Let $(M, g)$ be a connected, oriented, compact Riemannian manifold, and let
\begin{align*}
\bigwedge^k T^* M = \bigoplus_i \Lambda_i^k
\end{align*}
be the decomposition into irreducible representations of $\mathrm{Hol}(g)$, so that each fiber $(\Lambda_i^k)_x \subseteq \bigwedge^k T_x^* M$ is an irreducible $\mathrm{Hol}_x(g)$-representation. Then:
1. For all $\alpha \in \Omega_i^k(M) := \Gamma(\Lambda_i^k)$, we have $\Delta \alpha \in \Omega_i^k(M)$.
2. There is a decomposition of de Rham cohomology:
\begin{align*}
H_{\mathrm{dR}}^k(M) = \bigoplus_i H_{i,\mathrm{dR}}^k(M),
\end{align*}
where $H_{i,\mathrm{dR}}^k(M) = \{[\alpha] : \alpha \in \Omega_i^k(M),\ \Delta \alpha = 0\}$.
The dimensions $\dim H_{i,\mathrm{dR}}^k(M)$ are called the **refined Betti numbers** of $(M, g)$.