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arxiv: 2601.20640 · v2 · submitted 2026-01-28 · 🧮 math.AP · math.DG

Existence results for Leibenson's equation on Riemannian manifolds

Pith reviewed 2026-05-16 10:29 UTC · model grok-4.3

classification 🧮 math.AP math.DG
keywords Leibenson equationdoubly nonlinear equationsp-LaplacianRiemannian manifoldsexistence and uniquenessCauchy problemweak solutionsnonlinear diffusion
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The pith

The Cauchy problem for Leibenson's equation admits a unique weak solution on any Riemannian manifold under the condition pq ≥ 1.

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

This paper proves existence and uniqueness results for solutions to the Leibenson equation, a doubly nonlinear evolution equation of the form partial t u equals the p-Laplacian of u to the q, defined on a general Riemannian manifold. The result holds for p greater than 1, q positive with their product at least 1, and for initial data that are both integrable and bounded. This matters to readers interested in nonlinear partial differential equations because it extends well-posedness from flat space to curved geometries without additional assumptions on the manifold. A reader would care since such equations arise in modeling diffusion processes or geometric flows where the underlying space has curvature.

Core claim

The author establishes that if p > 1, q > 0 and pq ≥ 1, then for any initial datum u0 in the intersection of L1 and L infinity on the manifold M, there exists a unique weak solution to the Cauchy problem consisting of the time derivative of u equaling the p-Laplacian applied to u raised to q, for positive times, with the initial condition at time zero.

What carries the argument

The notion of weak solution to the doubly nonlinear equation, which uses the integration properties of the p-Laplacian on the Riemannian manifold.

If this is right

  • The solutions are defined globally in time for all positive times.
  • The result applies to any Riemannian manifold, including non-compact ones.
  • Uniqueness is guaranteed in the weak sense for the given range of parameters.
  • Initial data can be any function that is both integrable and essentially bounded.

Where Pith is reading between the lines

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

  • This opens the door to analyzing asymptotic behavior of solutions as time goes to infinity on manifolds with various curvatures.
  • Similar techniques might apply to other nonlinear parabolic equations on manifolds, such as those with different nonlinearities.
  • Potential applications include studying heat flows or diffusion models in general relativity or geometric analysis contexts.

Load-bearing premise

The chosen definition of a weak solution is suitable and permits the necessary integration-by-parts formulas for the p-Laplacian in the specified range of p and q.

What would settle it

Constructing an initial function in L1(M) cap L inf(M) for which either no weak solution exists or multiple distinct weak solutions can be found when pq is at least 1.

Figures

Figures reproduced from arXiv: 2601.20640 by Philipp S\"urig.

Figure 1
Figure 1. Figure 1: Cylinders Q and Q′ Remark 4.6. In [13] the same mean value inequality was proved under the condition that p > 2 and 1 p − 1 < q ≤ 1 or 1 < p < 2 and 1 ≤ q < 1 p − 1 . (4.76) Proof. Let us first prove (4.75) for σ large enough as in Lemma 4.1. Consider sequences rk =  1 2 + 2−k−1  R, where k = 0, 1, 2, ..., so that r0 = R and rk ↘ 1 2R as k → ∞ . Set Bk = B (x0, rk), Qk = Bk × [0, t] so that B0 = B, Q0 = … view at source ↗
Figure 2
Figure 2. Figure 2: Cylinders Qk Choose some θ > 0 to be specified later and define θk = [PITH_FULL_IMAGE:figures/full_fig_p024_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Range of p, q 27 [PITH_FULL_IMAGE:figures/full_fig_p027_3.png] view at source ↗
read the original abstract

We consider on an arbitrary Riemannian manifold $M$ the \textit{Leibenson equation} $\partial _{t}u=\Delta _{p}u^{q}$, that is also known as a \textit{doubly nonlinear evolution equation}. We prove that if $p>1, q>0$ and $pq\geq 1$ then the Cauchy-problem \begin{equation*} \left\{\begin{array}{ll}\partial _{t}u=\Delta _{p}u^{q} &\text{in}~M\times (0, \infty), \\u(x, 0)=u_{0}(x)& \text{in}~M,\end{array}\right.\end{equation*} has a unique weak solution for any $u_{0}\in L^{1}(M)\cap L^{\infty}(M)$.

