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arXiv:2603.28973

Bell's Inequality, Causal Bounds, and Quantum Bayesian Computation: A Unified Framework

Nick Polson, Vadim Sokolov, Daniel Zantedeschi

quant-phstat.COSubmitted Mar 30, 2026• Announced Apr 1, 2026• 0 citations
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Abstract

Bell inequalities characterize the boundary of the local-realist correlation polytope -- the set of joint probability distributions achievable by classical hidden-variable models. Quantum mechanics exceeds this boundary through non-commutativity, reaching the Tsirelson bound $2\sqrt{2}$ for CHSH. We show that this polytope structure is not specific to quantum foundations: it appears identically in the causal inference literature, where the instrumental inequality, the Balke--Pearl linear programming bounds, and the Tian--Pearl probabilities of causation all arise as facets of the same marginal compatibility polytope. Fine's theorem -- that CHSH inequalities hold if and only if a joint distribution exists -- is precisely the pivot: the instrumental variable model in causal inference is structurally equivalent to the Bell local hidden-variable model, with the instrument playing the role of the measurement setting and the latent confounder playing the role of the hidden variable $λ$. We develop this correspondence in detail, extending it to algorithmic (Kolmogorov complexity) and entropic formulations of Bell inequalities, the NPA semidefinite programming hierarchy, and the MIP$^*$=RE undecidability result. We further show that the Born-rule / Bayes-rule duality underlying quantum Bayesian computation exploits the same non-commutativity that enables Bell violation, providing polynomial speedups for posterior inference. The framework yields a concrete dictionary between quantum information theory, causal econometrics, and Bayesian computation, and suggests new directions including NPA-based quantum causal inference algorithms and quantum architectures for function approximation.

Related papers

A violation of the Tsirelson bound in the pre-quantum theory of trace dynamics

Rabsan Galib Ahmed, Singh, Tejinder P.

The term Bell's theorem refers to a set of closely related results which imply that quantum mechanics is incompatible with local hidden variable theories. Bell's inequality is the statement that if measurements are performed independently on two space-like separated particles of an entangled pair, the assumption that outcomes depend on hidden variables implies an upper bound on the correlations between the outcomes. Quantum mechanics predicts correlations which violate this upper bound. The CHSH inequality is a specific Bell inequality in which classical correlation (i.e. if local hidden variables exist) can take the maximum value of 2. Quantum mechanics violates this bound, allowing for a higher bound on the correlation, which can take the maximum value $2\sqrt{2}$, known as the Tsirelson bound. Popescu and Rohrlich showed that the assumption of relativistic causality allows for an even higher bound on the CHSH correlation, this value being 4. Why is the bound coming from causality higher than the Tsirelson bound? Are there relativistic causal dynamical theories which violate the Tsirelson bound? In the present paper we answer this question in the affirmative. We show that the pre-quantum theory of trace dynamics, from which quantum theory is emergent as a thermodynamic approximation, permits the CHSH correlation to take values higher than $2\sqrt{2}$. We interpret our findings to suggest that quantum theory is approximate, and emergent from the more general theory of trace dynamics.

arXiv:2208.02209•Aug 3, 2022•8 citations

CHSH Inequalities as Unified Rules Linking Entanglement to Device-Independent Tests — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Bell/CHSH inequalities define the boundary between local-hidden-variable (classical) and quantum correlations; recent work (Buscemi) recasts them as a unified family of "rules" linking entanglement to device-independent tests. | MATH: CHSH form S = E(a,b) − E(a,b′) + E(a′,b) + E(a′,b′) ≤ 2 (LHV bound); quantum (Tsirelson) bound S_max = 2√2 ≈ 2.828. Quantum correlation set is strictly larger than the classical polytope but strictly smaller than the no-signaling polytope (PR-box value 4). | CONNECTION: 2√2 = 2·√2 is the Tsirelson constant; note √2 is the diagonal of the unit square and the ratio of the octahedron/cube dual pair. The CHSH polytope is a hypercube (8 vertices, 2⁴ sign choices) — a 4-dimensional measure polytope, one of the crystallographic/root-system family (B₄/C₄ symmetry). The classical bound 2 and quantum bound 2√2 differ by factor √2 ≈ 1.414, not a Fibonacci/φ ratio. No 0.618/1.618 structure appears in the inequality itself. | DEPTH: 7 Notes on the other item Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Oct 26, 2026•0 citations

