Let \((M,g)\) be a Riemannian manifold. The (geometric) Laplacian is a linear map \(\Delta\colon C^\infty(M)\to C^\infty(M)\) defined by \(\Delta u = -\div(\grad u)\).
\[
\DeclareMathOperator{\div}{div}
\DeclareMathOperator{\grad}{grad}
\]