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

1 major / 2 minor

Summary. The manuscript proves existence and uniqueness of a weak solution to the Cauchy problem for the Leibenson (doubly nonlinear) equation ∂_t u = Δ_p u^q on an arbitrary Riemannian manifold M, for parameters p>1, q>0 with pq≥1 and initial data u_0 ∈ L^1(M) ∩ L^∞(M). The weak solution is defined by integration against compactly supported test functions.

Significance. If the result holds, it extends existence theory for nonlinear parabolic equations from Euclidean space to general Riemannian manifolds. This could serve as a foundation for studying doubly nonlinear flows in geometric settings, provided the technical framework is complete.

major comments (1)
  1. [Main theorem and §2 (weak formulation)] Main theorem (as stated in the abstract): the result is asserted for arbitrary Riemannian manifolds M without an explicit completeness assumption. The weak formulation ∫ u ∂_t φ + ∫ |∇(u^q)|^{p-2} ∇(u^q) · ∇φ = 0 for φ ∈ C_c^∞(M×(0,∞)) relies on global integration-by-parts identities and density of compactly supported functions in the appropriate Sobolev space; both can fail on incomplete manifolds, breaking the passage to the limit in any approximation scheme used for existence.
minor comments (2)
  1. [Abstract and §1] The abstract and introduction should explicitly state the precise definition of the weak solution and the range of test functions.
  2. [Introduction] Add a brief comparison to the corresponding result on R^n to clarify the contribution of the manifold setting.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We address the major concern point by point below.

read point-by-point responses
  1. Referee: [Main theorem and §2 (weak formulation)] Main theorem (as stated in the abstract): the result is asserted for arbitrary Riemannian manifolds M without an explicit completeness assumption. The weak formulation ∫ u ∂_t φ + ∫ |∇(u^q)|^{p-2} ∇(u^q) · ∇φ = 0 for φ ∈ C_c^∞(M×(0,∞)) relies on global integration-by-parts identities and density of compactly supported functions in the appropriate Sobolev space; both can fail on incomplete manifolds, breaking the passage to the limit in any approximation scheme used for existence.

    Authors: We agree that an explicit completeness assumption on M is necessary to justify the global integration-by-parts formula and the density of compactly supported smooth functions in the relevant Sobolev spaces used throughout the existence proof. These properties hold on complete Riemannian manifolds but may fail otherwise. In the revised manuscript we will add the standing assumption that M is complete, update the abstract, introduction, and main theorem statement accordingly, and note that all subsequent arguments remain valid under this hypothesis. No other changes to the proofs are required. revision: yes

Circularity Check

0 steps flagged

Direct existence proof without circular reduction

full rationale

The paper establishes existence and uniqueness of weak solutions for the doubly nonlinear parabolic equation via standard approximation schemes, monotonicity arguments, and passage to the limit in the weak formulation. No step reduces a claimed prediction or result to a fitted parameter, self-definition, or self-citation chain; the integration-by-parts identities and density arguments are invoked as standard properties of the p-Laplacian on Riemannian manifolds under the stated assumptions on p and q. The central claim therefore remains independent of its own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The result rests on standard properties of the p-Laplacian and weak-solution definitions on Riemannian manifolds; no free parameters or new entities are introduced.

axioms (2)
  • standard math The p-Laplacian is well-defined in the weak sense on any Riemannian manifold for p>1
    Invoked implicitly when writing the equation Δp u^q.
  • domain assumption Existence and uniqueness follow from standard monotone-operator or approximation techniques once the weak formulation is set
    The abstract claims a proof without exhibiting the steps, so the argument is assumed to rely on established PDE machinery.

pith-pipeline@v0.9.0 · 5424 in / 1227 out tokens · 28365 ms · 2026-05-16T10:29:27.840562+00:00 · methodology

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Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Long time upper bounds for solutions of Leibenson's equation on Riemannian manifolds

    math.AP 2026-04 unverdicted novelty 4.0

    A certain upper bound for weak solutions of the Leibenson equation on Riemannian manifolds is equivalent to a Euclidean-type Sobolev inequality.

