Information Dynamics provides a novel response to the Einstein-Bohr debate: quantum nonlocality is not superluminal signaling, but rather the projection of global coherence in virtual space; no parallel universes are required—measurement is merely a unidirectional projection from the virtual to the real component of information; the geometric constant 0.25 in Bell inequality violations originates from the intrinsic curvature of the two-dimensional virtual space (SU(2)). The violation of the Clauser-Horne (CH) inequality is a core result in the experimental verification of Bell's theorem. In 2025, the BESIII experiment measured the CHSH parameter S = 2.800 ± 0.010 for entangled ΛΛ¯ pairs with exceptional precision, unambiguously violating classical local realism. Within the Information Dynamics framework, we treat quantum systems as Information Superconductors—featuring global coherence in virtual space, information conservation, and a dynamic real-virtual coupling matrix K(x). Starting from two primitive axioms, we rigorously prove that virtual space possesses constant curvature K = 1/4, from which we derive in a unified manner: The Tsirelson bound for the CH inequality: (√2−1)/2 ≈ 0.2071 (projection of one-dimensional geodesic arc length); The quantum upper bound for the I3322 inequality: 0.25 (projection of two-dimensional spherical area). More importantly, we propose a novel testable prediction: for partially entangled pure states, the Information Dynamics prediction for the CH violation, S^ID_CH(η) = (√(1+sin 2η)−1)/2, is systematically larger than the standard quantum mechanical prediction, S^QM_CH(η) = (√(1+sin² 2η)−1)/2, with the two converging only at maximal entanglement. Taking η=30° as an example, the relative deviation exceeds 13%, well within the resolution of current photonic entanglement experiments, thereby providing a direct falsification pathway for Information Dynamics. First-Principles Numerical Verification: We further perform first-principles numerical simulations starting from the generalized Ginzburg-Landau equation, using FFT spectral methods on 2D lattices (up to 128×128). The results show that in the information superconducting phase (ρ_target ≳ 0.85), the effective curvature K_eff(C) ∝ C emerges naturally from the dynamics with ΔAIC = -5.67 and 91% Monte Carlo support, and the fitted exponent α = 1.02 ± 0.06, in excellent agreement with the geometric prediction α = 1. A quick version (64×64, 10 seeds, running in ~25 seconds on a personal computer) also strongly favors the linear model (ΔAIC < -60) across all tested parameter sets. These results provide strong first-principles numerical support for the linear projection hypothesis of Information Dynamics. This work not only answers "why" the geometric scale is 0.25, but also elevates imaginary space from a mathematical tool to a physical entity with measurable curvature, offering a new information-theoretic perspective on the century-old Einstein-Bohr debate.
Information Dynamics provides a novel response to the Einstein-Bohr debate: quantum nonlocality is not superluminal signaling, but rather the projection of global coherence in virtual space; no parallel universes are required—measurement is merely a unidirectional projection from the virtual to the real component of information; the geometric constant 0.25 in Bell inequality violations originates from the intrinsic curvature of the two-dimensional virtual space (SU(2)). The violation of the Clauser-Horne (CH) inequality is a core result in the experimental verification of Bell's theorem. In 2025, the BESIII experiment measured the CHSH parameter S = 2.800 ± 0.010 for entangled ΛΛ¯ pairs with exceptional precision, unambiguously violating classical local realism. Within the Information Dynamics framework, we treat quantum systems as Information Superconductors—featuring global coherence in virtual space, information conservation, and a dynamic real-virtual coupling matrix K(x). Starting from two primitive axioms, we rigorously prove that virtual space possesses constant curvature K = 1/4, from which we derive in a unified manner: The Tsirelson bound for the CH inequality: (√2−1)/2 ≈ 0.2071 (projection of one-dimensional geodesic arc length); The quantum upper bound for the I3322 inequality: 0.25 (projection of two-dimensional spherical area). More importantly, we propose a novel testable prediction: for partially entangled pure states, the Information Dynamics prediction for the CH violation, S^ID_CH(η) = (√(1+sin 2η)−1)/2, is systematically larger than the standard quantum mechanical prediction, S^QM_CH(η) = (√(1+sin² 2η)−1)/2, with the two converging only at maximal entanglement. Taking η=30° as an example, the relative deviation exceeds 13%, well within the resolution of current photonic entanglement experiments, thereby providing a direct falsification pathway for Information Dynamics. First-Principles Numerical Verification: We further perform first-principles numerical simulations starting from the generalized Ginzburg-Landau equation, using FFT spectral methods on 2D lattices (up to 128×128). The results show that in the information superconducting phase (ρ_target ≳ 0.85), the effective curvature K_eff(C) ∝ C emerges naturally from the dynamics with ΔAIC = -5.67 and 91% Monte Carlo support, and the fitted exponent α = 1.02 ± 0.06, in excellent agreement with the geometric prediction α = 1. A quick version (64×64, 10 seeds, running in ~25 seconds on a personal computer) also strongly favors the linear model (ΔAIC < -60) across all tested parameter sets. These results provide strong first-principles numerical support for the linear projection hypothesis of Information Dynamics. This work not only answers "why" the geometric scale is 0.25, but also elevates imaginary space from a mathematical tool to a physical entity with measurable curvature, offering a new information-theoretic perspective on the century-old Einstein-Bohr debate.
