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    <title>Stability | Gaoming Wang</title>
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    <description>Stability</description>
    <generator>Wowchemy (https://wowchemy.com)</generator><language>en-us</language><copyright>© 2026 Gaoming Wang</copyright><lastBuildDate>Mon, 14 Sep 2026 15:19:59 +0000</lastBuildDate>
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      <title>Stability</title>
      <link>https://gaomw.com/tag/stability/</link>
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    <item>
      <title>The stable Bernstein theorem in $\mathbb{R}^{7}$</title>
      <link>https://gaomw.com/publication/stablebernsteinr7/</link>
      <pubDate>Mon, 14 Sep 2026 15:19:59 +0000</pubDate>
      <guid>https://gaomw.com/publication/stablebernsteinr7/</guid>
      <description>&lt;h2 id=&#34;main-theorem&#34;&gt;Main theorem&lt;/h2&gt;
&lt;div class=&#34;publication-results-grid publication-proof-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Stable Bernstein theorem&lt;/p&gt;
    &lt;h3&gt;Flatness in $\mathbb R^7$&lt;/h3&gt;
    &lt;p&gt;Every smooth, connected, complete, two-sided stable minimal immersion $F:M^6\to\mathbb R^7$ has $A\equiv0$, and its image is a hyperplane. No properness, volume-growth, or curvature bound is assumed.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-architecture&#34;&gt;Proof architecture&lt;/h2&gt;
&lt;p&gt;The proof first establishes all subcritical Green-function moments, then uses
critical energy identities and the terminal Green flux to force flatness.
Write $A$ for the second fundamental form and $G$ for the minimal positive
Green function with a unit pole. For a fixed small $t_0&amp;gt;0$, set&lt;/p&gt;
&lt;p&gt;$$
J(t)=\int_{{G=t}}|\nabla G|^3,dA_g,
\qquad
\mathcal M_\sigma=\int_0^{t_0}J(t)t^{-\sigma-1},dt.
$$&lt;/p&gt;
&lt;h3 id=&#34;part-i--all-subcritical-moments&#34;&gt;Part I · All subcritical moments&lt;/h3&gt;
&lt;div class=&#34;publication-results-grid publication-proof-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 1 · Preparation&lt;/p&gt;
    &lt;h3&gt;Geometric reduction and Green functions&lt;/h3&gt;
    &lt;p&gt;A blow-up argument reduces the problem to bounded curvature. Unit Green flux and the estimate $|\nabla G|\leq CG$ give the initial integrability range $\mathcal M_\sigma&amp;lt;\infty$ for $\sigma&amp;lt;2$. The target is every $\sigma&amp;lt;5/2$, the critical exponent in dimension six.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 2 · Initial improvement&lt;/p&gt;
    &lt;h3&gt;From $2$ to $2.46$&lt;/h3&gt;
    &lt;p&gt;Bochner&#39;s formula, Simons&#39; identity, stability, and the divergence-free tensor $\tfrac12|A|^2g-A^2$ supply the integral identities. The full Codazzi constraint sharpens the directional estimates, while a Schoen–Simon–Yau inequality retaining its Laplacian term controls cutoff errors. Moment continuation yields $\mathcal M_{2.46}&amp;lt;\infty$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 3 · Nonlinear stability&lt;/p&gt;
    &lt;h3&gt;From $2.46$ to $2.4962$&lt;/h3&gt;
    &lt;p&gt;Apply stability to a nonlinear norm combining a curvature test function and a Green-gradient test function. Differentiating this norm retains an extra nonnegative gradient term. Together with the Green and curvature identities, it gives coercive estimates on fifteen rational parameter intervals and proves $\mathcal M_{2.4962}&amp;lt;\infty$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 4 · Spectral coercivity&lt;/p&gt;
    &lt;h3&gt;Every exponent below $5/2$&lt;/h3&gt;
    &lt;p&gt;Additional divergence identities for homogeneous curvature tensors involving $A^4$, $\operatorname{tr}(A^3)A$, and $\operatorname{tr}(A^4)g$ strengthen the coercive estimate near the critical exponent. They continue the moment range from $2.4962$ to every $\sigma&amp;lt;5/2$.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h3 id=&#34;part-ii--critical-energies-and-rigidity&#34;&gt;Part II · Critical energies and rigidity&lt;/h3&gt;
&lt;div class=&#34;publication-results-grid publication-proof-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 5 · Critical energies&lt;/p&gt;
    &lt;h3&gt;Remove the exterior cutoffs&lt;/h3&gt;