Unifying Bell Inequalities and Entanglement Witnesses via Correlation Polytope Geometry — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Buscemi's framework unifies Bell inequalities with entanglement witnesses via "semidefinite programming" and "facet structure" of correlation polytopes, showing quantum violations correspond to specific geometric facets. | MATH: Bell inequalities are linear inequalities over the correlation polytope \( \mathcal{P} \); quantum correlations form a convex set \( \mathcal{Q} \) strictly larger than \( \mathcal{P} \) (local hidden variable polytope). Buscemi's unification maps entanglement witnesses (Hermitian operators \( W \geq 0 \) with \( \mathrm{Tr}(W\rho) \geq 0 \) for separable \( \rho \)) to Bell-type inequalities via a "quantum channel" transformation. Key constants: the Tsirelson bound \( 2\sqrt{2} \) for CHSH, and the ratio \( 2\sqrt{2}/2 = \sqrt{2} \approx 1.414 \) (not a golden ratio, but a quadratic irrational). Facet structure: the polytope \( \mathcal{P} \) has facets defined by inequalities like \( \langle A_1B_1 \rangle + \langle A_1B_2 \rangle + \langle A_2B_1 \r Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Bell nonlocality and device-independent quantum information

Sachin .

Bell nonlocality is the experimentally testable incompatibility between quantum correlations and explanations based on local hidden variables. Its significance now extends beyond the foundations of quantum mechanics: a Bell-inequality violation can certify entanglement, randomness, measurement incompatibility, and cryptographic security without requiring a detailed model of the devices producing the observed data. This article develops the mathematical structure of Bell experiments and explains its role in device-independent quantum information. Conditional probability distributions are classified into local, quantum, and no-signalling sets; the Clauser-Horne-Shimony-Holt inequality is derived, and its classical, quantum, and algebraic limits are distinguished. Tsirelson’s bound is obtained from the CHSH operator, while Popescu-Rohrlich correlations demonstrate that no-signalling alone does not identify the quantum set. The relation between entanglement and nonlocality is examined through local entangled states, hidden nonlocality, and activation. Nonlocal games, semidefinite relaxations, self-testing, certified randomness, and device-independent quantum key distribution are treated as operational consequences of Bell violation. Particular attention is given to entropy accumulation, finite-data security, loophole-free experiments, and the limitations of device independence. Bell nonlocality emerges as both a foundational separation between classical and quantum causal models and a quantitative resource for cryptographic and informational tasks.

International Journal of Physics and Mathematics•Jan 1, 2026•0 citations

Beyond Qubits: Bell Violations as Structural Limits on Local Realism — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Bell inequality tests are being extended beyond standard qubit-pair setups — via Buscemi's unified framework and condensed-matter proposals — revealing that the violation is not merely a quantum artifact but a structural constraint on any local hidden-variable theory, with new bounds emerging from information-theoretic and geometric constraints. MATH: - Standard CHSH inequality: \( S = E(a,b) + E(a,b') + E(a',b) - E(a',b') \leq 2 \) (local hidden variables), quantum max \( S = 2\sqrt{2} \approx 2.828 \). - Ratio \( 2\sqrt{2}/2 = \sqrt{2} \approx 1.414 \) — not directly in golden set, but note \( \sqrt{2} \approx 1.414 \) and \( 1.618 \) are related via \( \phi = (1+\sqrt{5})/2 \), and \( \sqrt{2} \) appears in octahedral/cubic symmetry (root system \( B_3 \)). - Buscemi's unification: Bell inequalities as linear constraints on probability polytopes; violation corresponds to points outside the local polytope — the facet structure of these polytopes encodes all possible Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Sep 4, 2026•0 citations

Experimental Tests of Multiplicative Bell Inequalities

Dilip Paneru

This thesis is the synthesis of theoretical and experimental works performed in the area of quantum foundations, particularly on quantum correlations and experimental tests of multiplicative Bell inequalities. First we begin with a comprehensive theoretical work performed on the foundations of quantum mechanics, focusing on the puzzling concepts of quantum entanglement, and hidden variable theories. Specifically, we present a broad overview of different classes of hidden variable theories such as local, crypto-nonlocal, contextual and non-local theories, along with several Bell like inequalities for these theories, providing theoretical proofs based on quantum mechanics for the falsification of some of these theories. Second we present a body of experimental, and theoretical works performed on a new class of Bell inequalities, i.e., the multiplicative Bell inequalities. We experimentally report the observation of the Bell parameters close to the Tsirelson (quantum) limit, upto a large number of measurement devices $(n)$, and compare the results with a particular deterministic strategy. We also obtain classical bounds for some $n$, and report the experimental violation of these classical limits. We theoretically derive new richer bounds on the CHSH inequality (named after John Clauser, Michael Horne, Abnor Shimony and Richard Holt) and the multiplicative Bell parameter for $n=2$, based on the principle of ``relativistic independence'', and experimentally observe the distribution of Bell parameters as predicted by these bounds.

