Hodge theory
The Hodge decomposition or the set of Hodge is a central statement of the Hodge theory. This theory combines the mathematical subdivisions analysis, differential geometry and algebraic topology. Named are the Hodge decomposition and the Hodge theory after the mathematician William Vallance Douglas Hodge, who developed this as an extension to the De Rham cohomology in the 1930s.
Elliptic complex
With smooth cuts are referred to in a vector bundle. Be an oriented Riemannian manifold and a sequence of vector bundles. An elliptical complex is a sequence of partial differential operators of the first order
So that the following properties are valid.
- The result is a Kokettenkomplex, it is applicable to all and
- For each of the sequence of principal symbols
The rooms can be understood, for example, than that of differential forms rooms.
Set of Hodge
Let now a compact, oriented Riemannian manifold and the i-th cohomology group of the elliptic complex. In addition, defining a ( Laplace ) operator
By
This is an elliptical operator. Now, the following applies:
- The -th cohomology group is isomorphic to all of the core, ie
- The dimension of the -th cohomology group is for all finite
- There is an orthogonal decomposition
Example: De Rham cohomology
The De Rham complex
Is an elliptical complex. The spaces are the spaces of differential forms of degree i and again is the exterior derivative. The corresponding sequence of the main symbols is the Koszul complex. The operator is the Hodge - Laplace operator. At the core of this operator is called the space of harmonic differential forms, as this is indeed defined analogously to the space of harmonic functions. By the theorem of Hodge now exists an isomorphism between the i-th de Rham cohomology group - and the space of harmonic differential forms of degree.
In addition,
Well-defined figures, as the De Rham cohomology groups have finite dimension. These numbers are called Betti numbers. The Hodge star operator also induces an isomorphism between the spaces and. This is the Poincaré duality and applies for the Betti numbers