    &lt;p&gt;All subcritical moments are now finite. An elementary spectral inequality, stability, and Simons&#39; identity give finite critical curvature and derivative energies. The argument uses each fixed subcritical moment, with no uniform bound required as $\sigma\uparrow5/2$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 6 · Rigidity&lt;/p&gt;
    &lt;h3&gt;Terminal flux forces flatness&lt;/h3&gt;
    &lt;p&gt;The energy bounds give finite limits of the normalized Green flux $t^{-5/2}J(t)$ at both ends. Brendle&#39;s sharp isoperimetric inequality determines the sign of the terminal Bochner boundary term. Combining this sign with the critical spectral inequality forces the critical curvature energy to vanish, so $A\equiv0$.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
</description>
    </item>
    
    <item>
      <title>Stable Minimal Hypersurfaces in Positively Curved $4$-Manifolds</title>
      <link>https://gaomw.com/publication/stablepositivecurvature/</link>
      <pubDate>Sun, 23 Aug 2026 07:45:35 +0000</pubDate>
      <guid>https://gaomw.com/publication/stablepositivecurvature/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This paper studies complete two-sided stable minimal hypersurfaces of dimension
three in positively curved four-manifolds.  It identifies the curvature gap
that forces rigidity and shows, by an explicit construction, why that gap is
essential.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Rigidity&lt;/p&gt;
    &lt;h3&gt;Positive scalar curvature forces total geodesicity&lt;/h3&gt;
    &lt;p&gt;If the ambient sectional curvature is nonnegative and the ambient scalar curvature satisfies $\overline R\geq\kappa&gt;0$, then every complete, connected, two-sided stable minimal immersion $M^3\to X^4$ has $A\equiv0$ and $\overline{\operatorname{Ric}}(\nu,\nu)\equiv0$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Sharpness&lt;/p&gt;
    &lt;h3&gt;The uniform scalar curvature gap is necessary&lt;/h3&gt;
    &lt;p&gt;There is a complete metric with strictly positive sectional curvature on $\mathbb R^4$ containing a complete, embedded, one-ended, nonparabolic, two-sided stable minimal hypersurface $\Sigma^3\cong\mathbb R^3$ that is not totally geodesic.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Improvement&lt;/p&gt;
    &lt;h3&gt;No bounded-geometry or upper-curvature hypothesis&lt;/h3&gt;
    &lt;p&gt;The rigidity theorem removes the weakly bounded geometry assumption from the earlier result of Chodosh--Li--Stryker.  It also requires no uniform upper bound for the ambient sectional curvature.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-architecture&#34;&gt;Proof architecture&lt;/h2&gt;
&lt;p&gt;The argument replaces extrinsic volume comparison by an intrinsic spectral and
potential-theoretic route.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 1&lt;/p&gt;
    &lt;h3&gt;Spectral and topological reduction&lt;/h3&gt;
    &lt;p&gt;A positive Jacobi function turns stability into spectral Ricci and scalar curvature inequalities.  Sharp splitting and topology theorems reduce the only nontrivial case to a one-ended manifold diffeomorphic to $\mathbb R^3$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 2&lt;/p&gt;
    &lt;h3&gt;Separating warped $\mu$-bubbles&lt;/h3&gt;
    &lt;p&gt;Escaping warped $\mu$-bubble separators are constructed with a uniform integral estimate for their mean curvature, the prescribed curvature term, and the normal derivative of the Jacobi weight.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Step 3&lt;/p&gt;
    &lt;h3&gt;Harmonic functions and flux&lt;/h3&gt;
    &lt;p&gt;A level-set identity gives a uniform $L^1$ bound for capacitor gradients.  Nonparabolicity would contradict conservation of flux, so the hypersurface is parabolic; stability cutoffs then force the Jacobi potential to vanish identically.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;the-counterexample-mechanism&#34;&gt;The counterexample mechanism&lt;/h2&gt;
&lt;p&gt;Starting from the Chodosh&amp;ndash;Li&amp;ndash;Stryker positively curved model, the ambient
metric is changed only near a compact subset of a totally geodesic stable
hypersurface.  The perturbation introduces a nonzero trace-free second
fundamental form while preserving both the induced metric and the Jacobi
potential&lt;/p&gt;
&lt;p&gt;$$
|A|^2+\overline{\operatorname{Ric}}(\nu,\nu).
