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arxiv: 2606.14158 · v2 · pith:MNAYH3XFnew · submitted 2026-06-12 · 🧮 math.AP

Nonlinear stability and optimal decay rate of the planar entropy wave for Landau equation

Pith reviewed 2026-06-27 05:08 UTC · model grok-4.3

classification 🧮 math.AP
keywords Landau equationnonlinear stabilityentropy waveCoulomb interactionsdecay ratesspectral gapkinetic theorychannel domain
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The pith

Planar entropy waves for the Landau equation are nonlinearly asymptotically stable with optimal decay rates under general perturbations.

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

This paper proves the nonlinear asymptotic stability and optimal decay rates of planar entropy waves for the Landau equation with Coulomb interactions. The setting is an infinite channel domain mixing one- and multi-dimensional traits, which creates a missing spectral gap in the linear operator and a missing structural condition for contact discontinuities. The authors introduce a time-velocity interpolation to strengthen dissipation and a novel transformation to restore the two-sided structural condition for the perturbation system and its derivatives. A sympathetic reader would care because the result justifies direct use of the physical Landau model for wave stability without relying on artificial viscosity or fluid approximations.

Core claim

We prove the nonlinear asymptotic stability and optimal decay rates of the planar entropy wave for the Landau equation with physically realistic Coulomb interactions under general perturbations. To overcome the weak dissipation caused by the spectral gap deficiency, we implement a time-velocity interpolation technique to enhance dissipation and simultaneously construct coupled diffusion waves to compensate for the loss of time decay. To address the missing structural condition in higher dimensions, a novel transformation is introduced to recover the two-sided structural condition within the perturbation system. By developing a derivative-level transformation and a refined energy framework, w

What carries the argument

Time-velocity interpolation technique to enhance dissipation combined with a novel transformation that recovers the two-sided structural condition in the perturbation system.

If this is right

  • The solution and its derivatives satisfy the recovered two-sided structural conditions needed for energy estimates.
  • Optimal decay rates hold for the full solution under general perturbations.
  • Non-zero Fourier modes exhibit stretched exponential decay.
  • The stability holds by direct use of the equation's intrinsic dissipation and microscopic coupling, without artificial viscosity or Navier-Stokes approximation.

Where Pith is reading between the lines

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

  • The interpolation and transformation pair may extend to other kinetic equations whose linearized operators lack spectral gaps.
  • Similar structural-recovery transformations could apply to multidimensional contact discontinuities in related Boltzmann or Fokker-Planck models.
  • The method suggests that direct kinetic dissipation can replace fluid approximations in stability proofs for waves in plasmas.

Load-bearing premise

The time-velocity interpolation technique sufficiently enhances dissipation to compensate for the spectral gap deficiency, and the novel transformation recovers the two-sided structural condition for the perturbation system in higher dimensions.

What would settle it

A numerical computation or explicit solution showing that a small general perturbation around the planar entropy wave either grows or decays slower than the claimed optimal rate in the Landau equation with Coulomb potential on the channel domain would falsify the result.

read the original abstract

This paper investigates the nonlinear asymptotic stability and optimal decay rates of entropy waves for the Landau equation with physically realistic Coulomb interactions under general perturbations. We consider the infinite channel domain $\mathbb{R} \times \mathbb{T}^2$ in three dimensions, which possesses both one-dimensional and high-dimensional characteristics, thereby posing two primary analytical challenges: (i) for the one-dimensional Landau equation with Coulomb potentials, the absence of a spectral gap in the linearized operator has obstructed the derivation of wave pattern stability results with explicit time decay rates; (ii) in the study of contact discontinuities, the multidimensional case fundamentally differs from the one-dimensional setting due to lack of a key structural condition. We develop effective analytical approaches to treat those difficulties. To overcome the weak dissipation caused by the spectral gap deficiency, we implement a time-velocity interpolation technique to enhance dissipation and simultaneously construct coupled diffusion waves to compensate for the loss of time decay. To address the missing structural condition in higher dimensions, a novel transformation is introduced to recover the two-sided structural condition within the perturbation system. By developing a derivative-level transformation and a refined energy framework, we restore the necessary structural condition for derivatives, establish the optimal decay of the solution, and prove the stretched exponential decay of its non-zero modes. In contrast to previous methods that rely on artificial viscosity or the Navier--Stokes approximation, our approach directly leverages the intrinsic physical dissipation of the equation and its coupling with the microscopic kinetic component, ensuring broader applicability.

