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Semiclassical theory for spatial density oscillations in fermionic systems.

J Roccia1, M Brack, A Koch

  • 1Institute for Theoretical Physics, University of Regensburg, D-93040 Regensburg, Germany.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|April 7, 2010
PubMed
Summary
This summary is machine-generated.

We developed a semiclassical theory to calculate particle and kinetic-energy densities for N fermions in a potential. This method accurately predicts quantum densities, even for moderate particle numbers.

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Area of Science:

  • Quantum mechanics
  • Statistical physics
  • Computational physics

Background:

  • Semiclassical theories offer approximations for quantum systems.
  • Previous work developed a semiclassical theory for densities based on classical closed orbits.
  • Generalizing this theory to higher dimensions and regularizing specific behaviors is needed.

Purpose of the Study:

  • To generalize a semiclassical theory for particle and kinetic-energy densities to D>1 dimensions.
  • To regularize the theory for symmetry breaking at r=0 and near classical turning points.
  • To validate the generalized theory against exact quantum calculations.

Main Methods:

  • Generalization of a semiclassical theory based on classical closed orbits.
  • Regularization techniques for U(1) symmetry breaking and Friedel oscillations.
  • Comparison with exact quantum-mechanical calculations for various potentials.

Main Results:

  • The generalized semiclassical theory accurately calculates densities in D>1 dimensions.
  • Two types of oscillations (radial and nonradial) are identified for spherical systems.
  • Excellent agreement is found between semiclassical and exact densities for moderate N.
  • The Thomas-Fermi functional is shown to reproduce quantum density oscillations to first order.

Conclusions:

  • The generalized semiclassical theory provides a robust method for calculating fermionic densities.
  • The theory successfully captures oscillatory features in quantum densities.
  • This approach offers a computationally efficient alternative to exact quantum calculations.