$$&lt;/p&gt;
&lt;p&gt;Thus completeness, minimality, and stability remain unchanged, while the
hypersurface ceases to be totally geodesic.  Because the deformation is compactly
supported and small in $C^2$, strict positivity of sectional curvature is
preserved.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>Regularity of branched stable minimal immersed hypersurfaces</title>
      <link>https://gaomw.com/publication/regularitybranchedstable/</link>
      <pubDate>Fri, 31 Jul 2026 17:09:37 +0000</pubDate>
      <guid>https://gaomw.com/publication/regularitybranchedstable/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This work develops a regularity theory for branched stable minimal immersed
hypersurfaces.  The conclusions are sharp, and the examples show that the
remaining singularities are a genuine feature of the immersed setting rather
than an artifact of the proof.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Sharp regularity&lt;/p&gt;
    &lt;h3&gt;An optimal bound for non-branch singularities&lt;/h3&gt;
    &lt;p&gt;The non-branch singular set is empty in dimension $n=2$, discrete in dimension $n=3$, and has Hausdorff dimension at most $n-3$ for every $n\geq4$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Sharpness examples&lt;/p&gt;
    &lt;h3&gt;A stable cone with a genuine non-branch singularity&lt;/h3&gt;
    &lt;p&gt;We construct a non-flat stable minimal cone in $\mathbb R^4$ arising from a branched minimal immersion.  Its products with Euclidean factors attain the $n-3$ bound in every dimension $n\geq3$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Analytic mechanism&lt;/p&gt;
    &lt;h3&gt;A branched sheeting theory&lt;/h3&gt;
    &lt;p&gt;The proof combines a generalized Schoen inequality with a sheeting theorem near stationary classical cones and unions of hyperplanes.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;starting-model-for-the-construction&#34;&gt;Starting model for the construction&lt;/h2&gt;
&lt;p&gt;The construction of our sharpness examples starts from a minimal surface in
$\mathbb S^3$ obtained by desingularizing two orthogonal Clifford tori.
The image below visualizes this starting model, which provides the geometric
input for the subsequent construction of a branched stable minimal cone in
$\mathbb R^4$.&lt;/p&gt;
&lt;figure style=&#34;max-width: 560px; margin: 1.75rem auto 2.5rem;&#34;&gt;
  &lt;img src=&#34;starting-model.png&#34; width=&#34;1600&#34; height=&#34;1600&#34; loading=&#34;lazy&#34; alt=&#34;Bronze rendering of the starting surface obtained by desingularizing two orthogonal Clifford tori, shown in stereographic projection.&#34; style=&#34;display: block; width: 100%; height: auto; border-radius: 12px;&#34;&gt;
  &lt;figcaption style=&#34;margin-top: 0.85rem; font-size: 0.85rem; line-height: 1.6; text-align: left;&#34;&gt;Starting model for the sharpness examples: a numerical visualization of the $m=30$ Choe–Soret surface in $\mathbb S^3$, shown in stereographic projection. This depicts the starting surface, not the final branched stable cone. The bronze finish and pedestal are presentation elements.&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;h2 id=&#34;companion-materials&#34;&gt;Companion materials&lt;/h2&gt;
&lt;p&gt;The two resources below give a closer view of how the project developed and
of the geometry behind one of its principal examples.&lt;/p&gt;
&lt;div class=&#34;publication-companion-grid&#34;&gt;
  &lt;article class=&#34;publication-companion-card publication-companion-card--note&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Research record&lt;/p&gt;
    &lt;h3&gt;How we found the test function&lt;/h3&gt;
    &lt;p&gt;This note follows the route from the capillary prototype through numerical screening, the small-$k$ expansion, the local linear repair, and the cutoff ODE.  GitHub Copilot and Cursor Composer 2 were used chiefly to turn hand calculations into rapidly testable code; the numerical evidence guided the choice of formula, while the final verification remained analytic.&lt;/p&gt;
