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 {} {}j(j+1) where j is the total angular-momentum eigenvalue.
No takes yet. Share an insight, caveat, or question.
Dowling et al. (1994) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: