Harmonic differential form Created 2026-09-24 Updated 2026-10-14
A differential form is harmonic when it lies in the kernel of the Hodge Laplacian . On a compact manifold, this is equivalent to and .
Its relation to cohomology is part of Hodge theory.
Hodge decomposition theorem Created 2026-09-24 Updated 2026-10-14
On a compact oriented Riemannian manifold,as an -orthogonal direct sum. Every de Rham cohomology class consequently has a unique harmonic representative.
This orthogonal-splitting theorem is one result of Hodge theory.
Hodge decomposition theorem for compact Kähler manifolds Created 2026-09-24 Updated 2026-10-14
This is the compact Kähler specialization of Hodge theory.
For a smooth -form on the complex projective line, solve its Dolbeault operator equation on a disc about zero and a disc about infinity. The difference of the primitives is a holomorphic function on their annular overlap. Split its Laurent series into a nonnegative-power part extending to the finite disc and a negative-power part extending holomorphically across infinity. Subtract the first part from the finite primitive and add the second to the infinite primitive. The results agree and define a global primitive, without Hodge theory.
Past exam of the mathematics course of the University of Cambridge 2005 iii Paper 21 5 c Solution Created 2026-10-03 Updated 2026-10-14
For a complex K3 surface, is torsion-free and has its integral cup product pairingThe K3 intersection lattice isthe even unimodular integral quadratic lattice of signature . Here is the hyperbolic plane with Gram matrixand is the negative of the positive-definite E8 lattice. Thus the rank is and the pairing has determinant of absolute value one.
These invariants can be checked from the topology and Hodge theory. The trivial canonical bundle and give . The Noether formula gives , which is the topological Euler characteristic. Since is simply connected, , so and . Integral Poincare duality gives unimodularity; the universal coefficient sequence and give torsion-freeness of .
Its second Stiefel–Whitney class is the reduction modulo two of , hence zero. The characteristic-class identitymakes the lattice even. Finally the real and imaginary parts of a holomorphic two-form give two positive directions, a Kähler class gives a third, and the primitive real classes are negative definite by the Hodge–Riemann bilinear relations. Therefore the signature is . The classification of indefinite even unimodular lattices then identifies the displayed lattice uniquely. In particular the Picard group is only the integral part; it should not be confused with this rank-twenty-two topological lattice.