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Local Tensorial Structure of the Projection Transition Operator: Resolving EPR Nonlocality (v.3).

Hennadii Kovalov

Published Sep 4, 2026• 0 citations
Publisher

Abstract

We formalize a bilocal extension of the Classical Transition Operator within the framework of phase dynamics to resolve the Einstein–Podolsky–Rosen (EPR) nonlocality paradox. By treating the electron () and positron () not as discrete, spatially isolated entities, but as dual, time-symmetric observational projections of a singular topological -cell, quantum entanglement is shown to be a strict artifact of dimensional reduction. Introducing a dynamic phase shift governed by an external Minkowski 4-potential , we employ the 4-dimensional Stokes’ theorem to map the phase accumulation directly onto the classical Maxwell field tensor , naturally deriving the covariant Lorentz force equation and its sign asymmetry without free parameters. Furthermore, we prove that the positron is a reactive topological "echo" of the primary forward phase step, introducing a sub-temporal causal delay bound by the Compton scale (), which resolves the cosmological baryon asymmetry problem.

DOI
10.5281/zenodo.22309674

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We formalize a bilocal extension of the Classical Transition Operator within the framework of phase dynamics to resolve the Einstein–Podolsky–Rosen (EPR) nonlocality paradox. By treating the electron () and positron () not as discrete, spatially isolated entities, but as dual, time-symmetric observational projections of a singular topological -cell, quantum entanglement is shown to be a strict artifact of dimensional reduction. Introducing a dynamic phase shift governed by an external Minkowski 4-potential , we employ the 4-dimensional Stokes’ theorem to map the phase accumulation directly onto the classical Maxwell field tensor , naturally deriving the covariant Lorentz force equation and its sign asymmetry without free parameters. Furthermore, we prove that the positron is a reactive topological "echo" of the primary forward phase step, introducing a sub-temporal causal delay bound by the Compton scale (), which resolves the cosmological baryon asymmetry problem.
We formalize a bilocal extension of the Classical Transition Operator within the framework of Phase Dynamics to resolve the Einstein–Podolsky–Rosen (EPR) nonlocality paradox. By treating the electron () and positron () not as discrete, spatially isolated entities, but as dual, time-symmetric observational projections of a singular topological -cell, quantum entanglement is shown to be a strict artifact of dimensional reduction. Introducing a dynamic phase shift governed by an external Minkowski 4-potential , we employ the 4-dimensional Stokes’ theorem to map the phase accumulation directly onto the classical Maxwell field tensor , naturally deriving the covariant Lorentz force equation and its sign asymmetry without free parameters. Furthermore, we prove that the positron is a reactive topological "echo" of the primary forward phase step, introducing a sub-temporal causal delay bound by the Compton scale (), which resolves the cosmological baryon asymmetry problem. Finally, we demonstrate that annihilation is not the destruction of matter, but the geometric collapse of the projection Jacobians and — extracting the system from Minkowski spacetime and returning it to the pure phase metric , where energy is absolutely conserved and probability vanishes.
We formalize a bilocal extension of the Classical Transition Operator within the framework to resolve the Einstein–Podolsky–Rosen (EPR) nonlocality paradox. By treating the electron () and positron () not as discrete, spatially isolated entities, but as dual, time-symmetric observational projections of a singular topological -cell, quantum entanglement is shown to be a strict artifact of dimensional reduction. Introducing a dynamic phase shift governed by an external Minkowski 4-potential , we employ the 4‑dimensional Stokes’ theorem to map the phase accumulation directly onto the classical Maxwell field tensor . This geometric mapping naturally derives the covariant Lorentz force equation. We demonstrate that the apparent “spooky action at a distance” is an artifact of the coordinate time projection, whereas the physical metric of the system remains strictly local and invariant within the absolute phase time .
We formalize a bilocal extension of the Classical Transition Operator within the framework of Phase Dynamics to resolve the Einstein–Podolsky–Rosen (EPR) nonlocality paradox. By treating the electron () and positron () not as discrete, spatially isolated entities, but as dual, time-symmetric observational projections of a singular topological -cell, quantum entanglement is shown to be a strict artifact of dimensional reduction. Introducing a dynamic phase shift governed by an external Minkowski 4-potential , we employ the 4‑dimensional Stokes’ theorem to map the phase accumulation directly onto the classical Maxwell field tensor . This geometric mapping naturally derives the covariant Lorentz force equation. We demonstrate that the apparent “spooky action at a distance” is an artifact of the coordinate time projection, whereas the physical metric of the system remains strictly local and invariant within the absolute phase time .
We formalize a bilocal extension of the Classical Transition Operator within the framework of Phase Dynamics to resolve the Einstein–Podolsky–Rosen (EPR) nonlocality paradox. By treating the electron () and positron () not as discrete, spatially isolated entities, but as dual, time-symmetric observational projections of a singular topological -cell, quantum entanglement is shown to be a strict artifact of dimensional reduction. Introducing a dynamic phase shift governed by an external Minkowski 4-potential , we employ the 4‑dimensional Stokes’ theorem to map the phase accumulation directly onto the classical Maxwell field tensor . This geometric mapping naturally derives the covariant Lorentz force equation. We demonstrate that the apparent “spooky action at a distance” is an artifact of the coordinate time projection, whereas the physical metric of the system remains strictly local and invariant within the absolute phase time .
This paper provides a strictly local, deterministic, and geometric derivation of quantum entanglement within the framework of Finsler-Maxwell Thermo-Relativistic (TR) Gravity. By extending the 4-dimensional positional space-time manifold to the 8-dimensional phase space of the Finsler tangent bundle TM, we demonstrate that quantum entanglement is not a non-local "spooky action at a distance." Instead, it is a manifestation of topological contiguity along the vertical fibers of velocity, frequency, and temperature. We prove that the measurement-induced correlation wave propagates at a superluminal coordinate velocity (V_intrication approx 2.603 * c) from a Riemannian perspective, yet remains strictly causal and subluminal (V_intrication < V_lim) within the conformally broadened Finslerian light-cone matrix. This approach provides a self-regularizing, geometric resolution to the Einstein-Podolsky-Rosen (EPR) paradox without violating local Lorentz covariance, showing that quantum correlations are encoded directly within the intrinsic non-zero bundle torsion.
This study examines and resolves one of the most fundamental problems in quantum mechanics, the apparent non-locality arising from quantum entanglement (EPR paradox), utilizing the axiomatic model of Topological Network Dynamics (Phi-ND). The research demonstrates that the state change of entangled systems does not violate the causal speed limit of relativity. The framework establishes that entanglement is physically a topological phase transition (vertex-fusion) on a discrete, fundamental graph, whereas macroscopic three-dimensional Euclidean distance is merely the result of a lower-energy projection. Because the distance between the two entangled objects is strictly zero within the fundamental topological space, causal phase-state updating remains local and instantaneous, thereby preserving local realism and providing a definitive mathematical explanation for the violation of Bell's inequalities.