Reference graph

Works this paper leans on

33 extracted references · 33 canonical work pages · cited by 1 Pith paper

  1. [1]

    Andreucci, A

    D. Andreucci, A. F. Tedeev, et al. Optimal decay rate for degenerate parabolic equations on noncompact manifolds.Methods Appl. Anal, 22(4):359–376, 2015

  2. [2]

    Barbu, S

    V. Barbu, S. Grube, M. Rehmeier, and M. R¨ ockner. The Leibenson process.arXiv preprint arXiv:2508.12979, 2025

  3. [3]

    B¨ ogelein, N

    V. B¨ ogelein, N. Dietrich, and M. Vestberg. Existence of solutions to a diffusive shallow medium equation.Journal of Evolution Equations, 21(1):845–889, 2021

  4. [4]

    B¨ ogelein, F

    V. B¨ ogelein, F. Duzaar, R. Korte, and C. Scheven. The higher integrability of weak solutions of porous medium systems.Advances in Nonlinear Analysis, 8(1):1004–1034, 2018

  5. [5]

    B¨ ogelein, F

    V. B¨ ogelein, F. Duzaar, and P. Marcellini. Parabolic systems withp, q-growth: a varia- tional approach.Archive for Rational Mechanics and Analysis, 210(1):219–267, 2013

  6. [6]

    Bonforte, G

    M. Bonforte, G. Grillo, and J. L. Vazquez. Fast diffusion flow on manifolds of nonpositive curvature.Journal of Evolution Equations, 8:99–128, 2008

  7. [7]

    P. Buser. A note on the isoperimetric constant.Ann. Sci. Ecole Norm. Sup., 15:213–230, 1982

  8. [8]

    De Giorgi

    E. De Giorgi. Sulla differenziabilit` a e l’analiticit` a delle estremali degli integrali multipli regolari.Mem. Accad. Sci. Torino, 3:25–43, 1957

  9. [9]

    De Ponti, M

    N. De Ponti, M. Muratori, and C. Orrieri. Wasserstein stability of porous medium- type equations on manifolds with Ricci curvature bounded below.Journal of Functional Analysis, 283(9):109661, 2022

  10. [10]

    S. Dekkers. Finite propagation speed for solutions of the parabolicp-laplace equation on manifolds.Communications in Analysis and Geometry, 13(4):741–768, 2005

  11. [11]

    Grigor’yan

    A. Grigor’yan. The heat equation on non-compact Riemannian manifolds.Math. USSR Sb., 72:47–77, 1992

  12. [12]

    Grigor’yan and P

    A. Grigor’yan and P. S¨ urig. Finite propagation speed for Leibenson’s equation on Rie- mannian manifolds.Comm. Anal. Geom., 2024

  13. [13]

    Grigor’yan and P

    A. Grigor’yan and P. S¨ urig. Sharp propagation rate for Leibenson’s equation on Rie- mannian manifolds.Ann. Scuola Norm. Super. Pisa, 2024

  14. [14]

    Grigor’yan and P

    A. Grigor’yan and P. S¨ urig. Upper bounds for solutions of Leibenson’s equation on Riemannian manifolds.Journal of Functional Analysis, page 110878, 2025

  15. [15]

    Grillo, D

    G. Grillo, D. D. Monticelli, and F. Punzo. The porous medium equation on noncompact manifolds with nonnegative Ricci curvature: A Green function approach.Journal of Differential Equations, 430:113191, 2025

  16. [16]

    Grillo and M

    G. Grillo and M. Muratori. Smoothing effects for the porous medium equation on Cartan–Hadamard manifolds.Nonlinear Analysis, 131:346–362, 2016

