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This paper proposes a classical field theory framework where quantum interference patterns emerge from statistical observables rather than requiring intrinsic non-classicality, effectively deriving the Schrödinger equation within this probabilistic model. By treating particles as subsystems defined by conserved charges in a complex scalar field, it offers an alternative perspective on foundational quantum mechanics that could influence theoretical approaches to interpreting wave functions and tunneling phenomena.
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Classical probabilistic realisation of quantum double-slit interference

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arXiv:2607.11580v2 Announce Type: replace Abstract: We demonstrate how the interference effects for a quantum particle in the double-slit experiment can be described by classical probabilities. We investigate a classical field theory for a complex scalar field with probabilistic initial conditions. A central element are conserved charges leading to the concept of particles. These are statistical observables which describe properties of the probability distribution for field configurations. The conserved charges define subsystems for particle excitations of a vacuum state. The classical probability distribution for the one-particle subsystem can be expressed in terms of a complex wave function. The Liouville equation for the classical probability distribution implies that the time evolution of this wave function obeys the Schr\"odinger equation for a quantum particle in a potential. The potential arises from space-dependent external fields in the otherwise relativistic classical field theory. It can be chosen arbitrarily, realizing the typical quantum effects of interference, tunneling or discrete energy spectra.

Abstract:We demonstrate how the interference effects for a quantum particle in the double-slit experiment can be described by classical probabilities. We investigate a classical field theory for a complex scalar field with probabilistic initial conditions. A central element are conserved charges leading to the concept of particles. These are statistical observables which describe properties of the probability distribution for field configurations. The conserved charges define subsystems for particle excitations of a vacuum state. The classical probability distribution for the one-particle subsystem can be expressed in terms of a complex wave function. The Liouville equation for the classical probability distribution implies that the time evolution of this wave function obeys the Schrödinger equation for a quantum particle in a potential. The potential arises from space-dependent external fields in the otherwise relativistic classical field theory. It can be chosen arbitrarily, realizing the typical quantum effects of interference, tunneling or discrete energy spectra.

Quantum Physics (quant-ph); Statistical Mechanics (cond-mat.stat-mech); High Energy Physics - Theory (hep-th)

arXiv:2607.11580 [quant-ph]

(or arXiv:2607.11580v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.11580 Focus to learn more arXiv-issued DOI via DataCite

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