ConceptComplete

Moduli of Curves - Key Properties

The moduli stacks Mg,n\mathcal{M}_{g,n} and Mg,n\overline{\mathcal{M}}_{g,n} have rich geometric structure that has been intensively studied. Understanding their properties is fundamental to algebraic geometry.

TheoremIrreducibility and Smoothness

For 2g2+n>02g - 2 + n > 0:

  1. Mg,n\mathcal{M}_{g,n} is a smooth irreducible Deligne-Mumford stack of dimension 3g3+n3g - 3 + n
  2. Mg,n\overline{\mathcal{M}}_{g,n} is a proper Deligne-Mumford stack with normal crossing boundary
  3. The locus of curves with automorphisms has codimension at least 1 for g3g \geq 3

The smoothness is fundamental for intersection theory and deformation theory of curves.

DefinitionBoundary Stratification

The boundary Mg,n=Mg,nMg,n\partial \overline{\mathcal{M}}_{g,n} = \overline{\mathcal{M}}_{g,n} \setminus \mathcal{M}_{g,n} admits a stratification by topological type: Mg,n=ΓMΓ\partial \overline{\mathcal{M}}_{g,n} = \bigcup_{\Gamma} \mathcal{M}_\Gamma where Γ\Gamma ranges over dual graphs. Each stratum MΓ\mathcal{M}_\Gamma is a product of moduli stacks of lower genus or fewer marked points.

ExampleGenus 2 Boundary

For M2\overline{\mathcal{M}}_2, the boundary consists of:

  • Δ0\Delta_0: Irreducible curves with one node (genus 1 curve with 2 points identified)
  • Δ1\Delta_1: Reducible curves (two genus 1 curves meeting at a node)

The boundary divisor is Δ=Δ0+Δ1\Delta = \Delta_0 + \Delta_1, and its class is explicitly computed in the Picard group.

TheoremPicard Group

For g2g \geq 2: Pic(Mg)Q=Q[λ,δ0,,δ[g/2]]\text{Pic}(\overline{\mathcal{M}}_g) \otimes \mathbb{Q} = \mathbb{Q}[\lambda, \delta_0, \ldots, \delta_{[g/2]}] where λ\lambda is the Hodge class and δi\delta_i are boundary classes. Relations come from pullbacks under gluing morphisms.

DefinitionHarel Classes

The ψ\psi-classes ψiA1(Mg,n)\psi_i \in A^1(\overline{\mathcal{M}}_{g,n}) are defined as: ψi=c1(Li)\psi_i = c_1(\mathbb{L}_i) where Li\mathbb{L}_i is the cotangent line bundle to the universal curve at the ii-th marked point. These classes satisfy: ψiMΓ=(boundary terms)\psi_i|_{\mathcal{M}_\Gamma} = \text{(boundary terms)} and generate much of the tautological ring.

TheoremMumford's Conjecture

The stable cohomology ring H(Mg,Q)H^*(\mathcal{M}_g, \mathbb{Q}) as gg \to \infty is a polynomial algebra: H(M,Q)=Q[κ1,κ2,κ3,]H^*(\mathcal{M}_{\infty}, \mathbb{Q}) = \mathbb{Q}[\kappa_1, \kappa_2, \kappa_3, \ldots] where κi\kappa_i are MMumford-Morita-Miller classes. This was proved by Madsen-Weiss using techniques from homotopy theory and is one of the deepest results about moduli of curves.

DefinitionHodge Bundle

The Hodge bundle EMg,n\mathbb{E} \to \overline{\mathcal{M}}_{g,n} has fiber H0(C,ωC)H^0(C, \omega_C) over a curve CC. Its Chern classes: λi=ci(E)Ai(Mg,n)\lambda_i = c_i(\mathbb{E}) \in A^i(\overline{\mathcal{M}}_{g,n}) are fundamental cohomology classes satisfying numerous relations (Faber's conjectures).

Remark

The relationship between ψ\psi-classes, λ\lambda-classes, and boundary classes is governed by complex combinatorics of stable graphs. The tautological ring R(Mg,n)R^*(\overline{\mathcal{M}}_{g,n}) is conjecturally finite-dimensional in each genus, but this remains open for g24g \geq 24.

These properties make Mg,n\overline{\mathcal{M}}_{g,n} one of the most studied objects in algebraic geometry, with connections to topology, number theory, and mathematical physics.