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This research establishes a rigorous mathematical trade-off between measurement dependence and detection efficiency in CHSH experiments, providing exact certificates for quantum correlations that challenge local hidden-variable models. By identifying a specific "moire phase-locking" mechanism that saturates these bounds, the study offers falsifiable predictions regarding fourfold coincidence sums that could distinguish quantum mechanics from surviving local accounts.
The exact price of local realism in CHSH experiments: a measurement-dependence-detection trade-off surface, a moir\'e phase-locking mechanism that saturates it, and an unmeasured fringe in the fourfold coincidence sum
arXiv:2608.18886v1 Announce Type: new Abstract: For local hidden-variable accounts of the CHSH experiment that are faithful -- reproducing the observed singles and coincidence rates and unbiased marginals of a polarization singlet with symmetric detector efficiency $\eta_{\rm eff}$ -- I determine the minimal measurement dependence $M$ (Hall's variational measure) needed to achieve a CHSH value $S$. Linear programming over all local strategies yields, to machine precision at 32 grid points, $M(S,\eta_{\rm eff})=\max\{0,\eta_{\rm eff}((S+2)\eta_{\rm eff}-4)/6\}$, whose edges reproduce Hall's tight bound at $\eta_{\rm eff}=1$, the Garg-Mermin detection threshold, and the postselection ceiling $S=4/\eta_{\rm eff}-2$. The quantum point is certified exactly: $M(2\sqrt{2},9/10)=(27\sqrt{2}-33)/100$, with primal and dual certificates in $\mathbb{Q}(\sqrt{2})$ arithmetic. I solve the unique detection profile $D(m)=\sqrt{m}\,h(m)$ under which a deterministic sign model reproduces the singlet exactly, derive the $\sqrt{m}$ edge law, and prove exact quantum correlations and angle-independent coincidence rates jointly impossible for any pure-detection model of this class. Surviving local accounts trade off measurement dependence against a $\cos 4(a-b)$ modulation of the fourfold coincidence sum, of relative amplitude up to 12.4%, which vanishes identically at the CHSH angles and appears never to have been bounded below 1%. A settings-torus protocol reaches $5\sigma$ sensitivity at 0.1% within hours: a flat result forces $M\gtrsim 95\%$ of Hall's floor; a fringe would contradict the flat-rate prediction of quantum mechanics. Finally I exhibit a local mechanism -- moire phase locking -- with deterministic phase evolution and all randomness quenched in frozen lattice offsets and flight times, which attains the certified floor exactly at $\eta_{\rm eff}=1$ (10% uniform fidelity); its softening of the correlation extremes is a falsifiable fingerprint.
Abstract:For local hidden-variable accounts of the CHSH experiment that are faithful -- reproducing the observed singles and coincidence rates and unbiased marginals of a polarization singlet with symmetric detector efficiency $\eta_{\rm eff}$ -- I determine the minimal measurement dependence $M$ (Hall's variational measure) needed to achieve a CHSH value $S$. Linear programming over all local strategies yields, to machine precision at 32 grid points, $M(S,\eta_{\rm eff})=\max\{0,\eta_{\rm eff}((S+2)\eta_{\rm eff}-4)/6\}$, whose edges reproduce Hall's tight bound at $\eta_{\rm eff}=1$, the Garg-Mermin detection threshold, and the postselection ceiling $S=4/\eta_{\rm eff}-2$. The quantum point is certified exactly: $M(2\sqrt{2},9/10)=(27\sqrt{2}-33)/100$, with primal and dual certificates in $\mathbb{Q}(\sqrt{2})$ arithmetic. I solve the unique detection profile $D(m)=\sqrt{m}\,h(m)$ under which a deterministic sign model reproduces the singlet exactly, derive the $\sqrt{m}$ edge law, and prove exact quantum correlations and angle-independent coincidence rates jointly impossible for any pure-detection model of this class. Surviving local accounts trade off measurement dependence against a $\cos 4(a-b)$ modulation of the fourfold coincidence sum, of relative amplitude up to 12.4%, which vanishes identically at the CHSH angles and appears never to have been bounded below 1%. A settings-torus protocol reaches $5\sigma$ sensitivity at 0.1% within hours: a flat result forces $M\gtrsim 95\%$ of Hall's floor; a fringe would contradict the flat-rate prediction of quantum mechanics. Finally I exhibit a local mechanism -- moire phase locking -- with deterministic phase evolution and all randomness quenched in frozen lattice offsets and flight times, which attains the certified floor exactly at $\eta_{\rm eff}=1$ (10% uniform fidelity); its softening of the correlation extremes is a falsifiable fingerprint.
10 pages, 5 figures. Code and exact certificates at this https URL
arXiv:2608.18886 [quant-ph]
(or arXiv:2608.18886v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2608.18886 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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