A warped product with a spherical factor and a logarithmically concave warping function satisfies a scalar curvature rigidity of the Llarull type. We develop a scalar curvature rigidity of the Llarull type for a general class of domains in a three dimensional spherical warped product. In the presence of rotational symmetry, we identify this class of domains as those satisfying a boundary condition analogous to the logarithmic concavity of the warping function.
Main results
The paper establishes Llarull-type scalar-curvature rigidity for domains in
three-dimensional spherical warped products, including models with boundary
and singular endpoint geometry.
Domain rigidity
Metric, scalar, and boundary comparison determine the model
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.
Endpoint geometry
Smooth, conical, and disk-type ends are treated uniformly
The rigidity theorem covers smooth poles, Euclidean or metric tangent cones, and truncations by end disks with matching mean-curvature and angle inequalities.
Conical Llarull theorem
Antipodal cone points are allowed
For warped three-spheres with $\psi(t_\pm)=a_\pm|t-t_\pm|+o(|t-t_\pm|)$ and $0
Proof strategy
Prescribed-mean-curvature capillary $\mu$-bubbles play the role of the
minimizing hypersurfaces in Llarull’s theorem. The stability inequality and a
Gauss–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.