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    <title>Minimal Surfaces | Gaoming Wang</title>
    <link>https://gaomw.com/tag/minimal-surfaces/</link>
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    <description>Minimal Surfaces</description>
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      <title>Minimal Surfaces</title>
      <link>https://gaomw.com/tag/minimal-surfaces/</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>Mixed Radial Volume Comparison under Spectral Ricci Bounds</title>
      <link>https://gaomw.com/publication/mixedradialvolumecomparison/</link>
      <pubDate>Wed, 02 Sep 2026 00:00:00 +0000</pubDate>
      <guid>https://gaomw.com/publication/mixedradialvolumecomparison/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This paper develops radial volume comparison under a spectral lower bound for
Ricci curvature.  The mixed radial construction separates the conformal
geometry used to choose rays from the weights used to truncate and measure
them.&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 comparison&lt;/p&gt;
    &lt;h3&gt;A space-form model for mixed radial balls&lt;/h3&gt;
    &lt;p&gt;Under the spectral inequality $\operatorname{Ric}_g-\alpha(\Delta_g u/u)g\geq(n-1)\kappa g$, the weighted volume of the $g$-arclength mixed radial domain satisfies a scale-invariant comparison with the corresponding space-form volume.&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;Polynomial growth&lt;/p&gt;
    &lt;h3&gt;No pointwise bounds on the spectral weight&lt;/h3&gt;
    &lt;p&gt;For an explicit range of radial and measure exponents, mixed radial balls have polynomial weighted-volume growth.  The optimal exponent can attain the Euclidean value $n$.&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;Applications&lt;/p&gt;
    &lt;h3&gt;Diameter, sharp volume, and stable Bernstein&lt;/h3&gt;
    &lt;p&gt;The comparison gives radial proofs of the spectral Bonnet--Myers and sharp volume theorem of Antonelli--Xu, together with a short volume-growth proof that every complete two-sided stable minimal immersion $M^3\to\mathbb R^4$ is flat.&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 begins with an exact Riccati identity for the weighted radial
Jacobian along geodesics of the conformal metric $h_\alpha=u^{2\alpha}g$.
Taking the $(n-1)$-st root of this Jacobian converts the identity into a
one-dimensional Sturm comparison and yields the space-form estimate.  For
general mixed radial balls, the logarithmic derivatives of the Jacobian and
the spectral weight are instead treated as coupled variables; a quadratic
estimate and a Bellman-type correction produce the polynomial-growth
monotonicity formula.  The positive-curvature case also gives an optimal
diameter bound among smooth closed examples.&lt;/p&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>Spectral splitting theorem and ends of minimal hypersurfaces</title>
      <link>https://gaomw.com/publication/spectralsplitting/</link>
      <pubDate>Thu, 14 May 2026 15:06:46 +0000</pubDate>
      <guid>https://gaomw.com/publication/spectralsplitting/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The paper develops a geodesic-line approach to spectral Ricci curvature and
uses it to control the topology at infinity of minimal hypersurfaces.&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;A weighted minimizing line recovers classical rigidity&lt;/h3&gt;
    &lt;p&gt;If $\lambda_1(-\alpha\Delta+\operatorname{Ric})\geq0$ with $\alpha&lt;4/(n-1)$ and the associated weighted metric admits a minimizing line, then $\operatorname{Ric}\geq0$ pointwise and the manifold splits off an $\mathbb R$ factor.&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;Ends at infinity&lt;/p&gt;
    &lt;h3&gt;Infinitely many ends create a weighted line&lt;/h3&gt;
    &lt;p&gt;Nonnegative spectral Ricci curvature outside a compact set, together with infinitely many ends, forces the existence of a weighted minimizing geodesic line outside a larger compact set.&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;Minimal hypersurfaces&lt;/p&gt;
    &lt;h3&gt;Finite index implies finitely many ends&lt;/h3&gt;
    &lt;p&gt;Every complete two-sided finite-index minimal hypersurface in an ambient manifold of dimension at most five with nonnegative biRic curvature has finitely many ends, without a properness assumption.&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 splitting proof adapts the Cheeger&amp;ndash;Gromoll Busemann-function argument to
