Definition
Covariant Hodge Laplacian
The covariant Hodge Laplacian is the second-order operator obtained by anticommuting a covariant exterior derivative with its formal adjoint.
Definition
Let be a vector bundle with bundle metric and compatible connection over an oriented Riemannian manifold. The covariant Hodge Laplacian on -valued -forms is
where is the exterior covariant derivative and is its formal adjoint. It is a formally self-adjoint elliptic operator with scalar principal symbol . Unlike the ordinary de Rham differential, need not vanish: curvature acts on the coefficient bundle. The operator preserves form degree and depends on both the Riemannian metric and the connection.
Energy identity and kernel
On a compact manifold without boundary,
Consequently, a smooth form lies in exactly when it is both -closed and -closed. This conclusion uses compactness or boundary conditions that eliminate boundary terms.
If is flat, then , so is a complex and the kernel represents cohomology through the corresponding Hodge theorem. For a curved connection, remains analytically meaningful, but it is not generally a cohomological model.
Weitzenböck form
The covariant Hodge Laplacian has a Weitzenböck decomposition
where the last two terms are zeroth-order actions of the Riemannian curvature and the curvature of . Thus the distinction between and the rough connection Laplacian is precisely a curvature correction. This is why “connection Laplacian” is not used here as an unqualified alias.
In gauge theory, the operator and its gauge-fixed variants control infinitesimal deformations and regularity of connections Freed–Uhlenbeck, chapter 2.
References
- Daniel S. Freed and Karen K. Uhlenbeck, Instantons and Four-Manifolds, 2nd ed., Springer, 1991. DOI record. Relevant: chapter 2, covariant differential operators, ellipticity, and gauge-theoretic estimates.
- Raymond O. Wells Jr., Differential Analysis on Complex Manifolds, 3rd ed., Springer, 2008. DOI record. Relevant: chapter IV, Hodge Laplacians and elliptic operator theory.