Finite classical-communication simulation problem for quantum communication and Bell nonlocality
For each integer , determine whether there exists a classical protocol using a finite amount of classical communication and unlimited shared randomness that exactly reproduces both (i) the statistics of arbitrary -dimensional quantum communication and (ii) all correlations obtainable from measurements on two entangled -dimensional quantum systems. When such protocols exist, determine the required communication cost; when they do not, prove that no finite classical communication suffices.
References
Primary source
Additional references
Progress summary
A September preprint claims finite classical simulations exist through qutrits but are impossible from four dimensions onward, yet nobody has independently verified the result.
Known results
- Toner and Bacon (2003) gave a one-bit protocol for the singlet correlation, a restricted two-qubit case.
- Regev and Toner (2009) gave a two-bit simulation for two-outcome measurements on shared bipartite -dimensional states.
- Earlier work reported lower bounds of messages for qutrit communication and for ququart communication, with finite upper bounds unknown.
September 3, 2026 claimed classification
Carlos de Gois, Thyago S. R. Santos, and Carlos Vieira claim that classical bits exactly simulate qubit communication and all entangled-qubit correlations, that qutrits admit an explicit -bit protocol, and that no finite protocol exists for either task when . The arXiv preprint is unrefereed and has no independent verification.
Community submission (unverified)
A submitted proof argues for the same qutrit/ququart transition, reducing impossibility to a fidelity kernel on complex projective space and a zero-slope property at zero fidelity; it presents the -bit figure as an upper bound, not an optimum. Its analytic ingredients are explicitly left source-dependent.
Current status (as of September 2026): the claimed -bit qubit result and -bit qutrit protocol are reported, while impossibility for and the full classification remain unverified.
Sources
- cqi.inf.usi.ch
- arxiv.org
- arxiv.org
- quantum-journal.org
- homepages.cwi.nl
- inspirehep.net
- dst.gov.in
- rintonpress.com
- quantamagazine.org
- scientificamerican.com
- arxiv.org
- ar5iv.labs.arxiv.org
- ar5iv.labs.arxiv.org
- arxiv.org
- mathstodon.xyz
- quantamagazine.org
- quantamagazine.org
- mathstodon.xyz
- quantamagazine.org
- inspirehep.net
- repository.tudelft.nl
- link.aps.org
- access.archive-ouverte.unige.ch
- quantamagazine.org
- quantamagazine.org
- quantamagazine.org
- arxiv.org
- arxiv.org
- www-cdn.anthropic.com
- quantamagazine.org
- scientificamerican.com
Solutions 1
ProofFinite Classical-Communication Simulation of Quantum Communication and Bell Nonlocality DR. ARIE-ARIADNE DEWATSON A proof-oriented reconstruction and audit of the dimensional classification claimed in arXiv:2609.04182v1See full solution
We study exact simulation of finite-dimensional quantum communication and bipartite quantum correlations by classical protocols with unlimited shared randomness and a finite classical communication alphabet. The classification claimed in arXiv:2609.04182v1 exhibits a sharp transition between qutrits and ququarts. Qubit communication and qubit Bell correlations admit exact finite simulations; an explicit qutrit construction uses fewer than 2^357 messages, hence at most 357 bits in a fixed-length encoding; whereas no finite exact classical simulation is claimed for any dimension d >= 4. The impossibility argument reduces the problem to the fidelity kernel on complex projective space, uses fixed-fidelity averaging and a projective-harmonic spectral decomposition, and derives a zero-slope property at zero fidelity. The latter contradicts the quantum kernel K(t)=t. We also explain the reduction to Bell correlations.
This manuscript is a source-faithful reconstruction of the supplied audit and the cited preprint. In particular, the 357-bit figure is an explicit upper bound, not an optimality claim. The higher-order level-set step and the cited auxiliary analytic/geometric results should be regarded as source-dependent ingredients unless independently verified from their original references.