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Geometric Control of Quantum Time Delay in Non-Smooth Regimes: Operational Descriptors, Spectral Mechanism, Scaling Laws, and Falsifiability

CHECHELNITSKY IGOR

Published Feb 11, 2026• 0 citations
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Abstract

Scope (minimal thesis): The record contains (i) the main preprint (PDF), (ii) LaTeX source (fully reproducible), and (iii) an extended “explainer” PDF (intuition-first, minimal prerequisites, with figures and tables). Key idea: effective degradation of geometric regularity—defined without smooth curvature—can act as a temporal bottleneck, increasing measurable quantum time delays. Operational proxies: (1) volume-growth/ball-measure deficit proxy , and (2) spectral/heat-kernel descriptors including spectral dimension . Mechanism anchor: geometry-induced spectral modifications can shift scattering phase through spectral shift theory (Kreĭn / Birman–Yafaev viewpoint), hence modifying EWS delays. Test program: controlled families where a geometric scale is varied at fixed probe conditions; fit versus and apply falsifiability Types I–III. Non-claims: no new gravity, no QM violation, no “free energy”, no universal constant assumed a priori. Reproducibility: theoretical/conceptual; no proprietary data required.

DOI
10.5281/zenodo.18608881

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Geometric Control of Quantum Time Delay in Non-Smooth Regimes: Operational Descriptors, Spectral Mechanism, Scaling Laws, and Falsifiability

CHECHELNITSKY IGOR

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.

•Feb 15, 2026•0 citations

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. 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. 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•Feb 16, 2026•0 citations

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A Nuisance-Aware Residual-Test Framework for Geometry-Induced Quantum Potentials in Curved Constrained Platforms

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Version 4.0 public record for “A Nuisance-Aware Residual-Test Framework for Geometry-Induced Quantum Potentials in Curved Constrained Platforms”. Version 4.0 is a substantive revision of the public record. It updates the title and scientific framing, clarifies the established Jensen–Koppe–da Costa geometric-potential anchor versus the new nuisance-aware residual-test methodology, adds an explicit finite-width/disorder/spin-orbit/electrostatic validity envelope, strengthens the minimum experimental-design protocol, improves figure readability, and synchronizes the journal and Zenodo packages. The work is framed as a conservative methodological and design-level residual-test framework for geometry-induced quantum potentials in curved constrained platforms. The manuscript is anchored to the established Jensen–Koppe–da Costa geometry-induced potential for scalar particles constrained to smooth curves. The standard constrained-curve prediction is represented by the fixed coefficient −1/4, while the residual parameter delta-lambda is defined as a falsifiable null-test quantity. Standard constrained quantum mechanics predicts delta-lambda = 0. The manuscript emphasizes that any nonzero residual should first be treated as a platform anomaly unless it survives curvature scaling, nuisance projection, matched-reference controls, blind residual extraction, and cross-geometry replication. No experimental detection is claimed. The included simulations and prospective bounds remain design-level estimates. The package contains the manuscript, supplementary information, figures, reproducibility code, generated CSV/JSON data, metadata files, and public technical materials sufficient to regenerate the numerical validation tables, platform-specific energy-scale estimates, residual sensitivity plots, and figures.

