Bellettini’s Sheeting Theorem and Schoen–Simon Regularity

Theorem 4.4.1

Suppose \(M\) is a properly immersed, two-sided, stable minimal hypersurface in \(B^{n+1}_4(0)\) with \(\mathcal{H}^{n-2}(\mathrm{sing}(M))\lt{}\infty\) and

\[ \mathcal{H}^n(M\cap B^{n+1}_4(0))\leq \Lambda . \]

Then there exists \(\varepsilon=\varepsilon(n,\Lambda)\gt{}0\) such that if

\[ \int_{M\cap B^{n+1}_4(0)} \text{dist}(x,P)^2 d\mathcal{H}^n \leq \varepsilon \]

for \(P=\{ x_{n+1}=0 \}\), then \(\pi:M \cap B^n_1(0)\times \mathbb{R}\backslash \pi^{-1}(\Sigma)\to B^n_1(0)\backslash \Sigma\) is a smooth projection map, where \(\Sigma\) is the projection of \(\text{sing}(M)\) to \(P\) in \(B^n_1(0)\).

In particular, if \(\mathcal{H}^{n-2}(\text{sing}(M))=0\), then \(\Sigma=\emptyset\) and \(M\cap B^n_1(0)\times \mathbb{R}\) is a union of minimal graphs over \(B^n_1(0)\).

Theorem 4.4.2

Suppose \(M\) is a properly immersed, two-sided, stable minimal hypersurface in \(B^{n+1}_4(0)\) with \(\mathcal{H}^{n-2}(\mathrm{sing}(M))\lt{}\infty\) and

\[ \mathcal{H}^n(M\cap B^{n+1}_4(0))\leq \Lambda . \]

Then, there exists \(\varepsilon=\varepsilon(n,\Lambda)\gt{}0\) such that if

\[ \int_{M\cap B^{n+1}_4(0)} |x_{n+1}|^2 d\mathcal{H}^n \leq \varepsilon, \]

then

\[ g(x)\leq C \left( \int_{M\cap B_{2}(0)} g^{2}(x) \right)^{\frac{4}{4+n}}. \]

Here, \(g(x)=\sqrt{1-(\nu \cdot e_{n+1})^{2}}\) where \(\nu\) is the unit normal vector of \(M\).

Geometric meaning of \(g\).

Definition 4.4.3

The tilt excess of \(M\) in \(B^{n+1}_r(0)\) with respect to \(P=\{ x_{n+1}=0 \}\) is

\[ E_M(r,P):=r^{-n}\int_{M\cap B^{n+1}_r(0)} |T_x M - P|^{2} d\mathcal{H}^n. \]

For the codimensional one case, one can use \(|\nu-e_{n+1}||\nu+e_{n+1}|\) as the distance between \(T_x M\) and \(P\). We have

\[ |T_xM-P|^{2}\simeq |\nu-e_{n+1}|^{2}|\nu+e_{n+1}|^{2}=4(1-(\nu \cdot e_{n+1})^{2})=4g^{2}. \]

This agrees with the standard definition of tilt excess up to a constant multiple.

Lemma 4.4.4

For any \(k\in [0,\frac{1}{2n}]\), we have

\[ \frac{1}{2n}\int_{ \{ g\gt{}k \}} |\nabla g|^{2} \left( 1-\frac{k}{g} \right) \phi^{2} \leq \int_{\{ g\gt{}k \} } (g-k) ^{2}|\nabla \phi|^{2}. \]

for any Lipschitz function \(\phi\) supported in \(B^{n+1}_{\frac{3}{2}}(0)\).

Proof. Choose \((g-k)^+ \phi\) as a test function in the stability inequality, together with

\[ g\Delta g = - \frac{|\nabla g|^{2}}{1-g^{2}}+|A|^{2}(1-g^{2}) \]

and

\[ \frac{|\nabla g|^{2}}{1-g^{2}}\leq \frac{n-1}{n}|A|^{2}, \]

we can finish the proof for this lemma for the \(\phi\) with compact support in the regular part of \(M\). The general case can be obtained by a standard cut-off argument near the singular set of \(M\).

The proof for \(\varepsilon\)-regularity theorem for the tilt is similar to the proof of the previous \(\varepsilon\)-regularity theorem for \(|A|\), as we only need to repeat the de Giorgi iteration process.

The proof of the sheeting theorem is as follows.

