ProofComplete

Calabi-Yau Manifolds - Key Proof

We present the key steps in Yau's proof of the Calabi conjecture, focusing on the solution of the complex Monge-Ampère equation. This proof is a landmark achievement in geometric analysis, combining techniques from partial differential equations, differential geometry, and complex analysis.

ProofProof of Calabi-Yau Theorem (Outline)

Let XX be a compact KΓ€hler manifold with c1(X)=0c_1(X) = 0 and let [Ο‰0][\omega_0] be a KΓ€hler class. We seek a KΓ€hler metric Ο‰=Ο‰0+iβˆ‚βˆ‚Λ‰Ο†\omega = \omega_0 + i\partial\bar{\partial}\varphi with Ric(Ο‰)=0\text{Ric}(\omega) = 0.

Step 1: Setup of the Monge-Ampère equation

The Ricci curvature of a KΓ€hler metric satisfies: Ric(Ο‰)=βˆ’iβˆ‚βˆ‚Λ‰log⁑(Ο‰n)\text{Ric}(\omega) = -i\partial\bar{\partial}\log(\omega^n)

For Ο‰=Ο‰0+iβˆ‚βˆ‚Λ‰Ο†\omega = \omega_0 + i\partial\bar{\partial}\varphi to be Ricci-flat, we need: (Ο‰0+iβˆ‚βˆ‚Λ‰Ο†)n=eFΟ‰0n(\omega_0 + i\partial\bar{\partial}\varphi)^n = e^F \omega_0^n

where FF is determined by c1(X)=0c_1(X) = 0. Since c1(X)=0c_1(X) = 0, we have Ric(Ο‰0)=iβˆ‚βˆ‚Λ‰f\text{Ric}(\omega_0) = i\partial\bar{\partial}f for some function ff, so F=βˆ’fF = -f. The equation becomes: det⁑(gijΛ‰+βˆ‚2Ο†βˆ‚ziβˆ‚zΛ‰j)=eβˆ’fdet⁑(gijΛ‰)\det\left(g_{i\bar{j}} + \frac{\partial^2\varphi}{\partial z^i\partial\bar{z}^j}\right) = e^{-f} \det(g_{i\bar{j}})

This is the complex Monge-Ampère equation with φ\varphi as the unknown.

Step 2: Establishing a priori estimates

The core difficulty is obtaining a priori estimates for Ο†\varphi. We need bounds on:

  • C0C^0 norm: βˆ₯Ο†βˆ₯C0≀C0\|\varphi\|_{C^0} \leq C_0
  • Gradient: βˆ£βˆ‡Ο†βˆ£β‰€C1|\nabla\varphi| \leq C_1
  • Higher derivatives: βˆ₯Ο†βˆ₯Ck≀Ck\|\varphi\|_{C^k} \leq C_k

The C0C^0 estimate follows from the maximum principle and the constraint ∫Xeβˆ’f+φω0n=∫XΟ‰0n\int_X e^{-f+\varphi}\omega_0^n = \int_X \omega_0^n.

For the gradient estimate, we use Yau's method: consider the quantity: Q=log⁑trΟ‰0(Ο‰)βˆ’AΟ†Q = \log\text{tr}_{\omega_0}(\omega) - A\varphi

where AA is a large constant. At a maximum point of QQ, the Laplacian Δω0Q\Delta_{\omega_0}Q can be computed using the Monge-AmpΓ¨re equation, yielding: Δω0Qβ‰₯βˆ’C\Delta_{\omega_0}Q \geq -C

for a constant CC independent of Ο†\varphi. This bounds trΟ‰0(Ο‰)\text{tr}_{\omega_0}(\omega) and hence βˆ£βˆ‡Ο†βˆ£|\nabla\varphi|.

Step 3: Higher regularity

Once gradient bounds are established, higher derivative estimates follow from elliptic regularity theory. The linearization of the Monge-Ampère operator is elliptic when ω>0\omega > 0, allowing us to apply the Calderón-Zygmund theory and Schauder estimates.

Specifically, we obtain C2,αC^{2,\alpha} estimates, then bootstrap to C∞C^\infty using the elliptic equation and standard regularity results.

Step 4: Continuity method

With a priori estimates in hand, we use the continuity method. Define a family of equations: (Ο‰0+iβˆ‚βˆ‚Λ‰Ο†t)n=etfΟ‰0n,t∈[0,1](\omega_0 + i\partial\bar{\partial}\varphi_t)^n = e^{tf} \omega_0^n, \quad t \in [0,1]

At t=0t=0, the solution is Ο†0=0\varphi_0 = 0. We show the set S={t∈[0,1]:Ο†tΒ exists}S = \{t \in [0,1] : \varphi_t \text{ exists}\} is both open and closed in [0,1][0,1].

  • Openness: By the implicit function theorem for the Monge-AmpΓ¨re operator
  • Closedness: By the a priori estimates ensuring convergence of solutions

Therefore S=[0,1]S = [0,1], and Ο†1\varphi_1 gives the desired Ricci-flat metric.

Step 5: Uniqueness

Uniqueness follows from the maximum principle. If Ο‰1\omega_1 and Ο‰2\omega_2 are two Ricci-flat metrics in the same KΓ€hler class, then Ο‰1βˆ’Ο‰2=iβˆ‚βˆ‚Λ‰u\omega_1 - \omega_2 = i\partial\bar{\partial}u for some function uu. The difference of the Monge-AmpΓ¨re equations gives: Δω1u=0\Delta_{\omega_1}u = 0

By the maximum principle on compact XX, uu is constant, so Ο‰1=Ο‰2\omega_1 = \omega_2.

β– 

The proof technique has been tremendously influential, leading to solutions of other geometric PDE problems including the KΓ€hler-Einstein problem and various equations in special holonomy.

Remark

Yau's estimates are remarkably robust and have been adapted to prove existence results for Hermitian-Yang-Mills connections (used in the proof of the Hitchin-Kobayashi correspondence) and other geometric structures. The method of proving gradient estimates by considering auxiliary functions that achieve their maximum at interior points has become a standard tool in geometric analysis.

The technical heart of the proof lies in the second-order estimates. These require careful analysis of the geometry and use of the maximum principle in a sophisticated way. The computation at the maximum of the auxiliary function QQ involves intricate manipulations of the curvature tensor and clever choices of test functions.