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Fractional transport equations for Lévy stable processes
1Max-Planck-Institut für Kernphysik, Postfach 103980, 69029 Heidelberg, Germany.
Physical Review Letters
|April 6, 2001
Summary
This study derives quantum master equations and classical transport equations for systems with Lévy stable random forces. It introduces fractional extensions of Klein-Kramers and Smoluchowski equations, clarifying their interconnections.
Area of Science:
- Quantum mechanics
- Statistical physics
- Non-equilibrium systems
Background:
- The Feynman-Vernon influence functional method is a key tool for studying open quantum systems.
- Lévy stable random forces introduce non-Markovian dynamics and long-range correlations.
- Understanding transport phenomena in quantum systems under external noise is crucial.
Purpose of the Study:
- To derive a quantum master equation for systems subjected to Lévy stable random forces.
- To obtain classical transport equations for the Wigner function in weak and strong friction limits.
- To clarify the relationships between different fractional transport equations.
Main Methods:
- Application of the Feynman-Vernon influence functional method.
- Derivation of quantum master equations.
- Analysis of Wigner function transport in classical limits.
- Identification of fractional extensions of known equations.
Main Results:
- A quantum master equation for Lévy noise is obtained.
- Fractional extensions of the Klein-Kramers and Smoluchowski equations are derived.
- The fractional nature of position in Smoluchowski dynamics is linked to momentum in Klein-Kramers dynamics.
- Connections among various fractional transport equations are elucidated.
Conclusions:
- The study provides a theoretical framework for quantum systems with Lévy noise.
- Fractional calculus is essential for describing transport under such noise.
- The work clarifies the theoretical underpinnings of fractional transport equations.