    &lt;div class=&#34;publication-companion-actions&#34;&gt;
      &lt;a class=&#34;btn btn-primary&#34; href=&#34;https://gaomw.com/notes/test-function-discovery/&#34;&gt;Read the HTML note&lt;/a&gt;
      &lt;a class=&#34;btn btn-outline-primary&#34; href=&#34;https://gaomw.com/uploads/test-function-discovery-note.pdf&#34;&gt;Download the PDF&lt;/a&gt;
    &lt;/div&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-companion-card publication-companion-card--viewer&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Interactive geometry&lt;/p&gt;
    &lt;h3&gt;Desingularization of two orthogonal Clifford tori&lt;/h3&gt;
    &lt;p&gt;An interactive 3D viewer provides a geometric preview of the desingularization: rotate and zoom the model, or isolate individual regions to inspect how the two tori are joined.&lt;/p&gt;
    &lt;div class=&#34;publication-companion-actions&#34;&gt;
      &lt;a class=&#34;btn btn-primary&#34; href=&#34;https://gaomw.com/interactive/branched-stable-example/&#34;&gt;Open the 3D viewer&lt;/a&gt;
    &lt;/div&gt;
  &lt;/article&gt;
&lt;/div&gt;
</description>
    </item>
    
    <item>
      <title>A splitting theorem for manifolds with spectral nonnegative Ricci curvature and mean-convex boundary</title>
      <link>https://gaomw.com/publication/splitcurve/</link>
      <pubDate>Fri, 23 Jan 2026 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/splitcurve/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This paper proves a boundary splitting theorem under a spectral, rather than
pointwise, lower bound for Ricci curvature.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Spectral splitting&lt;/p&gt;
    &lt;h3&gt;An interior end forces a half-product&lt;/h3&gt;
    &lt;p&gt;Let $M^n$ have mean-convex boundary and $\lambda_1(-\alpha\Delta+\operatorname{Ric})\geq0$ for $\alpha&lt;4/(n-1)$.  If $M$ has an interior end, then it is isometric to $\Sigma\times\mathbb R_{\geq0}$ with $\Sigma$ closed and $\operatorname{Ric}_\Sigma\geq0$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Dichotomy&lt;/p&gt;
    &lt;h3&gt;Otherwise there are no interior ends&lt;/h3&gt;
    &lt;p&gt;The theorem allows a possibly noncompact boundary and gives a sharp alternative: either the product splitting occurs or every end of the manifold remains attached to the boundary.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Geometric application&lt;/p&gt;
    &lt;h3&gt;Stable free-boundary CMC hypersurfaces inherit the dichotomy&lt;/h3&gt;
    &lt;p&gt;In dimensions $n\leq4$, suitable nonnegative biRic curvature and mean convexity imply the same product-or-no-interior-end conclusion for complete two-sided stable free-boundary constant-mean-curvature immersions.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-strategy&#34;&gt;Proof strategy&lt;/h2&gt;
&lt;p&gt;A positive solution of the spectral Ricci equation defines the weighted length
functional $L_u^\alpha$.  An interior end produces a free-boundary weighted
minimizing ray, and a curve-capture argument constructs such a ray or line
through every point.  Its second variation forces the weight to be constant
and hence upgrades spectral nonnegativity to pointwise $\operatorname{Ric}\geq0$;
the classical boundary splitting theorem then finishes the proof.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>A splitting theorem for 3-manifold with nonnegative scalar curvature and mean-convex boundary</title>
      <link>https://gaomw.com/publication/spiltcapillary/</link>
      <pubDate>Thu, 16 Jan 2025 04:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/spiltcapillary/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This work proves scalar-curvature splitting theorems for noncompact
three-manifolds with mean-convex boundary, using noncompact minimizing
free-boundary and capillary surfaces as the rigidifying objects.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Free-boundary splitting&lt;/p&gt;
    &lt;h3&gt;A minimizing half-cylinder or strip forces flatness&lt;/h3&gt;
