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Breakdown of the coherent state path integral: two simple examples.

Justin H Wilson1, Victor Galitski

  • 1Joint Quantum Institute and Condensed Matter Theory Center, Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA.

Physical Review Letters
|April 8, 2011
PubMed
Summary
This summary is machine-generated.

The time-continuous coherent state path integral fails for specific quantum models, unlike its time-discretized counterpart. This breakdown occurs when the Hamiltonian is quadratic in the coherent state generator.

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Area of Science:

  • Quantum mechanics
  • Condensed matter physics

Background:

  • Coherent state path integrals are a powerful tool in quantum mechanics.
  • The single-site Bose-Hubbard model and spin-path integrals are important quantum systems.
  • Operator approaches provide a benchmark for path integral calculations.

Purpose of the Study:

  • To investigate the limitations of the time-continuous coherent state path integral.
  • To identify the conditions under which this path integral formulation breaks down.
  • To compare the performance of time-continuous and time-discretized path integrals.

Main Methods:

  • Analysis of the time-continuous coherent state path integral.
  • Examination of the single-site Bose-Hubbard model and spin-path integral.
  • Comparison with results from operator-based methods.

Main Results:

  • The time-continuous coherent state path integral fails for the single-site Bose-Hubbard model and spin-path integral.
  • Breakdown occurs when the Hamiltonian is quadratic in the coherent state generator.
  • The time-discretized path integral does not exhibit these issues.

Conclusions:

  • The time-continuous coherent state path integral is not universally applicable.
  • The quadratic nature of the Hamiltonian is a critical factor in the path integral's failure.
  • Time-discretization offers a robust alternative for these quantum systems.