Moduli Spaces - Core Definitions
Moduli spaces parametrize families of geometric objects, encoding how structures can vary while preserving essential properties. For Calabi-Yau manifolds, the moduli spaces of Kähler and complex structures form the geometric foundation for mirror symmetry.
A moduli space for a class of geometric objects is a space whose points correspond to isomorphism classes of those objects. Local coordinates on parametrize continuous families of deformations.
For a moduli problem to be well-posed, we require:
- A notion of family (flat morphisms)
- An equivalence relation (isomorphism)
- Representability or existence of a coarse moduli space
For Calabi-Yau threefolds , two primary moduli spaces arise naturally from the geometry. The complex structure moduli space parametrizes complex structures preserving the Calabi-Yau condition, while the Kähler moduli space parametrizes Kähler forms modulo diffeomorphism.
The complex structure moduli space of a Calabi-Yau manifold is the space of complex structures on the underlying smooth manifold that preserve , modulo diffeomorphisms isotopic to the identity.
The tangent space at a point is:
where the isomorphism follows from Dolbeault cohomology and Serre duality.
The dimension of equals near smooth points. Infinitesimal deformations are controlled by the Kodaira-Spencer map, which associates to each tangent vector a class in .
The Kähler moduli space parametrizes Kähler classes with a positive -form. The tangent space is:
The dimension of is .
The Kähler cone consists of classes representable by Kähler forms. This is an open convex cone whose boundary corresponds to degenerate geometries.
The total moduli space has dimension . Mirror symmetry exchanges these two factors: for a mirror pair , the complex structure moduli of correspond to Kähler moduli of and vice versa.
For the quintic threefold , we have and . Thus while . The mirror quintic has and , demonstrating the moduli space exchange.
The geometry of these moduli spaces is highly constrained. They carry natural metric structures (Weil-Petersson and special Kähler metrics) and admit canonical coordinates related to period integrals and Yukawa couplings.