Note that by the 1st variation formula, (by choosing \(X = \phi^{2}x_{n+1}e_{n+1}\)) we have

\[ \int_{ } g^{2} \phi^{2} \leq 4 \int_{ } |x_{n+1}|^{2} |\nabla \phi|^{2}. \]

So

\[ \int_{ B_2} g^{2} \leq C \int_{ B_4} |x_{n+1}|^{2} \leq C \varepsilon \]

Then, given any \(\delta\gt{}0\), we can choose \(\varepsilon\) small enough such that \(g\lt{}\delta\) in \(B_1^n \times \mathbb{R}\cap \text{reg}(M)\) by the \(\varepsilon\)-regularity theorem for the tilt. In particular, each small regular region of \(M\cap B_1^n \times \mathbb{R}\) can be written as a graph over a domain in \(P\) with small gradient. Then, by the connectedness of \(M\cap B_1^n \times \mathbb{R}\) away from the singular set, we know \(M\cap B_1^n \times \mathbb{R}\backslash \pi^{-1}(\Sigma)\) can be written as a graph of smooth multiple valued function (locally, it is the union of smooth graphs) over \(B_1^n \backslash \Sigma\). This can be viewed as a covering map from \(M\cap B_1^n \times \mathbb{R}\backslash \pi^{-1}(\Sigma)\) to \(B_1^n \backslash \Sigma\).

In addition, if \(\mathcal{H}^{n-2}(\text{sing}(M))=0\), then \(B_1^n \backslash \Sigma\) is simply connected. So the covering map is trivial, and hence \(M\cap B_1^n \times \mathbb{R}\) is a union of minimal graphs over \(B_1^n(0)\backslash \Sigma\). Again by the removable singularity theorem, each graph can be extended to a smooth minimal graph over \(B_1^n(0)\). ◻

Theorem 4.4.5

Let \(\{M_k\}\) be a sequence of embedded, stable, orientable minimal hypersurfaces in \(B_2^{n+1}(0)\) with the following properties:

  1. \(0\in \bar{M}_k\) for each \(k\).

  2. \(\mathcal{H}^{n-2}(\mathrm{sing}M_k)=0\) for each \(k\).

  3. \(\|M_k\|(B_2^{n+1}(0))\leq \Lambda\) for some constant \(\Lambda\gt{}0\) independent of \(k\).

Then, up to a subsequence, \(M_k\) converges in the varifold sense to a stable minimal hypersurface \(M\) in \(B_2^{n+1}(0)\), which is smooth except for a closed singular set of Hausdorff dimension at most \(n-7\).

Proof. By Allard’s compactness theorem, up to a subsequence we have \(|M_i|\to V\) in the varifold sense.

Let \(S=\mathrm{sing}\|V\|\) be the embedded singular point set of \(V\). By Federer’s dimension-reduction argument, it suffices to prove the following lemma.

Lemma 4.4.6

For any \(\boldsymbol{C} \in \mathrm{VarTan}(V,x_0)\) for \(x_0 \in S \cap B^{n+1}_{\frac{1}{2}}(0)\), we can write \(\boldsymbol{C}=\boldsymbol{C}'\times \mathbb{R}^{n-p}\) for some \(p\geq 7\).

The proof of this lemma is similar to that of Lemma 4.3.7. We construct the iterated tangents of \(V\) at \(x_0 \in S\) as \(\{ \boldsymbol{C}_1,\cdots , \boldsymbol{C}_N \}\) with the following:

  1. \(x_j \in \mathrm{sing}\|\boldsymbol{C}_j\|\backslash \mathcal{S}(\boldsymbol{C}_j)\) for each \(1\leq j\leq N-1\) and \(\boldsymbol{C}_{j+1} \in \mathrm{VarTan}(\boldsymbol{C}_j,x_j)\).

  2. Each \(\boldsymbol{C}_j\) is not smoothly embedded (i.e., \(\mathrm{sing}\|\boldsymbol{C}_j\|\neq \emptyset\)).

  3. \(\mathrm{dim}(\mathcal{S}(\boldsymbol{C}_{j+1}))\gt{}\mathrm{dim}(\mathcal{S}(\boldsymbol{C}_{j}))\) for each \(j=1,2,\cdots ,N-1\).

  4. \(\boldsymbol{C}_N=\boldsymbol{C}'\times \mathbb{R}^{\mathrm{dim}(\mathcal{S}(\boldsymbol{C}_N))}\) where \(\boldsymbol{C}'\backslash \left\{ 0 \right\}\) is a smooth embedded cone after a suitable rotation in \(\mathbb{R}^{n+1}\).

