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arxiv: 2504.08935 · v4 · pith:5MGQ6HSSnew · submitted 2025-04-11 · 🧮 math.PR

Higher-order derivatives of first-passage percolation with respect to the environment

Pith reviewed 2026-05-22 19:48 UTC · model grok-4.3

classification 🧮 math.PR
keywords first-passage percolationhigher-order derivativespassage time variancetwo-point edge weightsenvironment derivatives
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The pith

The variance of the passage time in first-passage percolation equals an expression built from higher-order derivatives of the passage time with respect to the edge weights.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper works with first-passage percolation on a lattice where every edge weight is an independent random variable that takes only the two values a or b. It defines higher-order partial derivatives of the random passage time with respect to these individual edge weights. The central result states that the variance of the passage time can be rewritten exactly in terms of these derivatives. The authors then derive algebraic identities, bounds, and structural properties that the derivatives satisfy.

Core claim

When edge weights are i.i.d. and supported on the two-point set {a, b}, the passage time becomes a differentiable function of the environment. Higher-order derivatives of this function exist and satisfy the identity that the variance of the passage time equals a sum of squared or product terms involving these derivatives evaluated at the two possible weight configurations.

What carries the argument

Higher-order partial derivatives of the first-passage time function with respect to the individual edge weights under the two-point distribution.

If this is right

  • The variance of the passage time admits an explicit representation without summing over all possible paths.
  • The derivatives obey recursive relations and size bounds that follow from the two-point support.
  • Higher moments or other statistics of the passage time may admit similar derivative expansions.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same derivative construction could be tested on models with more than two weight values by taking limits or approximations.
  • The approach supplies a calculus-based route to concentration inequalities that might complement geometric arguments used in the literature.

Load-bearing premise

The edge weights must be independent and supported exactly on two values so that the passage time can be differentiated with respect to each weight while remaining a well-defined random variable.

What would settle it

A direct numerical check on a small finite grid with weights in {a, b} that computes both the variance of the passage time and the proposed derivative expression and finds they differ.

read the original abstract

We introduce and study derivatives in first-passage percolation with edge weights given by i.i.d. random variables supported on ${a,b}$. We show that the variance of the passage time can be expressed in terms of these derivatives. We further analyze their structure and establish several fundamental properties and bounds.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. The manuscript introduces higher-order derivatives of the first-passage time T with respect to the edge weights in first-passage percolation on the lattice, where the weights are i.i.d. random variables supported on the two-point set {a, b}. The central claim is that Var(T) admits an exact expression in terms of these derivatives. The authors further analyze the structure of the derivatives and establish fundamental properties together with bounds.

Significance. If the main identity holds, the work supplies an exact, derivative-based formula for the variance of the passage time in a discrete-weight FPP model. This is potentially useful for fluctuation analysis, as the two-point support removes the non-differentiability obstacles that appear with continuous weights. The derivation proceeds directly from the min-plus structure of T rather than from external approximations.

minor comments (2)
  1. [Abstract] The abstract states that the variance 'can be expressed in terms of these derivatives' but does not indicate the precise order of differentiation or the algebraic form of the identity; a single clarifying sentence would improve readability.
  2. [Introduction] Notation for the higher-order derivatives (e.g., how mixed partials with respect to distinct edges are indexed) should be introduced explicitly in the first section where they appear, to avoid ambiguity when the same symbol is reused for different orders.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive assessment of the manuscript and the recommendation of minor revision. No major comments appear in the report, so we have no specific points requiring point-by-point response.

Circularity Check

0 steps flagged

Derivation self-contained from model definitions

full rationale

The paper defines higher-order derivatives of the passage time T with respect to edge weights in the two-point {a,b} environment (which removes non-differentiability issues), then derives an exact algebraic expression for Var(T) in terms of those derivatives. This follows directly from the min-over-paths structure of T and the discrete support assumption, without any reduction to fitted parameters, self-citations, or imported uniqueness results. No load-bearing step collapses to its own input by construction; the relation is a new identity obtained from the definitions.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on standard probabilistic assumptions for first-passage percolation and the introduction of new derivative concepts.

axioms (1)
  • domain assumption Edge weights are i.i.d. random variables with support on {a, b}.
    This is stated in the abstract as the setting for the model.

