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Dephasing representation: Employing the shadowing theorem to calculate quantum correlation functions.
1Mathematical Sciences Research Institute, Berkeley, California 94720, USA. vanicek@post.harvard.edu
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|December 17, 2004
Summary
This study introduces a unique dephasing representation for quantum systems, simplifying calculations of quantum fidelity and correlation functions. This method offers a practical approach for complex, multi-dimensional systems where exact quantum computations are infeasible.
Area of Science:
- Quantum mechanics
- Statistical physics
- Chaos theory
Background:
- Classical and quantum systems can correspond due to the Heisenberg uncertainty principle.
- Existing semiclassical methods often rely on approximations like the Van Vleck determinant.
- Calculating quantum correlation functions in complex systems is computationally challenging.
Purpose of the Study:
- To develop a unique semiclassical representation for quantum systems.
- To provide a rigorous method for calculating quantum correlation functions.
- To extend the applicability of semiclassical linear-response theory to generic mixed systems.
Main Methods:
- Introduced a 'dephasing representation' based on the Feynman path integral formulation.
- Utilized the correspondence between classical systems and quantum systems.
- Related the approach to the shadowing theorem for rigorous approximation.
Main Results:
- Developed a unique semiclassical representation without the Van Vleck determinant.
- Demonstrated that all contributing trajectories in the dephasing representation have the same amplitude.
- Showed that numerical implementation requires only actions along unperturbed trajectories.
Conclusions:
- The dephasing representation is rigorously applicable to systems where the shadowing theorem holds.
- This method is valid for generic, mixed quantum systems, extending previous theories.
- It offers a practical computational tool for quantum correlation functions in high-dimensional, nonuniversal regimes.