In 1964, John Bell showed that any local hidden‑variable theory must satisfy a specific inequality on correlations between distant measurements. In its CHSH form (Clauser, Horne, Shimony, Holt 1969), the inequality reads |S| = |E(a,b) + E(a,b′) + E(a′,b) − E(a′,b′)| ≤ 2, where E(a,b) is the correlation between measurement outcomes at two separated parties using settings a and b. Any local realist theory respects this bound. Quantum mechanics violates it. Experiments confirm the violation. The standard quantum prediction for a maximally entangled state with optimal measurement angles is |S| = 2√2 ≈ 2.828. In 1980, Boris Tsirelson proved that 2√2 is not just one quantum prediction — it is the *maximum* value any quantum correlation can produce. No quantum state, no measurement scheme, no clever protocol can push |S| beyond 2√2. The bound is sharp, the value is exact, and it has been measured in laboratories around the world to experimental precision. The Tsirelson bound is one of the deepest empirical structures in physics. It tells us that quantum correlations exceed classical correlations by a specific, finite amount — there is room to violate Bell’s inequality, but only so much room. The number 2√2 has no obvious physical interpretation. It does not appear in the formulation of quantum mechanics. It emerges from the mathematics of the bipartite Hilbert space when the CHSH operator is constructed and bounded. The question is where it comes from. In standard QM, the answer is that it falls out of the Hilbert‑space structure plus Cauchy–Schwarz plus an operator‑norm bound on the CHSH operator. Technically correct, and Tsirelson’s 1980 proof remains the canonical derivation — but it leaves the deeper structure unanswered. The Hilbert space is postulated. The inner product that makes Cauchy–Schwarz available is postulated. The bipartite tensor‑product structure on H_A ⊗ H_B is postulated. The 2√2 value is what those postulates produce when run through the CHSH operator. This walkthrough shows how the Event Density framework derives the Tsirelson bound from a smaller set of structural commitments. The Hilbert‑space structure, the inner product, and the bipartite tensor‑product structure all emerge as forced consequences of the substrate ontology rather than being postulated. With those structures forced rather than assumed, Tsirelson’s 1980 argument applies directly, and the 2√2 value is no longer the output of a chain of postulates but the output of a chain of derived theorems. Like Heisenberg, Bell–Tsirelson is a place where the framework’s contribution is upstream. The bound itself is mathematical physics already in the literature; what changes is the foundational status of the structures the argument requires. ED does not produce a new derivation step beyond standard QM here — it removes the postulational status of the structures the standard derivation already uses. The 2√2 value is now a derived consequence of the substrate ontology, all the way down.
We derive the Bell–CHSH inequality as a conditional theorem inside Charlton Geometry (CG), rather than as an independent axiom about “local realism”. The key CG primitive is non-invertibility, η(ω) = η(−ω), which forces an observational quotient and produces irrecoverable “lost state” carried by polarity and intrinsic phase. In a bipartite experiment, Bell’s bound is recovered exactly when one adds an additional factorization condition asserting that outcomes depend only on local settings and a local lift choice, i.e. that the lost-state fiber decomposes into independent local fibers. Within CG, the natural geometric coupling of two regions through shared lift and holonomy generically violates that factorization while preserving operational no-signaling, so the Bell inequality becomes a theorem about a restricted subclass of quotients rather than a universal constraint. Using the Born brick as an upstream theorem that fixes the unique binary law cos2(θ/2) on the spin-lifted setting space, we recover the standard singlet correlation E(a, b) = −a °§ b and the Tsirelson bound 2√2 as the sharp CG-compatible CHSH maximum. In this framing, Bell violation is not an ontic miracle but the expected signature of a globally shared, non-invertible geometric substate whose reversal cannot be represented Original DOI: 10.5281/zenodo.18216032 Version: 0.9.0
Abstract: Quantum entanglement and Bell inequality violation are regarded as the most iconic non-classical phenomena in quantum mechanics, yet their physical origin remains mysterious. Within Space Ontology, we demonstrate that the nonlocal correlations between an EPR pair are not due to "spooky action at a distance," but are a natural manifestation of the intrinsic geometric correlations between two identical spatial modes generated by the same disturbance. We introduce the effective shape parameter alpha_eff and the geometric entanglement entropy E_geo, and derive from first principles the analytic relation between the CHSH polynomial S and E_geo: S = 2√2 · tanh(2E_geo(alpha_eff)). The classical limit (E_geo → 0) recovers Bell's inequality (S ≤ 2), while the quantum limit (E_geo → ∞) yields the maximum violation S = 2√2. By direct comparison with authoritative data from loophole-free Bell experiments, high-dimensional orbital angular momentum entanglement experiments, and the Micius satellite entanglement distribution experiment, the theoretical predictions are in excellent agreement with experimental observations — with typical deviations below 3% and no free parameters. We further propose schemes for actively designing entanglement resources by controlling the shape parameter of spatial modes, providing a new physical dimension for quantum communication and quantum computation. This work demonstrates that quantum nonlocality can be completely reduced to space geometry — twin ripples are telepathic because they share the same initial texture from the same spatial disturbance. This paper is the third in the first series (17 papers total) of Space Ontology.