  17. [17]

    Grillo, M

    G. Grillo, M. Muratori, and F. Punzo. The porous medium equation with measure data on negatively curved Riemannian manifolds.Journal of the European Mathematical Society, 20(11):2769–2812, 2018. 28

  18. [18]

    Grillo, M

    G. Grillo, M. Muratori, and F. Punzo. Fast diffusion on noncompact manifolds: well- posedness theory and connections with semilinear elliptic equations.Transactions of the American Mathematical Society, 374(9):6367–6396, 2021

  19. [19]

    Grillo, M

    G. Grillo, M. Muratori, and J. L. V´ azquez. The porous medium equation on Riemannian manifolds with negative curvature. the large-time behaviour.Advances in Mathematics, 314:328–377, 2017

  20. [20]

    K. Ishige. On the existence of solutions of the cauchy problem for a doubly nonlinear parabolic equation.SIAM Journal on Mathematical Analysis, 27(5):1235–1260, 1996

  21. [21]

    Ivanov and P

    A. Ivanov and P. Mkrtychyan. Existence of H¨ older continuous generalized solutions of the first boundary value problem for quasilinear doubly degenerate parabolic equations. Journal of Soviet Mathematics, 62(3):2725–2740, 1992

  22. [22]

    A. V. Ivanov. Regularity for doubly nonlinear parabolic equations.Journal of Mathe- matical Sciences, 83(1):22–37, 1997

  23. [23]

    Kinnunen and P

    J. Kinnunen and P. Lindqvist. Pointwise behaviour of semicontinuous supersolutions to a quasilinear parabolic equation.Annali di Matematica Pura ed Applicata, 185(3):411–435, 2006

  24. [24]

    Ladyzhenskaya, V

    O. Ladyzhenskaya, V. Solonnikov, and N. Ural’tseva. Linear and quasilinear equations of parabolic type, transl. math.Monographs, Amer. Math. Soc, 23, 1968

  25. [25]

    Leibenson

    L. Leibenson. General problem of the movement of a compressible fluid in a porous medium. izv akad. nauk sssr.Geography and Geophysics, 9:7–10, 1945

  26. [26]

    Leibenson

    L. Leibenson. Turbulent movement of gas in a porous medium.Izv. Akad. Nauk SSSR Ser. Geograf. Geofiz, 9:3–6, 1945

  27. [27]

    Meglioli, F

    G. Meglioli, F. Oliva, and F. Petitta. Global existence for a Leibenson type equation with reaction on Riemannian manifolds.arXiv preprint arXiv:2505.08304, 2025

  28. [28]

    P.-A. Raviart. Sur la r´ esolution de certaines ´ equations paraboliques non lin´ eaires.Journal of Functional Analysis, 5(2):299–328, 1970

  29. [29]

    Saloff-Coste.Aspects of Sobolev-type inequalities

    L. Saloff-Coste.Aspects of Sobolev-type inequalities. LMS Lecture Notes Series, vol. 289. Cambridge Univ. Press, 2002

  30. [30]

    P. S¨ urig. Finite extinction time for subsolutions of the weighted Leibenson equation on Riemannian manifolds.arXiv preprint arXiv:2412.06496, 2024

  31. [31]

    P. S¨ urig. Sharp sub-Gaussian upper bounds for subsolutions of Trudinger’s equation on Riemannian manifolds.Nonlinear Analysis, 249:113641, 2024

  32. [32]

    P. S¨ urig. Gradient estimates for Leibenson’s equation on Riemannian manifolds.arXiv preprint arXiv:2506.07221, 2025

  33. [33]

    J. L. V´ azquez. Fundamental solution and long time behavior of the porous medium equa- tion in Hyperbolic space.Journal de Math´ ematiques Pures et Appliqu´ ees, 104(3):454– 484, 2015. Universit¨ at Bielefeld, Fakult¨ at f¨ ur Mathematik, Postfach 100131, D-33501, Bielefeld, Ger- many philipp.suerig@uni-bielefeld.de 29