  We are concerned with a phase-space probability distribution which is known
as Husimi $Q$-function of a density operator with respect to a set of coherent
states $\vert\widetilde{\kappa}_{z,B,R,m}\rangle$ attached to an $m$th
hyperbolic Landau level and labeled by points $z$ of an open disk of radius
$R$, where $B>0$ is proportional to a magnetic field strength. For a density
operator representing a projector on a Fock state $\left\vert j\right\rangle$
we obtain the $Q_{j}$ distribution and discuss some of its basic properties
such as its characteristic function and its main statistical parameters. We
achieve the same program for the thermal density operator (mixed states) of the
isotonic oscillator for which we establish a lower bound for the associated
thermodynamical potential. We recover most of the results of the Euclidean
setting (flat case) as the parameter $R$ goes to infinity by making appeal to
asymptotic formulas involving orthogonal polynomials and special functions. As
a tool, we establish a summation formula for the special Kamp\'{e} de
F\'{e}riet function $\digamma _{2:0:0}^{1:2:2}$.