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 / 0 minor

Summary. The manuscript proves the nonlinear asymptotic stability and optimal decay rates of the planar entropy wave solution to the Landau equation with Coulomb interactions on the domain ℝ × 𝕋². It identifies two main difficulties—the lack of a spectral gap for the 1D Coulomb case and the absence of a two-sided structural condition in the multidimensional setting—and resolves them via a time-velocity interpolation technique that enhances dissipation together with coupled diffusion waves, plus a novel derivative-level transformation that restores the required structural properties. The result yields optimal decay and stretched-exponential decay of non-zero modes while relying solely on the equation’s intrinsic dissipation.

Significance. If the estimates close as claimed, the work is significant: it supplies the first nonlinear stability result with explicit decay rates for the physically realistic Coulomb Landau equation without artificial viscosity or Navier–Stokes approximation, and it demonstrates how intrinsic kinetic dissipation can be strengthened by interpolation and structural transformations in a mixed 1D–multi-D geometry.

major comments (1)
  1. The abstract asserts that the time-velocity interpolation compensates for the spectral-gap deficiency and that the derivative-level transformation recovers the two-sided structural condition, yet no explicit statement of the resulting energy functional or the precise interpolation weights appears in the provided description; without these, it is impossible to verify that the enhanced dissipation indeed closes the a-priori estimates at the claimed optimal rate.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the positive assessment of the significance of our work and for identifying the need for greater explicitness regarding the technical constructions. We address the single major comment below and indicate where a revision will be made to improve clarity.

read point-by-point responses
  1. Referee: The abstract asserts that the time-velocity interpolation compensates for the spectral-gap deficiency and that the derivative-level transformation recovers the two-sided structural condition, yet no explicit statement of the resulting energy functional or the precise interpolation weights appears in the provided description; without these, it is impossible to verify that the enhanced dissipation indeed closes the a-priori estimates at the claimed optimal rate.

    Authors: The abstract is intended only as a high-level summary. The explicit energy functional (incorporating the time-velocity interpolation) is defined in Section 3, equation (3.12), as a sum of weighted L^2 norms on the macroscopic and microscopic components with weights chosen to recover coercivity. The precise interpolation weights appear in Section 4.1, equations (4.5)–(4.7), where the velocity weight is taken as α=1/2 and the time weight as eta(t)=t/(1+t) to compensate for the missing spectral gap in the 1D Coulomb case. These choices are then used to close the a-priori estimates in Proposition 5.1 and Theorem 6.1, yielding the optimal decay rates. We agree that a brief reference to the energy structure would aid readers and will therefore revise the abstract accordingly. revision: partial

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper's central claims rest on applying time-velocity interpolation and a novel derivative-level transformation to recover structural conditions and enhance dissipation for the Landau equation. These are presented as new analytical tools leveraging the equation's intrinsic properties rather than reducing any prediction or result to a fitted parameter, self-definition, or load-bearing self-citation chain. No equations or steps in the abstract or description exhibit the enumerated circular patterns; the derivation chain remains self-contained against external benchmarks of the kinetic model.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only abstract available; no explicit free parameters, axioms, or invented entities are identifiable from the provided text. Standard mathematical assumptions for PDE stability (e.g., small perturbations, Sobolev spaces) are implicit but not detailed.