    &lt;p&gt;If the manifold contains an absolutely area-minimizing free-boundary half-cylinder or strip, then it is flat.  Up to scaling, the resulting models are covered by $\mathbb S^1\times\mathbb R^2_+$ or are isometric to $[0,1]\times\mathbb R^2$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Capillary extension&lt;/p&gt;
    &lt;h3&gt;The theorem holds for every contact angle&lt;/h3&gt;
    &lt;p&gt;For $\theta\in(0,\pi)$, an absolutely $\theta$-energy-minimizing half-cylinder gives the corresponding tilted flat model; the strip statement also holds when its two boundary curves lie on different boundary components.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;No compact-boundary hypothesis&lt;/p&gt;
    &lt;h3&gt;The ambient boundary may be noncompact or disconnected&lt;/h3&gt;
    &lt;p&gt;The argument requires neither compactness nor a prescribed number of components of $\partial M$, extending earlier boundary splitting theorems beyond their usual global assumptions.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-strategy&#34;&gt;Proof strategy&lt;/h2&gt;
&lt;p&gt;Plateau-type problems in carefully chosen prism-shaped domains produce a
sequence of minimizing capillary surfaces near the given noncompact surface.
Stability classifies the possible limits, while energy comparisons rule out
unwanted disk, half-plane, plane, and cylinder degenerations.  The surviving
half-cylinders or strips form a rigid family; equality in the scalar-curvature
and boundary inequalities then propagates to an ambient flat product.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>On $\delta$-Stable Minimal Hypersurfaces in $\mathbb{R}^{n&#43;1}$</title>
      <link>https://gaomw.com/publication/deltastability/</link>
      <pubDate>Thu, 04 Jul 2024 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/deltastability/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The paper extends regularity, compactness, and Bernstein theory from stable
minimal hypersurfaces to the weaker notion of $\delta$-stability.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Regularity and compactness&lt;/p&gt;
    &lt;h3&gt;A quantitative theory above the catenoid threshold&lt;/h3&gt;
    &lt;p&gt;For $n\geq3$ and $\delta&gt;(n-2)/n$, sequences with uniform area control admit varifold subsequences whose singular sets satisfy an explicit dimension bound determined by $\delta$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Bernstein theorem&lt;/p&gt;
    &lt;h3&gt;Flatness in dimensions three and four&lt;/h3&gt;
    &lt;p&gt;For $n=3,4$, complete two-sided $\delta$-stable immersed hypersurfaces are flat under either a stronger numerical stability range or the combination of simple connectivity, properness, and finitely many ends.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Sharp threshold&lt;/p&gt;
    &lt;h3&gt;The lower bound on $\delta$ cannot be improved&lt;/h3&gt;
    &lt;p&gt;The $n$-dimensional catenoid is exactly $(n-2)/n$-stable.  Simons-type cones also identify the sharp threshold for the cone-classification component of the theory.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-strategy&#34;&gt;Proof strategy&lt;/h2&gt;
&lt;p&gt;The regularity argument combines a Caccioppoli inequality, De Giorgi
iteration, an $\varepsilon$-regularity theorem for the second fundamental
form, and tangent-cone analysis.  A sharp classification of $\delta$-stable
minimal cones supplies the dimension reduction.  In low dimensions,
point-picking and curvature estimates reduce the Bernstein statements to the
global flatness results.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>Generalized Bernstein Theorem for Stable Minimal Plateau Surfaces</title>
      <link>https://gaomw.com/publication/plateausurfaces/</link>
      <pubDate>Thu, 20 Oct 2022 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/plateausurfaces/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The classical Bernstein question is extended from smooth minimal surfaces to
Plateau surfaces, whose local models may also contain $Y$- and $T$-type soap-film
singularities.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Generalized Bernstein theorem&lt;/p&gt;