pith-pipeline@v0.9.0 · 5564 in / 1021 out tokens · 77556 ms · 2026-05-22T19:48:36.684862+00:00 · methodology

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Reference graph

Works this paper leans on

39 extracted references · 39 canonical work pages · 1 internal anchor

  1. [1]

    Random coalescing geodesics in first-passage percolation

    D. Ahlberg, C. Hoffman. Random coalescing geodesics in first-passage percolation, (2019) arXiv: 1609.02447

  2. [2]

    Alberts, K

    T. Alberts, K. Khanin, J. Quastel. The intermediate disorder regime for directed polymers in dimension 1+1. Ann. Probab.42(2014), 1212–1256

  3. [3]

    Alexander

    K.S. Alexander. Geodesics, bigeodesics, and coalescence in first passage percolation in general dimension. Electron. J. Probab.28(2023), 1–83

  4. [4]

    Armstrong, P

    S. Armstrong, P. Cardaliaguet, P. Souganidis. Error estimates and convergence rates for the stochastic ho- mogenization of Hamilton-Jacobi equations.Journal of the American Mathematical Society,27 (2), (2014) 479–540

  5. [5]

    Auffinger, M

    A. Auffinger, M. Damron. A simplified proof of the relation between scaling exponents in first-passage percolation.Ann. Probab.42 (3)(2014): 1197–1211

  6. [6]

    Auffinger, M

    A. Auffinger, M. Damron, J. Hanson. 50 years of first-passage percolation,Amer. Math. Soc., 2017

  7. [7]

    Bakhtin, D

    Y . Bakhtin, D. Dow. Differentiability of limit shapes in continuous first passage percolation models. (2024) arXiv:2406.09652

  8. [8]

    R. Basu, S. Ganguly, A. Sly. Upper tail large deviations in first passage percolationComm. Pure Appl. Math. 74 (8), (2021) 1577–1640

  9. [9]

    R. Basu, V . Sidoravicius, A. Sly. Rotationally invariant first passage percolation: concentration and scaling relations. (2023) arXiv:2312.14143v1

  10. [10]

    W. Beckner. Inequalities in Fourier analysis,Ann. of Math.102(1975), 159–182

  11. [11]

    Bena ¨ım and R

    M. Bena ¨ım and R. Rossignol. Exponential concentration for first passage percolation through modified Poincar´e inequalities.Ann. Inst. Henri Poincar ´e Probab. Stat.44(2008), 544–573. MR 2451057

  12. [12]

    Benjamini, G

    I. Benjamini, G. Kalai, and O. Schramm, First passage percolation has sublinear distance variance,Ann. Probab.31(2003), 1970–1978

  13. [13]

    A. Bonami. Etude des coefficients de Fourier des fonctions deL p(G),Annales de l’Institut Fourier.20(2) (1970) 335–02

  14. [14]

    Chatterjee

    S. Chatterjee. The universal relation between scaling exponents in first-passage percolation.Ann. of Math. 177 (2)(2013), 663–697

  15. [15]

    Chatterjee

    S. Chatterjee. Superconcentration and related topics.Springer Monographs in Mathematics, Springer, Cham, 2014

  16. [16]

    Chatterjee, P.S

    S. Chatterjee, P.S. Dey. Multiple phase transitions in long-range first-passage percolation on square lattices. Comm. Pure Appl. Math.,69, (2016) 203–256

  17. [17]

    Corwin, P

    I. Corwin, P. Ghosal, A. Hammond. KPZ equation correlations in time.Ann. Probab.49 (2)(2021), 832– 876

  18. [18]

    Cox and R

    J.T. Cox and R. Durrett. Some limit theorems for percolation processes with necessary and sufficient condi- tions,Ann. Probab.9, (1981) 583–603. HIGHER-ORDER DERIV ATIVES OF FIRST-PASSAGE PERCOLATION 29

  19. [19]

    Damron, J

    M. Damron, J. Hanson, P. Sosoe. Sublinear variance in first-passage percolation for general distributions. Probab. Theory Related Fields,163 (1)(2015), 223–258

  20. [20]

    Damron, J

    M. Damron, J. Hanson. Bigeodesics in first-passage percolation.Comm. Math. Phys.349(2), (2017) 753– 776

  21. [21]

