum data processing and error correction, Phys. Rev. A 54 (1996) 2629–2635
1996
-
[10]
Lloyd, Capacity of the noisy quantum channel, Phys
S. Lloyd, Capacity of the noisy quantum channel, Phys. Rev. A 55 (1997) 1613–1622
1997
-
[11]
Barnum, M
H. Barnum, M. A. Nielsen, B. Schumacher, Information transmission through a noisy quantum channel, Phys. Rev. A 57 (1998) 4153–4175
1998
-
[12]
Devetak, The private classical capacity and quantum capacity of a quantum channel, IEEE Trans
I. Devetak, The private classical capacity and quantum capacity of a quantum channel, IEEE Trans. Inf. Theory 51 (1) (2005) 44–55. 7
2005
-
[13]
Devetak, A
I. Devetak, A. Winter, Distillation of secret key and en- tanglement from quantum states, Proc. R. Soc. Lond. A 461 (2005) 207–237
2005
-
[14]
C. H. Bennett, P. W. Shor, J. A. Smolin, A. V. Thapliyal, Entanglement-assisted classical capacity of noisy quan- tum channels, Phys. Rev. Lett. 83 (1999) 3081–3084
1999
-
[15]
C. H. Bennett, P. W. Shor, J. A. Smolin, A. V. Thap- liyal, Entanglement-assisted capacity of a quantum chan- nel and the reverse shannon theorem, IEEE Trans. Inf. Theory 48 (2002) 2637
2002
-
[16]
C. H. Bennett, I. Devetak, A. W. Harrow, P. W. Shor, A. Winter, The quantum reverse shannon theorem and resource tradeoffs for simulating quantum channels, IEEE Trans. Inf. Theory 60 (2014) 2926
2014
-
[17]
Devetak, A
I. Devetak, A. W. Harrow, A. Winter, A resource frame- work for quantum Shannon theory, IEEE Trans. Inf. The- ory 54 (2008) 4587–4618
2008
-
[18]
Abeyesinghe, I
A. Abeyesinghe, I. Devetak, P. Hayden, A. Winter, The mother of all protocols: Restructuring quantum informa- tion’s family tree, Proc. R. Soc. A 465 (2009) 2537–2563
2009
-
[19]
Devetak, A
I. Devetak, A. W. Harrow, A. Winter, A family of quan- tum protocols, Phys. Rev. Lett. 93 (2004) 230504
2004
-
[20]
Datta, M.-H
N. Datta, M.-H. Hsieh, The apex of the family tree of protocols: optimal rates and resource inequalities, New J. Phys. 13 (2011) 093042
2011
-
[21]
Wang, State-adaptive quantum error correction and fault-tolerant quantum computing, Phys
D.-S. Wang, State-adaptive quantum error correction and fault-tolerant quantum computing, Phys. Rev. A 113 (2026) 012438
2026
-
[22]
Csisz´ ar, J
I. Csisz´ ar, J. K¨ orner, Information Theory: Coding The- orems for Discrete Memoryless Systems, 2nd Edition, Cambridge University Press, 2011
2011
-
[23]
Z. Luo, I. Devetak, Channel simulation with quantum side information, arXiv preprint arXiv:0611008 (2006)
2006
-
[24]
Devetak, J
I. Devetak, J. Yard, Exact cost of redistributing mul- tipartite quantum states, Phys. Rev. Lett. 100 (2008) 230501
2008
-
[25]
J. Yard, I. Devetak, Optimal quantum source coding with quantum side information at the encoder and decoder, IEEE Trans. Inf. Theory 55 (2009) 5339–5351
2009
-
[26]
J. Oppenheim, State redistribution as merging: introduc- ing the coherent relay, arXiv preprint arXiv:0805.1065 (2008)
Pith/arXiv arXiv 2008
-
[27]
Datta, M.-H
N. Datta, M.-H. Hsieh, J. Oppenheim, An upper bound on the second order asymptotic expansion for the quan- tum communication cost of state redistribution, J. Math. Phys. 57 (2016) 052203
2016
-
[28]
Ye, Y.-K
M.-Y. Ye, Y.-K. Bai, Z. D. Wang, Quantum state redis- tribution based on a generalized decoupling, Phys. Rev. A 78 (2008) 030302(R)
2008
-
[29]
J. Yard, P. Hayden, I. Devetak, Quantum broadcast channels, IEEE Trans. Inf. Theory 57 (2011) 7147–7162
2011
-
[30]
Pastawski, J
F. Pastawski, J. Eisert, H. Wilming, Towards holography via quantum source-channel codes, Phys. Rev. Lett. 119 (2017) 020501
2017
-
[31]
Berta, F
M. Berta, F. G. S. L. Brand˜ ao, C. Majenz, M. M. Wilde, Conditional decoupling of quantum information, Phys. Rev. Lett. 121 (2018) 040504
2018
-
[32]
U. Pereg, Entanglement-assisted capacity of quan- tum channels with side information, arXiv preprint arXiv:1909.09992 (2019)
arXiv 1909
-
[33]
Briegel, W
H.-J. Briegel, W. D¨ ur, J. I. Cirac, P. Zoller, Quantum repeaters: the role of imperfect local operations in quan- tum communication, Phys. Rev. Lett. 81 (1998) 5932
1998
-
[34]
Ahlswede, I
R. Ahlswede, I. Csisz´ ar, Common randomness in infor- mation theory and cryptography. I. Secret sharing, IEEE Trans. Inf. Theory 39 (1993) 1121–1132
1993
-
[35]
Ahlswede, I
R. Ahlswede, I. Csisz´ ar, Common randomness in infor- mation theory and cryptography. II. CR capacity, IEEE Trans. Inf. Theory 44 (1998) 225–240
1998
-
[36]
A. D. Wyner, The wire-tap channel, Bell Syst. Tech. J. 54 (1975) 1355–1387
1975
-
[37]
Hayden, R
P. Hayden, R. Jozsa, D. Petz, A. Winter, Structure of states which satisfy strong subadditivity of quantum en- tropy with equality, Commun. Math. Phys. 246 (2004) 359–374
2004
-
[38]
Petz, Sufficient subalgebras and the relative entropy of states of a von neumann algebra, Commun
D. Petz, Sufficient subalgebras and the relative entropy of states of a von neumann algebra, Commun. Math. Phys. 105 (1986) 123–131
1986
-
[39]
M. Ohya, D. Petz, Quantum entropy and its use, Springer-Verlag, Berlin, Heidelberg, 1993
1993
-
[40]
K. P. Seshadreesan, M. M. Wilde, Fidelity of recovery, squashed entanglement, and measurement recoverability, Phys. Rev. A 92 (2015) 042321
2015
-
[41]
J. A. Smolin, F. Verstraete, A. Winter, Entanglement of assistance and multipartite state distillation, Phys. Rev. A 72 (2005) 052317
2005
-
[42]
Winter, On environment-assisted capacities of quan- tum channels, Markov Proc
A. Winter, On environment-assisted capacities of quan- tum channels, Markov Proc. Rel. Fields 13 (1-2) (2007) 297–314
2007
-
[43]
B. M. Terhal, Is entanglement monogamous?, IBM J. Res. Dev. 48 (2004) 71
2004
-
[44]
K. Li, A. Winter, X. Zou, G. Guo, Private capacity of quantum channels is not additive, Phys. Rev. Lett. 103 (2009) 120501
2009
-
[45]
Squashed entanglement
M. Christandl, A. Winter, “Squashed entanglement”: an additive entanglement measure , J. Math. Phys. 45 (2004) 829
2004
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