    &lt;h3&gt;Stability and quadratic area growth force flatness&lt;/h3&gt;
    &lt;p&gt;If a complete orientable minimal Plateau surface in $\mathbb R^3$ is stable and has at most quadratic area growth, then every component of its regular part lies in a plane.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;No $T$-points&lt;/p&gt;
    &lt;h3&gt;The surface is cylindrical over a planar network&lt;/h3&gt;
    &lt;p&gt;When no $T$-type singularity occurs, the surface is, after a rigid motion, of the form $N\times\mathbb R$ for an embedded stationary network $N\subset\mathbb R^2$.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;With $T$-points&lt;/p&gt;
    &lt;h3&gt;Only two global configurations remain&lt;/h3&gt;
    &lt;p&gt;If $T$-type singularities occur, there is either one such point and the surface is the standard $T$ cone, or there are exactly two points joined in the explicitly classified flat configuration.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-strategy&#34;&gt;Proof strategy&lt;/h2&gt;
&lt;p&gt;The proof transfers the stability inequality to the regular sheets while
retaining the balancing information along the singular curves.  Curvature
estimates and logarithmic cutoffs, made possible by quadratic area growth,
force the second fundamental form to vanish.  Once each sheet is planar, the
topology and Plateau angle conditions reduce the remaining work to a global
classification of the straight $Y$-curves and isolated $T$-points.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>Curvature Estimates for Stable Minimal Surfaces with a Common Free Boundary</title>
      <link>https://gaomw.com/publication/curvature-estimate-triple/</link>
      <pubDate>Thu, 19 May 2022 11:41:35 +0800</pubDate>
      <guid>https://gaomw.com/publication/curvature-estimate-triple/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The paper extends curvature estimates and Bernstein-type rigidity from smooth
minimal surfaces to weighted multiple-junction surfaces sharing a common free
boundary.&lt;/p&gt;
&lt;div class=&#34;publication-results-grid&#34;&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--regularity&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Curvature estimate&lt;/p&gt;
    &lt;h3&gt;An $L^p$ theory compatible with the junction&lt;/h3&gt;
    &lt;p&gt;For stable minimal multiple-junction surfaces, the second fundamental forms satisfy an $L^{2p}$ estimate for $1&lt;p&lt;5/4$, with the boundary contribution expressed explicitly through the junction curvature and conormal derivatives.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--examples&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Compact junction&lt;/p&gt;
    &lt;h3&gt;Quadratic growth forces every sheet to be flat&lt;/h3&gt;
    &lt;p&gt;A complete, orientable, stable minimal multiple-junction surface in $\mathbb R^3$ with quadratic area growth, compact common boundary, and constant pairwise angles has flat sheets.&lt;/p&gt;
  &lt;/article&gt;
  &lt;article class=&#34;publication-result-card publication-result-card--method&#34;&gt;
    &lt;p class=&#34;publication-card-eyebrow&#34;&gt;Straight junction&lt;/p&gt;
    &lt;h3&gt;The same Bernstein conclusion holds along a line&lt;/h3&gt;
    &lt;p&gt;For a triple junction meeting at $120^\circ$, the flatness conclusion also holds when the common boundary is a straight line, under the corresponding completeness, stability, and area-growth assumptions.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;proof-strategy&#34;&gt;Proof strategy&lt;/h2&gt;
&lt;p&gt;Simons&amp;rsquo; inequality is applied sheet by sheet and combined with the global
stability inequality using test functions that satisfy the junction
compatibility condition.  The conormal boundary terms do not disappear
automatically; the weighted balance law reorganizes them into a controllable
expression.  Iteration of the resulting $L^p$ estimate with large cutoffs and
quadratic area growth forces the curvature to vanish.&lt;/p&gt;
</description>
    </item>
    
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