- The paper proves that positive reach of the domain and a Lipschitz, positive conformal factor guarantee uniformly regular conformal geodesics with reach at least min(τ_M/2, f_min/(8κ)).
- The paper develops weighted ball-graph and nearest-neighbor estimators whose relative error reaches O((log n/n)^{1/d}) with sufficiently accurate edge quadrature, while sample-only evaluations yield O((log n/n)^{2/(3d)}).
- The paper extends guarantees beyond smooth manifolds to arbitrary positive-reach sets and establishes a minimax lower bound of n^{-1/(d−1/2)}, leaving the exact optimal rate under minimal assumptions open.
Overview
The paper studies conformal metrics over subsets of Euclidean space: given a closed path-connected domain M⊂RN and a positive conformal factor f:M→R+∗, the conformal distance between two points is the infimum over Lipschitz paths of the weighted length ∫f(γ)∥γ˙∥dt. The author's goal is twofold: first, to establish regularity properties of geodesics for such metrics under a positive reach assumption on M (with no requirement that M be a submanifold), and second, to derive convergence rates for estimating DM,f from an i.i.d. point cloud. The motivating application is the Fermat distance, where f=ρ−β for a density ρ, used in topological data analysis and metric learning.
Throughout, the sole structural assumptions are that M has positive reach τM>0 (in the sense of Federer) and that f:M→R+∗0 is f:M→R+∗1-Lipschitz and lower bounded by f:M→R+∗2. By McShane extension, f:M→R+∗3 may be taken to be defined on all of f:M→R+∗4 without loss of generality, which is exploited in constructing practical estimators.
The first main contribution is a lower bound on the reach of geodesics for the conformal metric. Building on the characterization of reach via metric distortion (2602.16466), the paper defines the conformal reach f:M→R+∗5 as the infimum of the reaches of all conformal geodesics, and proves it satisfies an analogous arcsine-type characterization. The central result of this section states:
f:M→R+∗6
Consequently, every conformal geodesic is a f:M→R+∗7 curve whose angular velocity is controlled by its reach. This yields a technical but crucial lemma bounding the deviation of short secant directions from the tangent direction, and the difference of normalized steps on either side of a point, both proportional to step size over reach. These estimates are what later allow the Hausdorff-error term in the approximation bound to be quadratic rather than linear.
Polygonal Approximation on Weighted Graphs
Given a finite point cloud f:M→R+∗8, distances are estimated by shortest paths on a graph over f:M→R+∗9: either an ∫f(γ)∥γ˙∥dt0-ball graph or a ∫f(γ)∥γ˙∥dt1-nearest-neighbors graph, with edges weighted by a quadrature formula ∫f(γ)∥γ˙∥dt2 that approximates the integral of ∫f(γ)∥γ˙∥dt3 along straight segments using ∫f(γ)∥γ˙∥dt4 evaluations of ∫f(γ)∥γ˙∥dt5 (resolution ∫f(γ)∥γ˙∥dt6 corresponds to the trapezoidal weight ∫f(γ)∥γ˙∥dt7; ∫f(γ)∥γ˙∥dt8 to the exact integral).
For endpoints within distance ∫f(γ)∥γ˙∥dt9, the relative distortion of the weights is bounded by
M0
where the first term vanishes as resolution grows and the second reflects the curvature of geodesics. The main deterministic approximation theorem then gives, assuming M1,
M2
Balancing terms via M3 and M4 makes the total error proportional to the Hausdorff distance. Two points deserve emphasis:
- For the induced metric (M5), the paper recovers the quadratic error M6 previously obtained under stronger manifold assumptions, showing that positive reach alone—no M7 structure, not even a manifold—is sufficient.
- If M8 can only be evaluated on the sample (M9), the error degrades to order M0, matching the rate achievable under the weaker "geodesic smoothness" assumption of prior work.
When the true factor M1 is replaced by any estimate M2 with M3, the total error decomposes additively: it is bounded by twice the domain error plus M4. Hence the slowest of the two estimation errors dictates the overall rate.
Estimation from Random Samples
With M5 drawn i.i.d. from a M6-standard measure M7 (a one-sided Ahlfors condition ensuring balls carry mass at least M8), the Hausdorff distance M9 is shown in expectation to be DM,f0, where DM,f1. Substituting into the approximation theorem yields the following rates for the ball-graph estimator:
| Setting |
Parameters |
Expected relative error |
| High resolution (DM,f2) |
DM,f3 |
DM,f4 |
| Resolution DM,f5 |
DM,f6 |
DM,f7 |
In particular, for the induced metric, the estimator converges at rate DM,f8 (up to logs) for any set of positive reach. Under the stronger assumption that DM,f9 is a f=ρ−β0 submanifold, the minimax optimal rate for the induced metric is known to be f=ρ−β1; the present result extends the upper bound to the non-smooth regime at the cost of a slower rate.
