Cited by 87Quantum Mechanics and ApplicationsQuantum chaos and dynamical systemsAdvanced Thermodynamics and Statistical Mechanics

Stochastic path integrals and open quantum systems

Strunz, Walter T.·1996·Physical Review A

Abstract

The general theory of path integral propagators for the solution of linear quantum state diffusion (LQSD) stochastic Schr\"odinger equations describing open quantum systems is developed. Both Hamiltonian and, where possible, Lagrangian path integrals are derived and their connection established. The Hamiltonian version turns out to be more suitable. The results also show how the stochastic terms in the LQSD equation introduce a weight functional under the path integral, thus restricting the set of contributing paths. The center of this weight functional is determined by the stochastic processes governing the LQSD equation. In general, this picture holds in a semiclassical limit only. Some peculiarities of stochastic path integrals are pointed out. We evaluate the stochastic path integral in closed form for soluble models, gaining further insight into the behavior of the solutions of the LQSD equation. \textcopyright{} 1996 The American Physical Society.

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Crossref · 10.1103/physreva.54.2664

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32 of 32 references verified0 citation errors · 0 not checkable

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  • The representations assigned to triangles are simple representations of SO(4) of the form (j,j), i.e. class-1 representations with respect to SO(3), characterized by vanishing of the second Casimir.

    “the representations of the triangles are 'simple representations' of SO(4) of the form (j, j ), i.e. representations of class 1 with respect to the subgroup SO(3) [66], characterized by the vanishing of the second Casimir of the group”
  • Simple representations of the Lorentz group can be realized on square integrable functions on hyperboloids in Minkowski space: Q1, Q0, and Q-1.

    “In fact [66], the simple representations of the Lorentz group can be realized in the space of square integrable functions on hyperboloids in Minkowski space.These are Q 1 , or Lobachevskian space, characterized by x µ x µ = 1 and x 0 > 0, the positive null cone Q 0 , with x µ x µ = 0 and x 0 > 0, and the imaginary Lobachevskian space Q -1 , with x µ x µ = -1.”
  • The Hilbert space used to define the operators is built from gauge invariant cylindrical functions on the space of connections A.

    “The Hilbert space in which we will define the operators is constructed from the gauge invariant cylindrical functions on A [6,7,12,19,20].”

    From Volume and quantizations (1997) · cites this paper as [19]

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Authors
Strunz, W. T.
Affiliations
University of London (GB)
Corresponding author
Strunz, Walter T.
Venue
Physical Review A
Published
1996-10-01
Volume
54
Issue
4
Pages
2664-2674
ISSN
  • 0556-2791 (ISSN-L)
  • 1050-2947
  • 1094-1622
OpenAlex
W1992243061
Cited by
87
References
32
Citations by year
2025: 1 · 2024: 1 · 2023: 4 · 2021: 2 · 2019: 1 · 2018: 1 · 2017: 1 · 2014: 1 · 2013: 1 · 2012: 2
FWCI
8.16
Type
journal article
Language
en
Open access
closed
Locations
  • Physical Review A (publishedVersion)
  • PubMed (publishedVersion)
Topics
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Mechanics and Applications
  • Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Quantum chaos and dynamical systems
  • Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Advanced Thermodynamics and Statistical Mechanics
Keywords
stochastic path integral, open quantum systems, stochastic Schrödinger equation, Hamiltonian path integral, semiclassical limit

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