Wigner functions for describing wave fields and pulses

The Wigner function or Wigner distribution is a bilinear integral transformation that allows representing a function jointly in terms of its original variable and its Fourier conjugate. For example, by using the Wigner function, a time signal representing a piece of music can be represented jointly in terms of time and frequency, providing a representation qualitatively similar to a musical score. Wigner functions were first defined by Eugene Wigner in 1932 to describe the wavefunction of a quantum particle in terms of both position and momentum, hence providing a classical-like picture. They also have been applied to modeling the propagation of optical wave fields in terms of rays, and also for the propagation of optical pulses through simple dispersive media.
Our group’s work on Wigner functions and other phase space representations has included studying their behavior in certain limits, as well as providing new definitions for them that are best suited for describing different physical situations, such as nonparaxial propagation of scalar and electromagnetic fields, diffraction effects, propagation of pulses through transparent media with arbitrary dispersion properties, and wave fields constrained to simple curved spaces.

Review/tutorial articles

Standard Wigner functions and their use in optics

Journal articles

Wigner functions and other phase distributions for nonparaxial scalar and electromagnetic wave fields

Journal articles

Conference proceedings

Highlights

Wigner functions for short pulses in media with arbitrary dispersion

Journal articles

Wigner functions for curved spaces

Journal articles