Definition
Harmonic differential form
A differential form annihilated by the Hodge Laplacian of a Riemannian metric.
Definition
Let be an oriented Riemannian manifold, and let be a smooth differential form. The form is harmonic when
where
is the Hodge Laplacian and is the codifferential determined by and the orientation. Harmonicity therefore depends on the Riemannian metric. On a compact manifold without boundary, it is equivalent to the pair of first-order conditions and ; that equivalence need not hold for arbitrary smooth forms on a noncompact manifold de Cataldo, Lemma 2.3.2.
Energy characterization
When is compact and has no boundary, formal adjointness and Stokes' theorem give
Thus forces both summands to vanish. Conversely, a closed and coclosed form is harmonic directly from the definition of . The compactness and boundary hypotheses justify the integrated identity without extra boundary terms or decay assumptions Wells, Chapter IV, §2.
The space of harmonic -forms is denoted . On a compact manifold it is finite-dimensional, and the Hodge theorem identifies it with degree- de Rham cohomology.
Examples and near-misses
On a flat torus, differential forms with constant coefficients are harmonic. In degree zero, harmonic forms are precisely harmonic functions; on a connected compact manifold every such function is constant.
The function on is a decisive noncompact warning: with the Euclidean metric, , but . Hence a harmonic smooth form on a noncompact manifold need not be closed and coclosed under the unrestricted smooth definition. -harmonic forms require a specified self-adjoint realization and are a separate analytic setting.
References
- Mark Andrea A. de Cataldo, The Hodge Theory of Projective Manifolds, Imperial College Press, 2007. Author-hosted book PDF. Relevant: §2.3, especially Definition 2.3.1 and Lemma 2.3.2.
- Raymond O. Wells, Jr., Differential Analysis on Complex Manifolds, 3rd ed., Springer, 2008. Springer DOI record. Relevant: Chapter IV, §2 on harmonic forms and Hodge theory.