Ball graphs versus nearest-neighbor graphs
Optimal tuning of f=ρ−β2 requires knowledge of the intrinsic dimension f=ρ−β3. To remove this dependency, the paper establishes a high-probability equivalence between graph families under full f=ρ−β4-Ahlfors regularity of f=ρ−β5: with probability at least f=ρ−β6, the edge sets satisfy
f=ρ−β7
for f=ρ−β8 scaling like f=ρ−β9 up to ρ0 factors. Choosing ρ1 and ρ2 then transfers the ball-graph guarantee to the NN graph at the same rate ρ3, with the loss measured over ρ4 rather than ρ5—the author notes the version over all of ρ6 holds but is omitted for brevity. Notably, no knowledge of ρ7, the Ahlfors constants, ρ8, ρ9, or M0 is needed to run this estimator.
Complexity: building the M1-NN graph costs M2; evaluating weights costs M3; Dijkstra adds M4. With the recommended parameters the overall time is M5 per pair of query endpoints.
Minimax Lower Bound
Using Le Cam's method with a two-point construction—a cube versus the same cube with an edge carved by a ball of radius exactly M6—the paper proves that over the class of M7-standard measures supported on sets of reach at least M8, the minimax risk for the induced metric satisfies
M9
The construction exploits the fact that carving a region of volume τM>00 (length τM>01 along the affected direction, τM>02 transversally, forced by the standardness constraint) distorts a single interpoint distance by a factor of order τM>03. The resulting lower bound τM>04 does not match the upper bound τM>05, although the gap becomes negligible for large τM>06. The author argues that closing the gap likely requires a different technique, since the reach assumption caps the distortion achievable by perturbing domains near fixed endpoints at order τM>07, which appears to force the τM>08 volume argument. The exact minimax rate under only a positive-reach assumption therefore remains open.
Relation to Smooth-Manifold Estimators
Under a τM>09 assumption (f:M→R+∗00), minimax optimality f:M→R+∗01 is achieved by reconstructing the manifold (e.g., via tangential Delaunay complexes) at Hausdorff accuracy f:M→R+∗02 and reading off the induced metric—but these procedures are not computationally feasible since they involve non-discrete reconstructions. A concrete pipeline would reconstruct the manifold, sample a fine net over it, and apply the polygonal estimator; the results here certify that this achieves the optimal f:M→R+∗03 rate, though at the cost of inflating the effective sample size from f:M→R+∗04 to roughly f:M→R+∗05.
Two instances connect the theory to existing practice:
- Density-based factors: for f:M→R+∗06 (Fermat distance), prior estimators based on edge weights f:M→R+∗07 lack convergence guarantees. Coupling the polygonal estimator with a kernel density estimator converging at rate f:M→R+∗08 in f:M→R+∗09 (available when f:M→R+∗10 is a f:M→R+∗11 submanifold with f:M→R+∗12 density) yields, via the additive error decomposition, an estimator of the Fermat distance converging at the full rate f:M→R+∗13—at higher computational cost than discrete Fermat distances.
- Distance-to-measure: f:M→R+∗14 is f:M→R+∗15-Lipschitz and positively bounded away from zero whenever f:M→R+∗16 has no atoms, fitting the framework; it admits an estimator converging at rate f:M→R+∗17, faster than f:M→R+∗18 and thus not the bottleneck.
Limitations and Open Questions
Several caveats qualify the results. The optimal parameter choices in the ball-graph theorem depend explicitly on f:M→R+∗19, f:M→R+∗20, and f:M→R+∗21; while the NN-graph route removes the need to know them in practice, the theoretical constants still require Ahlfors regularity, and the NN-graph guarantee is stated over f:M→R+∗22 rather than f:M→R+∗23. The high-resolution regime assumes f:M→R+∗24 can be evaluated off-sample; when only sample evaluations are possible (f:M→R+∗25), the rate degrades to f:M→R+∗26. Most substantively, the minimax rate under the positive-reach-only model remains unresolved: the upper bound f:M→R+∗27 and the lower bound f:M→R+∗28 do not coincide, and the author offers reasons to suspect that Le Cam-type constructions may be inherently limited in this model. Finally, the density-based application inherits the additional smoothness assumptions (f:M→R+∗29 submanifold and f:M→R+∗30 density) required by the underlying kernel density estimator.
Conclusion
This work establishes that a positive reach assumption on the domain, together with Lipschitz and lower-bound conditions on the conformal factor, suffices for conformal geodesics to have uniformly positive reach, and consequently for the conformal metric to be estimated from i.i.d. samples at rate f:M→R+∗31 (up to logarithms) by an f:M→R+∗32-time nearest-neighbor graph algorithm requiring no knowledge of intrinsic parameters. The same machinery applies verbatim to the induced metric of arbitrary positive-reach sets, extending prior manifold-based bounds, and provides quantitative convergence guarantees for Fermat-type metrics where none were previously available.