Kähler Laplacian identity
= Kähler Laplacian identity
{c}
{title2=$\Delta_d=2\Delta_{\bar\partial}$}
On a <Kähler manifold>, expanding $d=\partial+\bar\partial$ and using the <Kähler identities> makes the mixed anticommutators vanish and gives $\Delta_\partial=\Delta_{\bar\partial}$. Therefore
$$
\Delta_d=2\Delta_{\bar\partial}=2\Delta_\partial.
$$