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Fractal Geometry of Quantum Correlation Space: Scale-Dependent Dimensionality, Long-Range Dependence, and Signatures in Time Delay Fluctuations

CHECHELNITSKY IGOR

Published Feb 15, 2026• 0 citations
Publisher

Abstract

We develop a metric-measure geometric reinterpretation of quantum entanglement in which nonlocal correlations are encoded in the intrinsic geometry of composite state space rather than in dynamical propagation. Using the Bures metric and CPTP coarse-graining semigroups, we define a scale-dependent effective dimension of the entangled-state manifold. We propose that geometric observables along the renormalization flow may exhibit long-range dependence (LRD) characterized by a Hurst exponent H ∈ (1/2,1). A conjectured infrared attractor H* ≈ 0.65 is formulated as a falsifiable hypothesis. The framework preserves no-signaling and does not modify quantum mechanics. A direct link to the variance (RMS) of Eisenbud–Wigner–Smith time delay is proposed, providing operational accessibility of geometric LRD effects.

DOI
10.5281/zenodo.18646758

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Geometric–Fractal Structure of Quantum Correlations and Time Delay: A Unified Metric–Measure Framework with Long-Range Dependence Scaling

CHECHELNITSKY IGOR

Overview This preprint develops a unified, mathematically self-contained geometric reinterpretation of quantum entanglement, in which nonlocal correlations arise from the intrinsic geometry of composite Hilbert space rather than from any dynamical propagation between subsystems. The framework is built on: the Bures metric, Quantum Fisher Information (QFI), and completely positive trace-preserving (CPTP) coarse-graining semigroups. This work constitutes the unified synthesis and mathematical completion of two companion preprints: DOI: 10.5281/zenodo.18646759 — Fractal Geometry of Quantum Correlation Space (geometric/LRD foundation) DOI: 10.5281/zenodo.18649326 — Geometric Control of Quantum Time Delay in Non-Smooth Regimes (EWS application) It closes all identified mathematical gaps in both documents and consolidates the results into a single publication-ready manuscript. 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C2 — Canonical Effective Dimension with Explicit Measure (§2, §4) We introduce a scale-dependent effective Bures dimension: D_{\mathrm{eff}}(\ell) = \lim_{\varepsilon \to 0} \frac{\log V(\varepsilon;\ell)}{\log \varepsilon} where is the volume of an -ball in the entangled-state manifold , measured using the canonical Bures volume measure: d\mu_\ell(\theta) = \sqrt{\det g^{\mathrm{B}}(\theta;\ell)}\; d\theta^1 \wedge \cdots \wedge d\theta^n This measure is: 1. coordinate-independent, 2. invariant under local unitaries, 3. monotone non-increasing under CPTP maps (by QFI monotonicity). Non-integer signals corners, cusps, or self-similar structure at arbitrarily fine scales in state space. C3 — Proposition: Closed-Form Scaling Exponent (§6) Assume: Born approximation, stationary zero-mean Gaussian random potential, spectral density S_V(q) \propto |q|^{-(1+2H)}, \quad H \in (1/2,1) We derive the exact RMS EWS time-delay scaling: \tau_{\mathrm{rms}}(k) \propto k^{-\chi(H)}, \quad \boxed{\chi(H)=\frac{3}{2}+H} Derivation steps: 1. 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We develop a metric-measure geometric reinterpretation of quantum entanglement in which nonlocal correlations are encoded in the intrinsic geometry of composite state space rather than in dynamical propagation. Using the Bures metric and CPTP coarse-graining semigroups, we define a scale-dependent effective dimension of the entangled-state manifold. We propose that geometric observables along the renormalization flow may exhibit long-range dependence (LRD) characterized by a Hurst exponent H ∈ (1/2,1). A conjectured infrared attractor H* ≈ 0.65 is formulated as a falsifiable hypothesis. The framework preserves no-signaling and does not modify quantum mechanics. A direct link to the variance (RMS) of Eisenbud–Wigner–Smith time delay is proposed, providing operational accessibility of geometric LRD effects.
