Asymptotics of the graph Laplace operator near an isolated singularity
Susovan Pal
TL;DR
The paper investigates how the continuous graph Laplacian on a smooth manifold behaves near an isolated singularity as the bandwidth $t$ tends to zero. It identifies two regimes: (i) if the metric extends across the singularity under a controlled curvature blow-up, the Laplacian converges to the weighted Laplace–Beltrami operator with density $p$; (ii) if a locally angular conformal modification makes the metric non-extendable, curvature blows up like $\kappa(s)\sim c/s^2$, causing intrinsic and extrinsic Laplacians to blow up at rate $O(t^{-1/2})$ under mild non-degeneracy. The work provides explicit asymptotic expansions (including $t^{-1/2}$ and Taylor-type terms) and supports them with numerical simulations on punctured disks and cone-apex geometries. These results deepen understanding of graph-based approximations to Riemannian operators in the presence of singularities and have implications for data-driven manifold learning near singular structures.
Abstract
In this paper, we investigate asymptotics of the continuous graph Laplace operator on a smooth Riemannian manifold $(M,g)$ admitting an isolated singularity $x$. We show that if the curvature function $κ$ doesn't grow too fast near $x$, then the graph Laplace operator at $x$ converges to the weighted Laplace-Beltrami operator as the bandwidth $t\downarrow 0.$ On the other hand, we also prove that if one locally modifies a given Riemannian metric across $x$ by a non-constant \textit{purely angular }conformal factor, then $κ$ grows too fast and the graph Laplace operator behaves like $O(\frac{1}{\sqrt{t}})$ near $x$, as $t\downarrow 0$, given a mild condition on the angular conformal factor. We provide the Taylor expansion of the graph Laplace operator as $t\downarrow 0$ in specific cases. Numerical simulations at the end illustrate our results.