•Jun 13, 2026•0 citations
Scope (minimal thesis): The record contains (i) the main preprint (PDF), (ii) LaTeX source (fully reproducible), and (iii) an extended “explainer” PDF (intuition-first, minimal prerequisites, with figures and tables). Key idea: effective degradation of geometric regularity—defined without smooth curvature—can act as a temporal bottleneck, increasing measurable quantum time delays. Operational proxies: (1) volume-growth/ball-measure deficit proxy , and (2) spectral/heat-kernel descriptors including spectral dimension . Mechanism anchor: geometry-induced spectral modifications can shift scattering phase through spectral shift theory (Kreĭn / Birman–Yafaev viewpoint), hence modifying EWS delays. Test program: controlled families where a geometric scale is varied at fixed probe conditions; fit versus and apply falsifiability Types I–III. Non-claims: no new gravity, no QM violation, no “free energy”, no universal constant assumed a priori. Reproducibility: theoretical/conceptual; no proprietary data required.
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.
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.
Using the de Branges--Kreĭn (DBK) canonical system and weighted Mellin space as carriers, we explicitly incorporate the finite bandwidth/time window of real instruments into spectral measures, forming a windowed readout framework; we characterize ``commit (collapse/commit)'' through KL/Bregman information geometry; use scattering phase--spectral density--Wigner--Smith delay as energy scale; close non-asymptotic errors via Nyquist--Poisson--Euler--Maclaurin (three-term decomposition); ensure realizability and stability through variational optimization of frame/sampling density and window/kernel. The core unified formula is $ \,\varphi'(E)=-\pi\,\rho_{\mathrm{rel}(E)=1{2}trQ(E)\,}\quad(a.e.) $ unifying (single/multi-channel) scattering phase derivative, relative local density of states (LDOS) and Wigner--Smith delay; under information geometry we obtain Born probability = minimal-KL projection (I-projection), and ``pointer basis'' is spectral minimum of windowed readout operator. Above criteria consistent with Herglotz--Weyl, Birman--Kreĭn, Wigner--Smith, Ky Fan, Poisson/EM and other standard results, directly interchangeable and implementable.
This record presents a short, time-stamped research note proposing a clean control experiment aimed at clarifying the physical origin of recently observed quantum-metric-induced trajectory bending in quantum materials. While such effects are commonly interpreted as arising from geometric structure in Hilbert space, an open question remains as to whether an effective temporal or phase-delay contribution may act as the underlying generator of the observed metric. The proposed protocol isolates temporal phase modulation from spatial geometry by keeping particle trajectories and external forces fixed while varying only the effective phase, delay, or frequency associated with the quantum state. The experiment constitutes a null test: a positive outcome would indicate a temporal contribution to the effective metric, while a null result would strengthen a purely geometric interpretation. The proposal requires no new instrumentation and is compatible with existing solid-state platforms (such as oxide-interface two-dimensional electron gases), topological or quantum Hall interferometers, and cold-atom interferometric systems. This note is intended as a conceptual and experimental guide rather than a report of new data.
We construct a unified framework of Windowed Scattering--Information Geometry (WSIG) centered on the ``operator--measure--function'' triple: observation is operationalized through Toeplitz/Berezin compression Kw,h=Πw Mh Πw\mathsf{K}_{w,h}=\Pi_w\,\mathsf{M}_h\,\Pi_wKw,h​=Πw​Mh​Πw​, reducing all readouts to linear functionals on spectral measures. The trinity scale identity φ′(E)/π=ρrel(E)=(2π)−1tr Q(E)=−ξ′(E)\varphi'(E)/\pi=\rho_{\mathrm{rel}}(E)=(2\pi)^{-1}\mathrm{tr}\,\mathsf{Q}(E)=-\xi'(E)φ′(E)/π=ρrel​(E)=(2π)−1trQ(E)=−ξ′(E) unifies phase, relative density of states, and Wigner--Smith group delay as master scales. For observer filter chains {Kθ}θ∈Θ\{\mathsf{K}_\theta\}_{\theta\in\Theta}{Kθ​}θ∈Θ​, we define an information action S\mathcal{S}S and induce an information metric via the Hessian gμν=∂μ∂νSg_{\mu\nu}=\partial_\mu\partial_\nu\mathcal{S}gμν​=∂μ​∂ν​S, interpreting connection and curvature as second-order non-commutative responses of readouts to observation parameters. Under the ``double-time separation'' postulate---where causal partial order is uniquely defined by frontier time t∗t_*t∗​ while windowed group delay Tγ[w,h]T_\gamma[w,h]Tγ​[w,h] serves only as operational scale---variation of the action A=(2κ)−1 ⁣∫(R−2Λ)∣g∣ dnθ+∫(Linfo+λμν[gμν−∂μ∂νSloc])∣g∣ dnθ\mathcal{A}=(2\kappa)^{-1}\!\int(\mathcal{R}-2\Lambda)\sqrt{|g|}\,d^n\theta+\int(\mathcal{L}_{\mathrm{info}}+\lambda^{\mu\nu}[g_{\mu\nu}-\partial_\mu\partial_\nu\mathcal{S}_{\mathrm{loc}}])\sqrt{|g|}\,d^n\thetaA=(2κ)−1∫(R−2Λ)∣g∣​dnθ+∫(Linfo​+λμν[gμν​−∂μ​∂ν​Sloc​])∣g∣​dnθ yields Einstein-type equations Gμν+Λgμν=κ Tμν\mathcal{G}_{\mu\nu}+\Lambda g_{\mu\nu}=\kappa\,\mathcal{T}_{\mu\nu}Gμν​+Λgμν​=κTμν​. The right-hand stress-energy tensor Tμν\mathcal{T}_{\mu\nu}Tμν​ arises from spectral responses of Kθ\mathsf{K}_\thetaKθ​. Under band-limited and Nyquist--Poisson--finite-order Euler--Maclaurin (NPE) discipline, we achieve error closure with ``non-increasing singularity: poles = master scales''. Within the same geometric framework, we unify quantum measurement: superposition = convex superposition of compatible components in static blocks; collapse = anchor switching and π\piπ-semantic collapse; entanglement = inseparable information correlations in causal networks. Continuous monitoring satisfies GKSL dynamics and Spohn entropy production monotonicity, with Belavkin filtering providing conditional state updates. Core criteria and required external theorems are provided, along with one-dimensional potential scattering examples and complete proof chains.
Version 4.0 public record for “A Nuisance-Aware Residual-Test Framework for Geometry-Induced Quantum Potentials in Curved Constrained Platforms”. Version 4.0 is a substantive revision of the public record. It updates the title and scientific framing, clarifies the established Jensen–Koppe–da Costa geometric-potential anchor versus the new nuisance-aware residual-test methodology, adds an explicit finite-width/disorder/spin-orbit/electrostatic validity envelope, strengthens the minimum experimental-design protocol, improves figure readability, and synchronizes the journal and Zenodo packages. The work is framed as a conservative methodological and design-level residual-test framework for geometry-induced quantum potentials in curved constrained platforms. The manuscript is anchored to the established Jensen–Koppe–da Costa geometry-induced potential for scalar particles constrained to smooth curves. The standard constrained-curve prediction is represented by the fixed coefficient −1/4, while the residual parameter delta-lambda is defined as a falsifiable null-test quantity. Standard constrained quantum mechanics predicts delta-lambda = 0. The manuscript emphasizes that any nonzero residual should first be treated as a platform anomaly unless it survives curvature scaling, nuisance projection, matched-reference controls, blind residual extraction, and cross-geometry replication. No experimental detection is claimed. The included simulations and prospective bounds remain design-level estimates. The package contains the manuscript, supplementary information, figures, reproducibility code, generated CSV/JSON data, metadata files, and public technical materials sufficient to regenerate the numerical validation tables, platform-specific energy-scale estimates, residual sensitivity plots, and figures.