Let $M^3\to X^4$ be a complete, connected, two-sided stable minimal immersion. We prove that if the ambient sectional curvature is nonnegative and the ambient scalar curvature has a positive uniform lower bound, then $M$ is totally geodesic and its normal Ricci curvature vanishes. No weak bounded geometry assumption and no upper curvature bound are imposed. We also construct a complete metric of strictly positive sectional curvature on $\mathbb{R}^4$ admitting a complete, embedded, one-ended, nonparabolic, two-sided stable minimal hypersurface diffeomorphic to $\mathbb{R}^3$ which is not totally geodesic. The rigidity proof combines spectral splitting theory, a warped $\mu$-bubble construction, and a harmonic function level set argument. The example is obtained by a compactly supported deformation of an example of Chodosh–Li–Stryker.
Main results
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.
Rigidity
Positive scalar curvature forces total geodesicity
If the ambient sectional curvature is nonnegative and the ambient scalar curvature satisfies $\overline R\geq\kappa>0$, then every complete, connected, two-sided stable minimal immersion $M^3\to X^4$ has $A\equiv0$ and $\overline{\operatorname{Ric}}(\nu,\nu)\equiv0$.
Sharpness
The uniform scalar curvature gap is necessary
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.
Improvement
No bounded-geometry or upper-curvature hypothesis
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.
Proof architecture
The argument replaces extrinsic volume comparison by an intrinsic spectral and
potential-theoretic route.
Step 1
Spectral and topological reduction
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 $\mathbb R^3$.
Step 2
Separating warped $\mu$-bubbles
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.
Step 3
Harmonic functions and flux
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.
The counterexample mechanism
Starting from the Chodosh–Li–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
$$
|A|^2+\overline{\operatorname{Ric}}(\nu,\nu).
$$
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.