Overview This preprint develops a unified, mathematically self-contained geometric reinterpretation of quantum entanglement, in which nonlocal correlations arise from the intrinsic geometry of composite Hilbert space rather than from any dynamical propagation between subsystems. The framework is built on: the Bures metric, Quantum Fisher Information (QFI), and completely positive trace-preserving (CPTP) coarse-graining semigroups. This work constitutes the unified synthesis and mathematical completion of two companion preprints: DOI: 10.5281/zenodo.18646759 — Fractal Geometry of Quantum Correlation Space (geometric/LRD foundation) DOI: 10.5281/zenodo.18649326 — Geometric Control of Quantum Time Delay in Non-Smooth Regimes (EWS application) It closes all identified mathematical gaps in both documents and consolidates the results into a single publication-ready manuscript. Main Contributions C1 — Theorem: No-Signaling Under CPTP Coarse-Graining (§3) For any CPTP map acting on subsystem , the reduced state of Alice satisfies: \operatorname{Tr}_B\!\left[(I_A \otimes \mathcal{E}_B)(\rho_{AB})\right] = \rho_A This follows from: linearity of partial trace, trace-preserving property of CPTP maps. Thus, Alice’s measurement statistics are provably independent of Bob’s local operation. The fractal geometry of the entangled-state manifold carries no dynamical signal and preserves relativistic causality. C2 — Canonical Effective Dimension with Explicit Measure (§2, §4) We introduce a scale-dependent effective Bures dimension: D_{\mathrm{eff}}(\ell) = \lim_{\varepsilon \to 0} \frac{\log V(\varepsilon;\ell)}{\log \varepsilon} where is the volume of an -ball in the entangled-state manifold , measured using the canonical Bures volume measure: d\mu_\ell(\theta) = \sqrt{\det g^{\mathrm{B}}(\theta;\ell)}\; d\theta^1 \wedge \cdots \wedge d\theta^n This measure is: 1. coordinate-independent, 2. invariant under local unitaries, 3. monotone non-increasing under CPTP maps (by QFI monotonicity). Non-integer signals corners, cusps, or self-similar structure at arbitrarily fine scales in state space. C3 — Proposition: Closed-Form Scaling Exponent (§6) Assume: Born approximation, stationary zero-mean Gaussian random potential, spectral density S_V(q) \propto |q|^{-(1+2H)}, \quad H \in (1/2,1) We derive the exact RMS EWS time-delay scaling: \tau_{\mathrm{rms}}(k) \propto k^{-\chi(H)}, \quad \boxed{\chi(H)=\frac{3}{2}+H} Derivation steps: 1. Born approximation for scattering phase , 2. computation of via spectral density, 3. differentiation and identification of dominant term in , 4. extraction of \mathrm{Var}[\tau_{\mathrm{EWS}}] \propto k^{-(3+2H)} Monotonicity: \chi'(H)=1>0 Numerical Predictions H χ(H) Physical regime 0.50 2.00 Brownian / diffusive borderline 0.65 2.15 Conjectured infrared attractor 0.75 2.25 Moderate long-range dependence 0.90 2.40 Strong long-range dependence C4 — Explicit Benchmark Calculations (§5) Depolarizing Channel on Bell State For \rho(p) = (1-p)\,|\Psi^-\rangle\langle\Psi^-| + \frac{p}{4}I\otimes I the Bures metric component: g^{\mathrm{B}}_{pp}(p) = \frac{9}{64(1-\tfrac{3}{4}p)} + \frac{3}{16p} A valid CPTP semigroup: p(\ell)=1-e^{-\gamma \ell} This family is smooth, yielding: D_{\mathrm{eff}}=1 This calibrates the formalism without over-claiming fractality. Werner States Near Entanglement Boundary \rho_W(p) = p|\Psi^-\rangle\langle\Psi^-| + (1-p)\frac{I}{4} Separability boundary (PPT): p^*=\frac{1}{3} Near the pure singlet , the metric diverges as: g^{\mathrm{B}}_{pp} \sim (1-p)^{-1/2} yielding: D_{\mathrm{eff}}\approx0.5 Non-integer dimension arises from metric singularity at boundary of . Falsifiable Conjectures Conjecture 1 — Fractal in Many-Body Critical Systems For CPTP block-spin coarse-graining of a 1D quantum critical ground state (central charge ): D_{\mathrm{eff}}(\ell)\notin\mathbb{Z} \quad \text{for } \ell_0<\ell<\ell^* Rejection criterion: Exact diagonalization (Ising chain ) yields integer at all scales. Conjecture 2 — LRD of Mutual Information Along RG Flow Let Y(\ell)=I(A:B)_{\rho(\ell)} Then: \mathrm{Cov}(Y(\ell),Y(\ell')) \sim C_H|\log\ell-\log\ell'|^{2H-2} Rejection criterion: DFA/R/S analysis yields or . Conjecture 3 — Infrared Attractor Under repeated CPTP coarse-graining: H(\ell)\to H^*\approx0.65 Rejection criterion: Five distinct universality classes all give Validity Domain The scaling law holds only if: 1. Born regime: , 2. No strong Anderson localization: , 3. Ergodic self-averaging, 4. Not in fully chaotic RMT regime (RMT predicts ), 5. Gaussian disorder (higher cumulants neglected). Violation of any condition invalidates the stated scaling. Experimental Platform and Measurement Protocol Central prediction: \tau_{\mathrm{rms}}(k) \propto k^{-2.15} \quad (H^*=0.65) Testable via attosecond spectroscopy: graphene nanoribbons, 2D transition-metal dichalcogenides, atomic chains on metallic surfaces. Falsification protocol: 1. Measure at values over one decade. 