Bounding Two-Way Average Communication Cost of Simulating Quantum Correlations
quant-ph
Submitted: 2026-10-03
Updated: 2026-10-03
Comments: 10+10 pages, 2 figures, 2 tables; Comments are welcome!
License: http://creativecommons.org/licenses/by/4.0/
The gist: Bell nonlocal correlations cannot be reproduced by local hidden-variable models without communication, making classical communication cost a natural quantitative measure of nonlocality.
Abstract
Bell nonlocal correlations cannot be reproduced by local hidden-variable models without communication, making classical communication cost a natural quantitative measure of nonlocality. Although finite communication always suffices to simulate any correlation in a fixed finite Bell scenario, determining the minimum amount needed to (exactly) simulate any given nonlocal correlation remains challenging, especially in the average-cost setting. Here, we derive lower bounds on input-average communication cost from nonlocal games, allowing variable-length, fully interactive two-way protocols. When applied to parallel games, these bounds yield explicit finite quantum correlations for which the exact simulation cost exceeds any prescribed finite input-average communication budget. For n parallel Magic-Square-winning correlations, we prove a lower bound of n 2(3/2) bits and give a one-way communication protocol that attains this rate asymptotically. For the quantum correlation maximally winning the n-copy of the Clauser--Horne--Shimony--Holt nonlocal game, we obtain an input-average lower bound of approximately 0.04627n bits for exact simulation. Finally, we formulate a hierarchy of lower bounds and complementary upper bounds using deterministic correlations up to chosen communication costs. Both recover the exact input-average cost at their final levels, and if the bounds agree at lower levels, their common value yields the exact input-average cost without needing to consider all communication strategies.
Sources
- Can outcome communication explain Bell nonlocality?
- Maximum Separation of Quantum Communication Complexity With and Without Shared Entanglement
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