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Path Integral for Multiplicative Noise: Generalized Fokker-Planck Equation and Entropy Production Rate in Stochastic Processes With Threshold

2 Oct 2024arXiv:2410.01387links table onlyarchive 2025-07-28

F. S. Abril-Bermúdez, C. J. Quimbay, J. E. Trinidad-Segovia, M. A Sánchez-Granero

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This paper introduces a comprehensive extension of the path integral formalism to model stochastic processes with arbitrary multiplicative noise. To do so, It\^o diffusive process is generalized by incorporating a multiplicative noise term (η(t)) that affects the diffusive coefficient in the stochastic differential equation. Then, using the Parisi-Sourlas method, we estimate the transition probability between states of a stochastic variable (X(t)) based on the cumulant generating function (𝒦_η) of the noise. A parameter γ∈[0,1] is introduced to account for the type of stochastic calculation used and its effect on the Jacobian of the path integral formalism. Next, the Feynman-Kac functional is then employed to derive the Fokker-Planck equation for generalized It\^o diffusive processes, addressing issues with higher-order derivatives and ensuring compatibility with known functionals such as Onsager-Machlup and Martin-Siggia-Rose-Janssen-De Dominicis in the white noise case. The general solution for the Fokker-Planck equation is provided when the stochastic drift is proportional to the diffusive coefficient and 𝒦_η is scale-invariant. Finally, the Brownian motion (BM), the geometric Brownian motion (GBM), the Levy α-stable flight (LF(α)), and the geometric Levy α-stable flight (GLF(α)) are simulated with thresholds, providing analytical comparisons for the probability density, Shannon entropy, and entropy production rate. It is found that restricted BM and restricted GBM exhibit quasi-steady states since the rate of entropy production never vanishes. It is also worth mentioning that in this work the GLF(α) is defined for the first time in the literature and it is shown that its solution is found without the need for It\^o's lemma.

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