2. Fit: \log \tau_{\mathrm{rms}} = -\chi \log k + C 3. If |\chi_{\mathrm{fit}}-2.15|>0.1 \quad \text{with } \sigma_\chi<0.05 then is rejected. What This Work Does NOT Claim No hidden-variable theory No faster-than-light communication No modification of quantum measurement postulates No fractal spacetime (structure is in operator space) No universality beyond stated validity window Relation to Companion Preprints 18646759 — geometric/LRD foundation 18649326 — EWS non-smooth application This work provides: complete no-signaling proof, explicit Bures measure , closed-form exponent . Files Included paper_unified_v1.0.pdf paper_unified_v1.0.tex paper_explainer_v1.0.md README.md CITATION.cff zenodo.json License and Reproducibility License: Creative Commons Attribution 4.0 International (CC BY 4.0) Copyright: © 2026 Igor Chechelnitsky Theoretical work. All results reproducible from definitions and derivations provided. No proprietary code or primary experimental data used.
This work introduces an operational geometric framework for analyzing Eisenbud–Wigner–Smith (EWS) time delay in non-smooth quantum regimes. Without modifying standard quantum mechanics, we define scale-dependent geometric proxies compatible with non-smooth metric-measure structures and connect them to spectral shift mechanisms via Krein theory. Two scaling regimes are distinguished and expressed through a falsifiable law τ(E;ℓ) ∝ (1 + X(ℓ))^γ. The framework explicitly preserves unitarity, no-signaling, and relativistic causality. Concrete falsifiability criteria (Types I–III) are formulated. Order-of-magnitude comparison with attosecond chronoscopy suggests compatibility with observed delay enhancements in reduced-dimensional systems. The work introduces no new fundamental fields; it reframes time-delay observables in terms of coarse-grained geometric descriptors.
This work introduces a resolution-dependent geometric framework—Quantum Fractal Geometry (QFG)—in which the effective physical description of systems depends explicitly on observational scale. Within this framework, entangled quantum systems are modelled as unified geometric structures at deep resolution, characterised by a scale-dependent metric g_{μν}(ℓ) and a geometric phase field φ(x,ℓ) valued on S¹. Measurement is interpreted as a resolution-dependent projection of this unified structure onto detector-scale observables. A symmetry-constrained coarse-graining map is introduced as the minimal fixed point of resolution flow, identifying antipodal phase configurations (S¹ → S¹/ℤ₂). Under isotropy, continuity, and convex-linearity, the quantum correlation function E(a,b) = −cos(θ_a − θ_b) is recovered as the unique rotationally invariant statistic compatible with the projection structure, saturating the Tsirelson bound. Within QFG, Bell inequality violation arises not from nonlocal signalling or measurement dependence, but from the failure of scale-independent separability. Locality (in the operational no-signalling sense) and measurement independence are preserved. The framework further outlines a programme for deriving the Born rule from resolution-induced measure structure and identifies falsifiable predictions, including resolution-dependent deviations from ideal cosine correlations. This work should be understood as establishing the minimal geometric structure required for the QFG interpretation of Bell correlations, with full dynamical derivations deferred to future work.
