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arXiv:1202.4810 · Physics Letters A

Probability density of quantum expectation values

Lorenzo Campos Venuti, Paolo Zanardi A

Published May 22, 2013• 12 citations
arXivHTMLPDF
DOI
10.1016/j.physleta.2013.05.041

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It is shown that the imaginary part of ψ*Pψ plays a crucial role in describing the dispersive properties of probability densities in quantum mechanics. The quantity Im(ψ*Pψ) is proportional to the dispersive velocity of the probability density and has the same form as the diffusion current. The dispersive velocity does not contribute to the expectation value of the momentum operator, but contributes to the expectation value of the kinetic energy operator. The interpretation of the dispersive velocity is given for the one-dimensional Gaussian wave packet, the stationary states of a particle in a one-dimensional box, and the stationary states of the hydrogen atom.
Based on the Ehrenfest theorem, the time-dependent expectation value of a momentum operator can be evaluated equivalently in two ways. The integrals appearing in the expressions are taken over two different functions. In one case, the integrand is the quantum mechanical flux density j̲, and in the other, a different quantity j̲̃ appears, which also has the units of a flux density. The quantum flux density j̲ is related to the probability density ρ via the continuity equation, and j̲̃ may as well be used to define a density ρ̃ that fulfills a continuity equation. Employing a model for the coupled dynamics of an electron and a proton, we document the properties of the densities and flux densities. It is shown that although the mean momentum derived from the two quantities is identical, the various functions exhibit a very different coordinate and time-dependence. In particular, it is found that the flux density j̲̃ directly monitors temporal changes in the probability density, and the density ρ̃ carries information about wave packet dispersion occurring in different spatial directions.