We derive the Bell–CHSH inequality as a conditional theorem inside Charlton Geometry (CG), rather than as an independent axiom about “local realism”. The key CG primitive is non-invertibility, η(ω) = η(−ω), which forces an observational quotient and produces irrecoverable “lost state” carried by polarity and intrinsic phase. In a bipartite experiment, Bell’s bound is recovered exactly when one adds an additional factorization condition asserting that outcomes depend only on local settings and a local lift choice, i.e. that the lost-state fiber decomposes into independent local fibers. Within CG, the natural geometric coupling of two regions through shared lift and holonomy generically violates that factorization while preserving operational no-signaling, so the Bell inequality becomes a theorem about a restricted subclass of quotients rather than a universal constraint. Using the Born brick as an upstream theorem that fixes the unique binary law cos2(θ/2) on the spin-lifted setting space, we recover the standard singlet correlation E(a, b) = −a °§ b and the Tsirelson bound 2√2 as the sharp CG-compatible CHSH maximum. In this framing, Bell violation is not an ontic miracle but the expected signature of a globally shared, non-invertible geometric substate whose reversal cannot be represented
We report the experimental demonstration of Bell violations reaching S = 4.0000, exceeding the Tsirelson bound of S ≤ 2√2 ≈ 2.828. Using curved geometric quantum theory with fundamental curvature parameter κ = 0.893469101829281, we observe universal super-quantum correlations across all tested scales (0.1 to 2.0). The quantum-classical boundary occurs at κ_quantum = 1/(2κ) = 0.559616442220894, which emerges as a new fundamental constant separating classical from quantum behavior. All quantum states reside on the π/2 = 1.570796 geometric horizon. This discovery demonstrates that super-quantum correlations are physically possible and suggests that standard quantum mechanics is a limiting case of a more general geometric theory. We present the first theoretical demonstration of Bell parameter S=4.0, achieving the PR-box limit previously considered unattainable in physical systems. Using a curved geometric quantum framework with fundamental curvature constant κ=0.893469101829281, we identify a critical scale parameter α_c=0.560 at which quantum correlations exceed the Tsirelson bound S≤2√2≈2.828. Our 4+4 paired qubit architecture exhibits deterministic correlations that saturate the maximum possible Bell violation, enabling super-quantum computation with O(N¹/³) search complexity. Experimental verification is immediately feasible with current quantum technology
Tsirelson's bound is the upper bound for a Bell inequality which is valid for all quantum mechanical systems. We discuss why Tsirelson's bound was developed by looking at some historical arguments in quantum physics, such as the Einstein-Podolsky-Rosen (EPR) paradox, an argument for the quantum mechanical description of physical reality being incomplete, and local hidden variables. We present the counterargument to those theories, Bell's inequality, which later expanded to include any inequality that a local system fulfills, but that an entangled quantum system can violate. We present the proof of two specific Bell inequalities: the Clauser-Horne-Shimony-Holt (CHSH) inequality and the I3322 inequality. Then the Tsirelson's bound for the CHSH inequality is proven with a simple system of two entangled spin-1/2 particles and with a general argument that is valid for all entangled systems. We give the upper quantum bound for the generalized CHSH inequality, which describes the situation that we have more than two measurement options, by using semidefinite programming. We prove the Tsirelson's bound for the I3322 inequality by using maximally entangled systems and semidefinite programming. Finally, we discuss the upper bounds that are obtained from these different methods.