Shared Randomness and Normalization in One-Use Loop Communication
Version 1 / Nov 02, 2026 / CC BY 4.0
Abstract
We study a finite-message communication model defined by contracting one backward binary symmetric channel with one fixed, finite-dimensional forward quantum channel and then normalizing the resulting weights. The devices may share a finite classical seed that is independent of the message before normalization. The seed branches are mixed at the level of unnormalized weights, followed by a single normalization for each message. For M ≥ 2 messages, backward crossover probability 0 < p < 1/2, and forward channel Φ, we derive the exact worst-message success probability S_raw(Φ,p,M) = 2(1−p)/[M−(M−2)(1−2p)δ(Φ)], where δ(Φ) = max over input states ρ, σ of ½‖Φ(ρ)−Φ(σ)‖₁. The quantity δ is the established trace-distance contraction coefficient, not a new channel invariant. A cyclic construction with M seed values attains the bound. Crucially, normalization can make the posterior seed distribution message-dependent: the theorem does not describe an average of separately normalized branches or require success for every seed. We give an exact example separating these conventions. Matched depolarizing-qubit and classical binary symmetric forward channels consequently have equal optima in this resource model. The result is a restricted one-use optimization, not a physical backward-communication protocol or a general asymptotic capacity theorem.
Provenance statement
Tools used
- OpenAI
- Lyra (OpenAI AI assistant); Python 3 with NumPy and SymPy; LaTeX/pdfLaTeX.
References
- K. Ji, S. Lloyd, and M. M. Wilde, ``Retrocausal capacity of a quantum channel: Communicating through noisy closed timelike curves,'' Physical Review Letters 136 , 230801 (2026). doi:10.1103/znyd-npk5 (https://doi.org/10.1103/znyd-npk5). arXiv:2509.08965v3 (https://arxiv.org/abs/2509.08965v3).arXivDOI
- K. Ji, B. Regula, and M. M. Wilde, ``Postselected communication over quantum channels,'' International Journal of Quantum Information 22 (5), 2440012 (2024). doi:10.1142/S0219749924400124 (https://doi.org/10.1142/S0219749924400124). arXiv:2308.02583v3 (https://arxiv.org/abs/2308.02583v3).arXivDOI
- O. Fawzi, A. Müller-Hermes, and A. Shayeghi, ``A lower bound on the space overhead of fault-tolerant quantum computation,'' in 13th Innovations in Theoretical Computer Science Conference (ITCS 2022) , LIPIcs 215 , 68:1--68:20 (Schloss Dagstuhl, 2022). doi:10.4230/LIPIcs.ITCS.2022.68 (https://doi.org/10.4230/LIPIcs.ITCS.2022.68).DOI
- F. Hiai and M. B. Ruskai, ``Contraction coefficients for noisy quantum channels,'' Journal of Mathematical Physics 57 (1), 015211 (2016). doi:10.1063/1.4936215 (https://doi.org/10.1063/1.4936215).DOI
- E. Chitambar, I. George, B. Doolittle, and M. Junge, ``The communication value of a quantum channel,'' IEEE Transactions on Information Theory 69 (3), 1660--1679 (2023). doi:10.1109/TIT.2022.3218540 (https://doi.org/10.1109/TIT.2022.3218540).DOI
- P. E. Frenkel and M. Weiner, ``Classical information storage in an -level quantum system,'' Communications in Mathematical Physics 340 (2), 563--574 (2015). doi:10.1007/s00220-015-2463-0 (https://doi.org/10.1007/s00220-015-2463-0).DOI
- J. Bowles, M. T. Quintino, and N. Brunner, ``Certifying the dimension of classical and quantum systems in a prepare-and-measure scenario with independent devices,'' Physical Review Letters 112 , 140407 (2014). doi:10.1103/PhysRevLett.112.140407 (https://doi.org/10.1103/PhysRevLett.112.140407).DOI
Version history
- v1 · 10 pagesSubmitted by Daniel Adam PyleInitial depositCurrentOct 31, 2026