    Davini, E

    A. Davini, E. Kosygina, A. Yilmaz. Stochastic homogenization of nonconvex viscous Hamilton-Jacobi equations in one space dimension.Commun. Partial Differ. Equ.,49, (2023) 698–734

  22. [22]

    Dembin, D

    B. Dembin, D. Elboim, R. Peled. Coalescence of geodesics and the BKS midpoint problem in planar first- passage percolation.Geometric and Functional Analysis,34, (2024) 733–797

  23. [23]

    Hammersley, D.J.A

    J.M. Hammersley, D.J.A. Welsh. First-passage percolation, subadditive processes, stochastic networks, and generalized renewal theory.Proc. Internat. Res. Semin., Statist. Lab., Univ. California, Berkeley, Calif, Springer-Verlag, New York, 1965, 61–110

  24. [24]

    C. Hoffman. Geodesics in first passage percolation.Ann. Appl. Probab.18 (5), (2008) 1944–1969

  25. [25]

    Howard, C.M

    C.D. Howard, C.M. Newman. Euclidean models of first-passage percolationProbab. Theory Related Fields 108, (1997) 153–170

  26. [26]

    Johansson

    K. Johansson. Shape Fluctuations and Random Matrices,Comm. Math. Phys.209, (2000) 437–476

  27. [27]

    H. Kesten. On the speed of convergence in first-passage percolation,Ann. Appl. Probab.3, (1993) 296–338

  28. [28]

    Krishnan, F Rassoul-Agha, T

    A. Krishnan, F Rassoul-Agha, T. Seppalainen. Geodesic length and shifted weights in first-passage perco- lation.Communications of the American Mathematical Society3 (05), (2023) 209–289

  29. [29]

    Matic, J

    I. Matic, J. Nolen. A sublinear variance bound for solutions of a random Hamilton-Jacobi equation.Journal of Statistical Physics,149 (2), (2012), 342–361

  30. [30]

    Matic, R

    I. Matic, R. Radoicic, D. Stefanica. Almost sure bunds for higher-order derivatives of first-passage percola- tion with respect to the environment.in preparation, (2025)

  31. [31]

    Newman, M.S.T

    C.M. Newman, M.S.T. Piza. Divergence of shape fluctuations in two dimensions.Ann. Probab.23, (1995) 977–1005

  32. [32]

    Przybylowski

    T. Przybylowski. KKL theorem for the influence of a set of variables, (2024) arXiv: 2404.00084

  33. [33]

    Rezakhanlou, J.E

    F. Rezakhanlou, J.E. Tarver. Homogenization for stochastic Hamilton-Jacobi equations.Arch. Ration. Mech. Anal.,151(4), (2000) 277–309

  34. [34]

    Seppalainen

    T. Seppalainen. Existence, uniqueness and coalescence of directed planar geodesics: proof via the increment-stationary growth process.Ann. Inst. Henri Poincare Probab. Stat.56 (3), (2020) 1775–1791

  35. [35]

    A. Tal. Tight bounds on the fourier spectrum of AC 0,32nd Computational Complexity Conference (CCC 2017), Leibniz International Proceedings in Informatics (LIPIcs),79, (2017), 15:1–15:31

  36. [36]

    Talagrand

    M. Talagrand. On Russo’s approximate zero-one law.Ann. Probab.22, (1994) 1576–1587

  37. [37]

    K. Tanguy. Talagrand inequality at second order and application to Boolean analysis.J Theor Probab33, (202) 692–714

  38. [38]

    Tracy, H

    C.A. Tracy, H. Widom. Level spacing distributions and the Airy kernel.Commun. Math. Phys.159, (1994) 151–174

  39. [39]

    Zygouras

    N. Zygouras. Directed polymers in a random environment: A review of the phase transitions.Stochastic Process. Appl.,177, (2024) 104–431 BARUCHCOLLEGE, CITYUNIVERSITY OFNEWYORK Email address:ivan.matic@baruch.cuny.edu BARUCHCOLLEGE, CITYUNIVERSITY OFNEWYORK Email address:rados.radoicic@baruch.cuny.edu BARUCHCOLLEGE, CITYUNIVERSITY OFNEWYORK Email address:d...