Limit shape of first-passage percolation
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Definitions and mathematical statement
Fix $d\ge2$ and give $\mathbb Z^d$ its nearest-neighbor edges. Assign independent exponential passage times $\tau_e$ of mean one to all edges. For vertices $x,y$, define \[ T(x,y)=\inf_{\gamma:x\to y}\sum_{e\in\gamma}\tau_e, \] where the infimum ranges over finite nearest-neighbor paths. Let $B(t)=\{x:T(0,x)\le t\}$, and replace each of its vertices by the unit cube centered there to obtain a subset $\widetilde B(t)\subset\mathbb R^d$.The shape theorem supplies a deterministic compact convex body $K_d$ with nonempty interior such that $t^{-1}\widetilde B(t)$ converges to $K_d$ almost surely in Hausdorff distance. Equivalently, $K_d=\{x:\mu_d(x)\le1\}$, where the directional time constant is $\mu_d(x)=\lim_{n\to\infty}T(0,nx)/n$ for lattice directions and is extended to a norm on $\mathbb R^d$.
Determine this body explicitly, or equivalently determine the directional dependence of $\mu_d$. If only the shape up to scale is sought, normalize $K_d$ to Euclidean diameter one. Merely expressing the answer through the same unknown passage-time limit does not identify the shape.
The equivalent discrete growth process begins with only $0$ black, chooses uniformly among edges with exactly one black endpoint, and turns that edge's white endpoint black. Exponential memorylessness makes this the embedded jump chain of the passage-time model. Uniform choice is among boundary edges, so a white vertex with several black neighbors is proportionally more likely to be chosen. This distinction fixes the precise random growth model in the original question.
Short English statement
What is the deterministic macroscopic shape of exponential first-passage growth on a Euclidean lattice?Sources
- S1 ULAM.AI and the UnsolvedMath Contributors, supplied problems.json, record 10100007 (AMR-100-0007), AMR Open Problem Lists. Catalogue identity and source transcription; CC BY 4.0. https://huggingface.co/datasets/ulamai/UnsolvedMath.
- S2 MathOverflow — Famous open problems in probability theory, answer 37167, source-order answer 7 of 13. Original source indexed by AMR-100-0007. https://mathoverflow.net/a/37167.
- S3 B. Kloeckner, MathOverflow answer 37167 (2010), the original boundary-edge growth question. https://mathoverflow.net/a/37167.
- S4 A. Auffinger, M. Damron and J. Hanson, 50 years of first passage percolation, shape theorem and limit-shape questions. https://arxiv.org/abs/1511.03262.
Statement licence: CC-BY-4.0 · Source file
Contributions 1
OpenAI claim summary for Math-1736
The cited theorem gives strict convexity and C1 differentiability of the planar exponential shape, but our question asks its explicit directional norm in every d>=2; neither a formula nor the other dimensions is determined. This entry records partial support; complete coverage of the question is not established by this catalogue.
Limit shape of first-passage percolation
OpenAI's claim
OpenAI presents a mathematical result relevant to this question in the selected manuscript. The exponential planar first-passage shape is claimed to be strictly convex with a continuously differentiable boundary; Gamma laws are also claimed to give differentiable time constants.Mathematical statement of the claimed result
Result 1.
For nearest-neighbor first-passage percolation on $\mathbb Z^2$ with independent exponential weights of fixed rate $\lambda>0$, let $\mu$ denote the time-constant norm and $\mathcal B=\{x:\mu(x)\le1\}$. The source claims differentiability of $\mu$ on $\mathbb R^2\setminus\{0\}$, a $C^1$ boundary of $\mathcal B$, and \[ x,y\in\partial\mathcal B,\ x\ne y,\ 0<t<1 \quad\Longrightarrow\quad\mu((1-t)x+ty)<1. \] Thus its unit ball is strictly convex and has one supporting line at each boundary point. This theorem is for exponential weights, not arbitrary passage laws.Outline of the argument
The argument separates the removal of corners from the removal of flat faces. Busemann and geodesic comparisons establish differentiability for Gamma weights, while an additional exponential-law argument excludes linear boundary segments; the two conclusions are then combined.Formal verification
For family 212, the documented entries give differentiability and continuously differentiable boundaries for planar Gamma shapes, including the exponential law. They do not supply strict convexity or the separate no-bigeodesic theorem. The listed Comparator files areGammaPassage.lean, PlanarFirstPassage.lean. Named declarations include OAI.PlanarFPP.manuscriptMain. This site has not executed the Lean code. The scope descriptions do not certify the remaining manuscript arguments.Status caveat
OpenAI attributes these manuscripts to work by an internal model. Its release cautions that arguments without formalization can contain mistakes. This catalogue has not independently checked the proofs; the labels report the mathematical claims attributed to OpenAI.Sources
- OpenAI, Strict convexity and differentiability of the planar exponential first-passage limit shape, 2026-09-24; citation key
OAI:Strict-convexity-and-differentiability-of-the-planar-exponential-first-passage-limit-shape-September-24-2026. PDF (GitHub); PDF (direct); Manuscript page and citation; Latest version; Statement source: thm:exponential-shape. - Family 212: Lean scope.
- Comparator GammaPassage.json.
- Comparator GammaPassage.lean.
- Comparator PlanarFirstPassage.json.
- Comparator PlanarFirstPassage.lean.
- OpenAI catalogue entry.