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The Double Covariance Model: A Stochastic Reconstruction of Quantum Entangled States via Interplay of Micro-Macro Time Scales

Andrei Khrennikov

TL;DR

The Double Covariance Model (DCM) reinterprets the quantum density operator as a macro-covariance that emerges from the micro-scale cross-covariances of two classical stochastic processes across a macro time window. It provides concrete constructions to realize Bell states, arbitrary pure states, and mixed states from purely classical time series, and it derives subsystem states via a stochastic partial trace that connects marginal covariances to quantum reductions. By treating entanglement as a macro-time phenomenon driven by micro-time consistency, the DCM offers a relational, scale-aware foundation for quantum states and a stochastic realization of the partial trace. This framework bridges classical probability and quantum structure, with potential applications in quantum-like modeling across disciplines and a fresh perspective on the universality of relational fields.

Abstract

This article presents a concrete mathematical framework for the generation of entangled quantum states from classical stochastic processes. We demonstrate that any density operator $ρ_{AB}$ of a composite system can be derived from the correlations between two underlying stochastic processes, $X(t)$ and $Y(t)$, representing the random fluctuations of its subsystems. This construction utilizes a two-scale temporal scheme - micro and macro time - where quantum correlations emerge as macro-correlations derived from underlying micro-correlations. We propose the Double Covariance Model (DCM), which reproduces the fundamental properties of quantum theory by treating the quantum state as the fourth-order moment structure of an underlying classical probability space.

The Double Covariance Model: A Stochastic Reconstruction of Quantum Entangled States via Interplay of Micro-Macro Time Scales

TL;DR

The Double Covariance Model (DCM) reinterprets the quantum density operator as a macro-covariance that emerges from the micro-scale cross-covariances of two classical stochastic processes across a macro time window. It provides concrete constructions to realize Bell states, arbitrary pure states, and mixed states from purely classical time series, and it derives subsystem states via a stochastic partial trace that connects marginal covariances to quantum reductions. By treating entanglement as a macro-time phenomenon driven by micro-time consistency, the DCM offers a relational, scale-aware foundation for quantum states and a stochastic realization of the partial trace. This framework bridges classical probability and quantum structure, with potential applications in quantum-like modeling across disciplines and a fresh perspective on the universality of relational fields.

Abstract

This article presents a concrete mathematical framework for the generation of entangled quantum states from classical stochastic processes. We demonstrate that any density operator of a composite system can be derived from the correlations between two underlying stochastic processes, and , representing the random fluctuations of its subsystems. This construction utilizes a two-scale temporal scheme - micro and macro time - where quantum correlations emerge as macro-correlations derived from underlying micro-correlations. We propose the Double Covariance Model (DCM), which reproduces the fundamental properties of quantum theory by treating the quantum state as the fourth-order moment structure of an underlying classical probability space.
Paper Structure (26 sections, 2 theorems, 70 equations)

This paper contains 26 sections, 2 theorems, 70 equations.

Key Result

Lemma 1

Let $(\Omega,\mathcal{F},\mathbb P)$ be a probability space. Let $\{S_k\}_{k=1}^M$ be a family of random variables with values in a measurable space $(E,\mathcal{E})$, and let $\eta$ be a discrete random variable taking values in $\{1,\dots,M\}$ with Assume that $\eta$ is independent of the family $\{S_k\}_{k=1}^M$. Define the random variable Then, for any measurable function $f : E \to L,$ wher

Theorems & Definitions (3)

  • Lemma 1: Random selection of stochastic processes
  • Lemma 2: The Discrete Synchronization Condition
  • proof