  Let $M= \Gamma \setminus \mathbb{H}_d$ be a compact quotient of the
$d$-dimensional Heisenberg group $\mathbb{H}_d$ by a lattice subgroup $\Gamma$.
We show that the eigenvalue counting function $N(\lambda)$ for any fixed
element of a family of second order differential operators
$\left\{\mathcal{L}_\alpha\right\}$ on $M$ has asymptotic behavior
$N\left(\lambda\right) \sim C_{d,\alpha} \operatorname{vol}\left(M\right)
\lambda^{d + 1}$, where $C_{d,\alpha}$ is a constant that only depends on the
dimension $d$ and the parameter $\alpha$. As a consequence, we obtain an analog
of Weyl's law (both on functions and forms) for the Kohn Laplacian on $M$. Our
main tools are Folland's description of the spectrum of $\mathcal{L}_{\alpha}$
and Karamata's Tauberian theorem.