the weighted length functional determined by a positive solution of the
spectral equation.  For the application, infinitely many ends are used to
construct a weighted line at infinity; the positive solution is then perturbed
to make the spectral inequality strict outside a compact set.  The second
variation of weighted length produces the contradiction and hence finiteness
of ends.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>Scalar curvature rigidity of domains in a 3-dimensional warped product</title>
      <link>https://gaomw.com/publication/warprigidity/</link>
      <pubDate>Thu, 06 Mar 2025 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/warprigidity/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The paper establishes Llarull-type scalar-curvature rigidity for domains in
three-dimensional spherical warped products, including models with boundary
and singular endpoint geometry.&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;Domain rigidity&lt;/p&gt;
    &lt;h3&gt;Metric, scalar, and boundary comparison determine the model&lt;/h3&gt;
    &lt;p&gt;For a domain whose side boundary is convex in the conformally related product metric, the inequalities $g\geq\bar g$, $R_g\geq R_{\bar g}$, and $H_g\geq H_{\bar g}$ force $g=\bar g$ under the stated endpoint hypotheses.&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;Endpoint geometry&lt;/p&gt;
    &lt;h3&gt;Smooth, conical, and disk-type ends are treated uniformly&lt;/h3&gt;
    &lt;p&gt;The rigidity theorem covers smooth poles, Euclidean or metric tangent cones, and truncations by end disks with matching mean-curvature and angle inequalities.&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;Conical Llarull theorem&lt;/p&gt;
    &lt;h3&gt;Antipodal cone points are allowed&lt;/h3&gt;
    &lt;p&gt;For warped three-spheres with $\psi(t_\pm)=a_\pm|t-t_\pm|+o(|t-t_\pm|)$ and $0&lt;a_\pm\leq1$, metric and scalar-curvature comparison already imply equality, even with the permitted conical singularities.&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;Prescribed-mean-curvature capillary $\mu$-bubbles play the role of the
minimizing hypersurfaces in Llarull&amp;rsquo;s theorem.  The stability inequality and a
Gauss&amp;ndash;Bonnet comparison make a minimizing bubble infinitesimally rigid, and a
local foliation propagates equality through the domain.  Near a vanishing
warping factor or a conical endpoint, local barriers and tangent-cone analysis
replace a formal singular perturbation and ensure that the minimizing problem
cannot escape through the pole.&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>Allard-Type Regularity for Varifolds with Prescribed Contact Angle</title>
      <link>https://gaomw.com/publication/allardregularity/</link>
      <pubDate>Tue, 26 Mar 2024 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/allardregularity/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This paper establishes a boundary Allard theorem for varifolds with prescribed
contact angle, including variable angles and ambient metrics of low regularity.&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;Boundary regularity&lt;/p&gt;
    &lt;h3&gt;A multiplicity-one tangent half-plane gives smooth structure&lt;/h3&gt;
    &lt;p&gt;If a boundary point admits a multiplicity-one tangent half-hyperplane, then the support is locally a $C^{1,\gamma}$ hypersurface with boundary for some $\gamma\in(0,1)$.&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;Contact angle&lt;/p&gt;
    &lt;h3&gt;The variational angle is recovered geometrically&lt;/h3&gt;
    &lt;p&gt;On the regular support, the geometric contact angle is the prescribed angle (apart from the explicitly identified orthogonal alternative); the ambiguity disappears under a natural nonorthogonality condition.&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;Density criterion&lt;/p&gt;
    &lt;h3&gt;Mass control alone suffices in favorable regimes&lt;/h3&gt;
    &lt;p&gt;For two-dimensional varifolds, or in every dimension when the angle is sufficiently close to $90^\circ$, a quantitative boundary density bound implies the required regularity.&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 is carried out in a flattened half-space equipped with a $C^1$
metric, so it remains intrinsic to the codimension-one contact-angle problem.