•Jan 7, 2021•0 citations
Bell inequalities characterize the boundary of the local-realist correlation polytope -- the set of joint probability distributions achievable by classical hidden-variable models. Quantum mechanics exceeds this boundary through non-commutativity, reaching the Tsirelson bound 222\sqrt{2}22​ for CHSH. We show that this polytope structure is not specific to quantum foundations: it appears identically in the causal inference literature, where the instrumental inequality, the Balke--Pearl linear programming bounds, and the Tian--Pearl probabilities of causation all arise as facets of the same marginal compatibility polytope. Fine's theorem -- that CHSH inequalities hold if and only if a joint distribution exists -- is precisely the pivot: the instrumental variable model in causal inference is structurally equivalent to the Bell local hidden-variable model, with the instrument playing the role of the measurement setting and the latent confounder playing the role of the hidden variable λλλ. We develop this correspondence in detail, extending it to algorithmic (Kolmogorov complexity) and entropic formulations of Bell inequalities, the NPA semidefinite programming hierarchy, and the MIP∗^*∗=RE undecidability result. We further show that the Born-rule / Bayes-rule duality underlying quantum Bayesian computation exploits the same non-commutativity that enables Bell violation, providing polynomial speedups for posterior inference. The framework yields a concrete dictionary between quantum information theory, causal econometrics, and Bayesian computation, and suggests new directions including NPA-based quantum causal inference algorithms and quantum architectures for function approximation.
The term Bell's theorem refers to a set of closely related results which imply that quantum mechanics is incompatible with local hidden variable theories. Bell's inequality is the statement that if measurements are performed independently on two space-like separated particles of an entangled pair, the assumption that outcomes depend on hidden variables implies an upper bound on the correlations between the outcomes. Quantum mechanics predicts correlations which violate this upper bound. The CHSH inequality is a specific Bell inequality in which classical correlation (i.e. if local hidden variables exist) can take the maximum value of 2. Quantum mechanics violates this bound, allowing for a higher bound on the correlation, which can take the maximum value 222\sqrt{2}22​, known as the Tsirelson bound. Popescu and Rohrlich showed that the assumption of relativistic causality allows for an even higher bound on the CHSH correlation, this value being 4. Why is the bound coming from causality higher than the Tsirelson bound? Are there relativistic causal dynamical theories which violate the Tsirelson bound? In the present paper we answer this question in the affirmative. We show that the pre-quantum theory of trace dynamics, from which quantum theory is emergent as a thermodynamic approximation, permits the CHSH correlation to take values higher than 222\sqrt{2}22​. We interpret our findings to suggest that quantum theory is approximate, and emergent from the more general theory of trace dynamics.
FINDING: Bell/CHSH inequalities define the boundary between local-hidden-variable (classical) and quantum correlations; recent work (Buscemi) recasts them as a unified family of "rules" linking entanglement to device-independent tests. | MATH: CHSH form S = E(a,b) − E(a,b′) + E(a′,b) + E(a′,b′) ≤ 2 (LHV bound); quantum (Tsirelson) bound S_max = 2√2 ≈ 2.828. Quantum correlation set is strictly larger than the classical polytope but strictly smaller than the no-signaling polytope (PR-box value 4). | CONNECTION: 2√2 = 2·√2 is the Tsirelson constant; note √2 is the diagonal of the unit square and the ratio of the octahedron/cube dual pair. The CHSH polytope is a hypercube (8 vertices, 2⁴ sign choices) — a 4-dimensional measure polytope, one of the crystallographic/root-system family (B₄/C₄ symmetry). The classical bound 2 and quantum bound 2√2 differ by factor √2 ≈ 1.414, not a Fibonacci/φ ratio. No 0.618/1.618 structure appears in the inequality itself. | DEPTH: 7 Notes on the other item Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Buscemi's framework unifies Bell inequalities with entanglement witnesses via "semidefinite programming" and "facet structure" of correlation polytopes, showing quantum violations correspond to specific geometric facets. | MATH: Bell inequalities are linear inequalities over the correlation polytope P \mathcal{P} P; quantum correlations form a convex set Q \mathcal{Q} Q strictly larger than P \mathcal{P} P (local hidden variable polytope). Buscemi's unification maps entanglement witnesses (Hermitian operators W≥0 W \geq 0 W≥0 with Tr(Wρ)≥0 \mathrm{Tr}(W\rho) \geq 0 Tr(Wρ)≥0 for separable ρ \rho ρ) to Bell-type inequalities via a "quantum channel" transformation. Key constants: the Tsirelson bound 22 2\sqrt{2} 22​ for CHSH, and the ratio 22/2=2≈1.414 2\sqrt{2}/2 = \sqrt{2} \approx 1.414 22​/2=2​≈1.414 (not a golden ratio, but a quadratic irrational). Facet structure: the polytope P \mathcal{P} P has facets defined by inequalities like \( \langle A_1B_1 \rangle + \langle A_1B_2 \rangle + \langle A_2B_1 \r Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
