We investigate properties of quasi-joint-probability (QJP) distributions on finite-state quantum systems, especially the two- and three-state systems, based on the general framework of quantum/quasi-classical representations [1,2]. We show that the Kirkwood–Dirac distribution is a prime candidate among the QJP distributions that behave well in view of the following two perspectives: the information contained in the QJP distribution and its affinity to genuine joint-probability distributions. Regarding the first criterion, we show that the Kirkwood–Dirac distributions on two- and three-state quantum systems yield faithful quasi-classical representations [1,2] of quantum states with a minimal set of observables, namely a pair of two different directions of the spin, and thereby point out that in general the imaginary parts of the QJP distributions play essential roles in this respect. As for the second criterion, we prove that the Kirkwood–Dirac distributions on finite-state quantum systems are supported on the product set of the spectra of the quantum observables involved.