  5. For each \(1\leq j\leq N\), we can find a sequence of points \(\left\{ y_k \right\}\) with \(y_k\to x_0\), a sequence of positive real numbers \(\left\{ r_k \right\}\) with \(r_k\to 0^+\) as \(k\to \infty\), such that \(\eta_{y_k,r_k}(M_k)\) converges to \(\boldsymbol{C}_j\) in the sense of varifolds and the convergence is smooth away from the singular set of \(\boldsymbol{C}_j\) by sheeting theorem.

We need to show that \(\boldsymbol{C}'\) has dimension at least \(7\). If the dimension of \(\boldsymbol{C}'\) is one, then \(\boldsymbol{C}_N\) is the sum of distinct half-hyperplanes with multiplicity.

For simplicity, we denote

\[ \boldsymbol{C}_N=\sum_{i=1}^{N_1} q_i \{ (\cos \theta_i r, \sin \theta_i r, y): r \geq 0, y \in \mathbb{R}^{n-1} \}. \]

We denote \(\hat{M}_k=\eta_{y_k,r_k}(M_k)\). By the sheeting theorem, for any \(\tau\gt{}0\) and all large \(k\), the set

\[ \hat{M}_k \cap B^{n+1}_2(0)\backslash T_\tau(\boldsymbol{C}_N) \]

decomposes into \(q=\sum_{i=1}^{N_1} q_i\) connected components. Each component is a smooth graph over the corresponding half-hyperplane in \(\boldsymbol{C}_N\).

Now, for \(\mathcal{H}^{n-1}\)-a.e. point \(y \in \mathbb{R}^{n-1}\cap B_1^{n-1}\), Sard’s theorem and \(\mathcal{H}^{n-2}(\mathrm{sing}\,\hat{M}_k)=0\) imply that \(\hat{M}_k \cap B_1^{2} \times \{ y \}\) consists of \(q\) embedded curves for large \(k\).

Choose two pieces \(N_1,N_2 \subset \hat{M}_k\backslash T_\tau(\boldsymbol{C}_N)\) such that \(N_i\) is a graph over a domain in \(\{ (\cos \theta_i r, \sin \theta_i r, y): r \geq \tau, y \in \mathbb{R}^{n-1} \}\) and \(N_1,N_2\) are connected by a curve \(\gamma\) as above.

Note that \(\left\vert \nu(\gamma \cap \{ r=\tau \}\cap N_1)-\nu(\gamma \cap \{ r=\tau \}\cap N_2) \right\vert \geq \frac{1}{2}|\sin(\theta_1 - \theta_2)|\) for \(k\) large enough. So the integral

\[ \int_{ \gamma \cap \{ r\lt{}\tau \}} |A|\geq \frac{1}{2}|\sin(\theta_1 - \theta_2)|. \]

Now, we integrate over all such curves \(\gamma\) for \(\mathcal{H}^{n-1}\)-a.e. point \(y \in \mathbb{R}^{n-1}\cap B_1^{n-1}\), we have

\[ \int_{ \hat{M}_k \cap B_\tau^{2} \times B_1^{n-1}} |A| \geq C \min_{i\neq j}|\theta_i-\theta_j|. \]

But on the other hand, using Cauchy-Schwarz inequality, we have

\[ \begin{aligned} \int_{ \hat{M}_k \cap B_\tau^{2} \times B_1^{n-1}} |A| &\leq \left( \mathcal{H}^n(\hat{M}_k \cap B_\tau^{2} \times B_1^{n-1}) \right)^{\frac{1}{2}} \left( \int_{ \hat{M}_k \cap B_\tau^{2} \times B_1^{n-1}} |A|^{2} \right)^{\frac{1}{2}} \nonumber \\ &\leq C \sqrt{\tau} \end{aligned} \]

for some \(C=C(n,\Lambda)\) independent of \(\tau\) and \(k\) by the monotonicity formula and the stability inequality. Since \(\tau\) is arbitrary, this is a contradiction.

Hence, we know \(\boldsymbol{C}'\) has dimension at least \(2\). But the fifth condition implies that \(\boldsymbol{C}'\) is a smooth embedded stable cone away from \(\{0\}\), and hence \(\boldsymbol{C}'\) has dimension at least \(7\). ◻

Gaoming Wang
Gaoming Wang
Assistant Professor

My research interests include Geometric Analysis and Partial Differential Equations.