Bell nonlocality is the experimentally testable incompatibility between quantum correlations and explanations based on local hidden variables. Its significance now extends beyond the foundations of quantum mechanics: a Bell-inequality violation can certify entanglement, randomness, measurement incompatibility, and cryptographic security without requiring a detailed model of the devices producing the observed data. This article develops the mathematical structure of Bell experiments and explains its role in device-independent quantum information. Conditional probability distributions are classified into local, quantum, and no-signalling sets; the Clauser-Horne-Shimony-Holt inequality is derived, and its classical, quantum, and algebraic limits are distinguished. Tsirelson’s bound is obtained from the CHSH operator, while Popescu-Rohrlich correlations demonstrate that no-signalling alone does not identify the quantum set. The relation between entanglement and nonlocality is examined through local entangled states, hidden nonlocality, and activation. Nonlocal games, semidefinite relaxations, self-testing, certified randomness, and device-independent quantum key distribution are treated as operational consequences of Bell violation. Particular attention is given to entropy accumulation, finite-data security, loophole-free experiments, and the limitations of device independence. Bell nonlocality emerges as both a foundational separation between classical and quantum causal models and a quantitative resource for cryptographic and informational tasks.
FINDING: Bell inequality tests are being extended beyond standard qubit-pair setups — via Buscemi's unified framework and condensed-matter proposals — revealing that the violation is not merely a quantum artifact but a structural constraint on any local hidden-variable theory, with new bounds emerging from information-theoretic and geometric constraints. MATH: - Standard CHSH inequality: S=E(a,b)+E(a,b′)+E(a′,b)−E(a′,b′)≤2 S = E(a,b) + E(a,b') + E(a',b) - E(a',b') \leq 2 S=E(a,b)+E(a,b′)+E(a′,b)−E(a′,b′)≤2 (local hidden variables), quantum max S=22≈2.828 S = 2\sqrt{2} \approx 2.828 S=22​≈2.828. - Ratio 22/2=2≈1.414 2\sqrt{2}/2 = \sqrt{2} \approx 1.414 22​/2=2​≈1.414 — not directly in golden set, but note 2≈1.414 \sqrt{2} \approx 1.414 2​≈1.414 and 1.618 1.618 1.618 are related via ϕ=(1+5)/2 \phi = (1+\sqrt{5})/2 ϕ=(1+5​)/2, and 2 \sqrt{2} 2​ appears in octahedral/cubic symmetry (root system B3 B_3 B3​). - Buscemi's unification: Bell inequalities as linear constraints on probability polytopes; violation corresponds to points outside the local polytope — the facet structure of these polytopes encodes all possible Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
This thesis is the synthesis of theoretical and experimental works performed in the area of quantum foundations, particularly on quantum correlations and experimental tests of multiplicative Bell inequalities. First we begin with a comprehensive theoretical work performed on the foundations of quantum mechanics, focusing on the puzzling concepts of quantum entanglement, and hidden variable theories. Specifically, we present a broad overview of different classes of hidden variable theories such as local, crypto-nonlocal, contextual and non-local theories, along with several Bell like inequalities for these theories, providing theoretical proofs based on quantum mechanics for the falsification of some of these theories. Second we present a body of experimental, and theoretical works performed on a new class of Bell inequalities, i.e., the multiplicative Bell inequalities. We experimentally report the observation of the Bell parameters close to the Tsirelson (quantum) limit, upto a large number of measurement devices (n)(n)(n), and compare the results with a particular deterministic strategy. We also obtain classical bounds for some nnn, and report the experimental violation of these classical limits. We theoretically derive new richer bounds on the CHSH inequality (named after John Clauser, Michael Horne, Abnor Shimony and Richard Holt) and the multiplicative Bell parameter for n=2n=2n=2, based on the principle of ``relativistic independence'', and experimentally observe the distribution of Bell parameters as predicted by these bounds.