Nash Equilibrium from Quantum-Field Entanglement

arXiv:2609.33188 · quant-ph, gr-qc, hep-th · Submitted 2026-09-27 · Read on arXiv

quant-ph, gr-qc, hep-th

Submitted: 2026-09-27

Updated: 2026-09-27

Comments: 28 pages

License: http://creativecommons.org/licenses/by/4.0/

The gist: Entanglement harvesting transfers quantum field correlations to localized probes, yet whether these correlations can alter stable strategic behavior has remained unclear.

Terminology

Abstract

Entanglement harvesting transfers quantum field correlations to localized probes, yet whether these correlations can alter stable strategic behavior has remained unclear. We formulate a quantum-input game in which two Unruh-DeWitt detectors harvest vacuum entanglement from a free massless scalar field in (3+1) -dimensional Minkowski spacetime. A referee converts this state into payoffs using independent question qubits and phase-calibrated local Bell measurements. To leading perturbative order, the mean reward is proportional to the signed entanglement margin sqrt H 2+ Q 2-P, where H is the Hadamard correlation contribution, Q is the Pauli-Jordan causal contribution, and P is the local excitation noise. Away from payoff degeneracies, allowing each player to exit or to choose an early or late interaction yields 1+2n+ trembling-hand perfect equilibria, where n+ counts the positive-reward timing equilibria. For one fixed protocol, five analytically certified settings realize the sequence 7 to3 to1 to7 to1. They represent the spacelike region, the first commutator lobe, central carrier cancellation, the second lobe, and the post-wavefront Huygens regime. Thus, within this fixed quantum-input verification protocol, distinct field-correlation regimes generate different stable strategic structures.

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