Quantum entanglement is a central resource of quantum information science, yet its correlations are ordinarily treated as properties of the quantum state rather than as the outcome of an underlying physical process. Here we explore the hypothesis that these correlations are mediated dynamically by a field propagating locally at finite velocity through an extension of ordinary spacetime. The model embeds physical (3,1)(3,1)(3,1)-dimensional spacetime in a warped five-dimensional geometry containing an additional timelike coordinate. Within the adopted geometric ansatz, the form of the extended spacetime metric is determined by the five-dimensional vacuum Einstein equations. A massless field propagating through the resulting five-dimensional bulk can mediate correlations whose projection onto observable four-dimensional spacetime connects arbitrarily distant locations at equal laboratory time, while preserving operational no-signaling. Coupling this field to a Bohm--Bub-inspired collapse scheme provides a possible dynamical realization of entanglement correlations and, under a stated statistical consistency condition, reproduces Born statistics. The framework leads to a concrete experimental test. Two nominally independent Bell pairs are predicted to develop a weak, distance-dependent contextual correlation between particles belonging to different pairs, as a consequence of bulk-field mediation. This cross-pair correlation is absent in standard quantum mechanics for independently prepared systems and is predicted to decrease as the inverse square of their separation. It could therefore be tested by varying the distance between two simultaneous Bell experiments using existing photonic technology. Observation of such a signal would support a dynamical spacetime account of quantum entanglement and could have implications for quantum networks employing multiple independent entangled resources.
This work presents a comprehensive theoretical formulation of Quantum Fractal Geometry (QFG), a framework in which spacetime is fundamentally resolution-dependent. The apparent distinction between quantum and classical physics emerges from a single geometric principle: observer resolution as a structural parameter. The paper develops the formal mathematical foundations of QFG, including the definition of resolution-dependent metrics, a projection operator governing information accessibility, and the derivation of key physical results. These include the emergence of the Born rule from projection covariance, the recovery of the Einstein field equations as an infrared limit, and the Schrödinger equation as a dual flow correspondence. The framework provides a unified geometric interpretation of entanglement, black hole entropy, and gravitational structure, and introduces the Curvature Texture Index (CTI) as a measurable prediction linking multiscale geometric structure to astrophysical observables. A companion empirical study tests the CTI prediction using observational data from supermassive black hole host galaxies. All predictions are formulated with explicit falsifiability criteria, enabling experimental validation or refutation.
We propose a unified geometric framework in which space and time emerge as observer-dependent projections of quantum correlations embedded in the universal wavefunction. In this approach, we formulate six axioms (including a duality between entanglement and time) that establish a correspondence between correlation structures and effective spacetime geometry. We introduce the "correlationhedron", a convex geometric object representing the set of all permissible correlation vectors of a given state, and show how different observer "slicings" (modeled by projection maps) yield distinct emergent spacetimes from this object. An emergent metric is defined on each observer's spacetime via the second derivative of a correlation density (analogous to a Fisher information metric), linking gradients in quantum entanglement to curvature. This paper establishes the conceptual foundations of this approach as the first in a planned series of investigations. We illustrate the framework with conceptual and quantitative examples, including an explicit calculation of the emergent geometry for a two- qubit system in both separable and entangled states. Connections to holography (AdS/CFT) (Maldacena1998, Ryu2006), tensor networks (Swingle2012), and relational quantum approaches (Rovelli1996) are discussed, along with experimental signatures (such as curvature variations with entanglement) that could support the theory. Finally, we outline the limitations of the framework, particularly regarding dynamics and observer-dependent causality, to guide future investigations. This kinematic framework establishes the conceptual skeleton of emergent spacetime; detailed constructions, proofs of smoothness, and dynamical laws will appear in forthcoming work.