It combines a boundary monotonicity formula with an $L^2$ height and tilt
estimate, a blow-up analysis, and geometric excess decay.  A reflection idea
inspired by Leon Simon explains how the boundary term and the capillary angle
are incorporated into a stationary comparison object.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>Dihedral rigidity in hyperbolic 3-space</title>
      <link>https://gaomw.com/publication/rigidity/</link>
      <pubDate>Wed, 08 Nov 2023 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/rigidity/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The paper proves hyperbolic analogues of Gromov&amp;rsquo;s dihedral comparison and
rigidity conjectures for tetrahedra and a broad class of prisms.&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;Comparison&lt;/p&gt;
    &lt;h3&gt;All inequalities cannot be simultaneously strict&lt;/h3&gt;
    &lt;p&gt;For the prescribed tetrahedra and prisms, scalar curvature greater than $-6$ and face mean curvature above the hyperbolic reference prevent every dihedral angle from being strictly smaller than its model value.&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;Rigidity&lt;/p&gt;
    &lt;h3&gt;Weak comparison forces the hyperbolic model&lt;/h3&gt;
    &lt;p&gt;Under the cylinder-trapping condition, or the stated side-angle alternative, the inequalities $R_g\geq-6$, $H_g\geq H_{\mathrm{hyp}}$, and $\gamma_g\leq\gamma_{\mathrm{hyp}}$ imply that the polyhedron is isometric to one in hyperbolic space.&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 scope&lt;/p&gt;
    &lt;h3&gt;Every hyperbolic tetrahedron in the class is covered&lt;/h3&gt;
    &lt;p&gt;All cone-type references satisfy cylinder trapping; for prisms it is equivalent to a concrete nesting condition between the two Euclidean base polygons.&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 variational functional produces a stable capillary surface of constant mean
curvature $\pm2$ with the contact angles of the reference foliation.  Its
second variation, together with Gauss&amp;ndash;Bonnet, converts scalar-, mean-, and
dihedral-curvature comparisons into a contradiction unless equality holds.
In the equality case, an infinitesimally rigid capillary surface is propagated
by a constant-mean-curvature foliation; a separate foliation construction at a
vertex completes the global rigidity argument.&lt;/p&gt;
</description>
    </item>
    
    <item>
      <title>Scalar curvature comparison of rotationally symmetric sets</title>
      <link>https://gaomw.com/publication/rotationallyrigidity/</link>
      <pubDate>Tue, 25 Apr 2023 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/rotationallyrigidity/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;This paper treats scalar-curvature rigidity for compact three-manifolds whose
reference boundary is rotationally symmetric and weakly convex, including
smooth, conical, and truncated models.&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;Euclidean rigidity&lt;/p&gt;
    &lt;h3&gt;Boundary comparison determines the interior&lt;/h3&gt;
    &lt;p&gt;If $R_g\geq0$, the induced boundary metric and mean curvature dominate those of the Euclidean reference, and the nonsmooth dihedral angles are no larger, then the manifold is flat under the stated pole hypotheses.&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;Endpoint geometries&lt;/p&gt;
    &lt;h3&gt;Disks, cones, and spherical poles are all included&lt;/h3&gt;
    &lt;p&gt;The theorem covers boundaries cut off by planar disks, boundaries with conical tips, and boundaries with smooth spherical poles.  Standard balls and right circular cones are important special cases.&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;Extensions&lt;/p&gt;
    &lt;h3&gt;Hyperbolic and circle-symmetric analogues&lt;/h3&gt;
    &lt;p&gt;The same capillary framework yields corresponding rigidity statements in hyperbolic space and in nonpositively curved spaces with an $\mathbb S^1$ symmetry.&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 argument minimizes a capillary functional whose prescribed contact angle
varies along the rotational boundary.  Stability and Gauss&amp;ndash;Bonnet force the
minimizing disk to be infinitesimally rigid, after which a foliation propagates
the equality.  The main difficulty is ensuring that a nontrivial minimizer
exists near a conical or spherical pole; local constant-mean-curvature barrier
foliations reduce those cases to the planar-end problem.&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>General Theory of Partial Differential Equations on Triple Junction Surfaces</title>
      <link>https://gaomw.com/publication/thesis/</link>
      <pubDate>Sat, 02 Jul 2022 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/thesis/</guid>
      <description>&lt;h2 id=&#34;main-contributions&#34;&gt;Main contributions&lt;/h2&gt;
&lt;p&gt;The thesis builds a general analytic framework for triple-junction
hypersurfaces: singular spaces obtained by identifying the boundaries of
several smooth sheets.&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;Function spaces&lt;/p&gt;
