Abstract
The general theory of quantum angular momentum is used to derive the unique Wigner distribution function for arbitrary angular-momentum states. We give the explicit distribution for atomic angular-momentum Dicke states, coherent states, and squeezed states that correspond to a collection of N two-level atoms. These Wigner functions W(θ,cphi) are represented as a pseudoprobability distribution in spherical phase space with spherical coordinates θ and cphi on the surface of a sphere of radius ħ √j(j+1) where j is the total angular-momentum eigenvalue.
- Received 10 November 1993
DOI:https://doi.org/10.1103/PhysRevA.49.4101
©1994 American Physical Society