    &lt;h3&gt;Analysis that remembers the junction geometry&lt;/h3&gt;
    &lt;p&gt;Sobolev- and Hölder-type spaces are defined sheetwise with compatibility and balancing conditions along the common boundary, providing the correct domains for geometric variation problems.&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;Elliptic theory&lt;/p&gt;
    &lt;h3&gt;Classical PDE tools extend to the singular setting&lt;/h3&gt;
    &lt;p&gt;For second-order elliptic operators on triple-junction hypersurfaces, the thesis develops existence, regularity, Fredholm, and spectral results analogous to those on smooth Riemannian manifolds.&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;Applications&lt;/p&gt;
    &lt;h3&gt;Geometry becomes accessible through the PDE framework&lt;/h3&gt;
    &lt;p&gt;The theory is applied to Jacobi operators, Morse index questions for minimal triple junctions, and conformal and uniformization problems for singular surfaces.&lt;/p&gt;
  &lt;/article&gt;
&lt;/div&gt;
&lt;h2 id=&#34;analytic-viewpoint&#34;&gt;Analytic viewpoint&lt;/h2&gt;
&lt;p&gt;The central principle is to separate local elliptic analysis on each smooth
sheet from the finite-dimensional matching data along the junction.  Trace
conditions encode which functions arise from ambient variations, while the
conormal balance supplies the natural transmission condition for second-order
operators.  Once regularity across that interface is established, variational,
spectral, and geometric tools can be used much as in the smooth theory.&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>
    
    <item>
      <title>Uniformization of surfaces with boundary and the application to the triple junction surfaces with negative Euler characteristic</title>
      <link>https://gaomw.com/publication/uniformization/</link>
      <pubDate>Sat, 09 Oct 2021 11:51:14 +0800</pubDate>
      <guid>https://gaomw.com/publication/uniformization/</guid>
      <description>&lt;h2 id=&#34;main-results&#34;&gt;Main results&lt;/h2&gt;
&lt;p&gt;The paper first develops a quantitative uniformization theorem for surfaces
with boundary and then uses it to match the three sheets of a triple-junction
surface.&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;Surfaces with boundary&lt;/p&gt;
    &lt;h3&gt;Prescribed constant interior and boundary curvature&lt;/h3&gt;
    &lt;p&gt;For a compact oriented surface with negative Euler characteristic and $(k,c)$ satisfying $k\leq0$ and $c&lt;\sqrt{-k}$, there is a unique conformal metric with Gaussian curvature $k$ and constant boundary geodesic curvature $c$.&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;Quantitative control&lt;/p&gt;
    &lt;h3&gt;Area and boundary length vary monotonically&lt;/h3&gt;
    &lt;p&gt;The area $A(k,c)$ and boundary length $L(k,c)$ are continuous and satisfy sharp monotonicity and limiting laws, including the behavior of $cL(k,c)$ needed to balance junction curvature.&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;Triple junctions&lt;/p&gt;
    &lt;h3&gt;A weak hyperbolic uniformization&lt;/h3&gt;
    &lt;p&gt;If a triple-junction surface has connected junction and $\chi(M)\leq0$, its three sheets admit conformal hyperbolic metrics with a common boundary length whose geodesic curvatures sum to zero; the sheet metric is unique when its Euler characteristic is nonpositive.&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 prescribed-curvature problem is written as a semilinear elliptic boundary
value problem.  Maximum-principle estimates give existence, uniqueness,
continuity, and monotonicity as $k$ and $c$ vary.  For the junction problem,
the boundary length is used as a common parameter: the three curvature-length
functions are added, and their monotonicity and endpoint limits produce the
unique balancing length.&lt;/p&gt;
&lt;h2 id=&#34;positive-curvature-phenomenon&#34;&gt;Positive-curvature phenomenon&lt;/h2&gt;
&lt;p&gt;The following is a short video shows that why the uniqueness might fail when $K&amp;gt;0$.&lt;/p&gt;









  





&lt;video controls  &gt;
  &lt;source src=&#34;https://gaomw.com/media/fix_c.mp4&#34; type=&#34;video/mp4&#34;&gt;
&lt;/video&gt;
&lt;p&gt;In this video, we suppose the surface $\Sigma$ is the two copies of the domain enclosed by six arcs by identifying their corresponding edges marked with green color. So here $\Sigma$ is just a genus zero surface with three boundary components. We fix one boundary of $\Sigma$ having geodesic curvature $-1$ (marked as red) and the remaining two boundaries being geodesic (marked as black). Then we can let the area grow to see how the Gauss curvature changes after uniformization. The blue circle in this video represents the infinity circle if $K&amp;lt;0$ or the geodesic circle if $K&amp;gt;0$. From the video, we can see that $K$ will increase as area $A$ increases, then $K$ will reach its maximal point and after that $K$ will decrease to 0. So we will see that for some $K&amp;gt;0$, there are indeed two metrics with prescribed Gauss curvature and geodesic curvatures of boundaries.&lt;/p&gt;
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