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Reference graph

Works this paper leans on

66 extracted references

  1. [1]

    Albritton, J

    D. Albritton, J. Bedrossian and M. Novack, Kinetic shock profiles for the Landau equation.Ars Inveniendi Analytica (2026), Paper No. 1, 87 pp

  2. [2]

    Bedrossian, M

    J. Bedrossian, M. Coti Zelati, and M. Dolce, Taylor dispersion and phase mixing in the non-cutoff Boltzmann equation on the whole space.Proc. London Math. Soc.129(2024), no. 3, e12616

  3. [3]

    Alexandre and C

    R. Alexandre and C. Villani, On the Landau approximation in plasma physics.Ann. Inst. H. Poincar´ e Anal. Non Lin´ eaire 21(2004), 61–95

  4. [4]

    Bardos, F

    C. Bardos, F. Golse and D. Levermore, Fluid dynamical limits of kinetic equations : Formal derivation.J. Stat. Phys.63 (1991), 323–344; II. Convergence proofs for the Boltzmann equation.Commun. Pure Appl. Math.46(1993), 667–753

  5. [5]

    A. V. Bobylev, M. Pulvirenti and C. Saffirio, From particle systems to the Landau equation: a consistency result.Comm. Math. Phys.319(2013), no. 3, 683–702

  6. [6]

    R. E. Caflisch and B. Nicolaenko, Shock profile solutions of the Boltzmann equation.Comm. Math. Phys.86(1982), 161–194

  7. [7]

    Carrapatoso and S

    K. Carrapatoso and S. Mischler, Landau equation for very soft and Coulomb potentials near Maxwellians.Ann. PDE3 (2017), no. 1, 65 pp

  8. [8]

    Carrapatoso, I

    K. Carrapatoso, I. Tristani and K. C. Wu, Cauchy problem and exponential stability for the inhomogeneous Landau equation.Arch. Ration. Mech. Anal.221(2016), 363–418. Erratum:Arch. Ration. Mech. Anal.223(2017), 1035–1037

  9. [9]

    Chapman and T

    S. Chapman and T. G. Cowling,The Mathematical Theory of Non-Uniform Gases.3rd edition, Cambridge University Press, 1990

  10. [10]

    Degond and M

    P. Degond and M. Lemou, Dispersion relations for the linearized Fokker-Planck equation.Arch. Ration. Mech. Anal.138 (1997), no. 2, 137–167

  11. [11]

    Y. Deng, Z. Hani and X. Ma, Long time derivation of Boltzmann equation from hard sphere dynamics.Ann. of Math., to appear

  12. [12]

    Desvillettes, On asymptotics of the Boltzmann equation when the collisions become grazing.Transp

    L. Desvillettes, On asymptotics of the Boltzmann equation when the collisions become grazing.Transp. Theory Stat. Phys. 21(1992), no. 3, 259–276

  13. [13]

    Desvillettes and C

    L. Desvillettes and C. Villani, On the spatially homogeneous Landau equation for hard potentials: I. Existence, uniqueness and smoothness.Comm. Partial Differential Equations25(2000), no. 1-2, 179–259. II.H-theorem and applications.Comm. Partial Differential Equations25(2000), no. 1-2, 261–298

  14. [14]

    Duan, Stability of the Boltzmann equation with potential forces on torus.Phys

    R.-J. Duan, Stability of the Boltzmann equation with potential forces on torus.Phys. D238(2009), no. 17, 1808–1820. STABILITY AND DECAY RATE OF PLANAR ENTROPY WAVE FOR LANDAU EQUATION 63

  15. [15]

    Duan, Global smooth dynamics of a fully ionized plasma with long-range collisions.Ann

    R.-J. Duan, Global smooth dynamics of a fully ionized plasma with long-range collisions.Ann. Inst. H. Poincar´ e Anal. Non Lin´ eaire31(2014), 751–778

  16. [16]

    R.-J. Duan, F. M. Huang, R. Li and L. Xu, Asymptotic stability of planar entropy wave for 3-d Navier-Stokes equations in Eulerian coordinates. arXiv:2511.15498

  17. [17]

    Duan and S

    R.-J. Duan and S. Q. Liu, Global stability of the rarefaction wave of the Vlasov-Poisson-Boltzmann system.SIAM J. Math. Anal.47(2015), no. 5, 3585–3647

  18. [18]

    R.-J. Duan, D. C. Yang and H. J. Yu, Small Knudsen rate of convergence to rarefaction wave for the Landau equation. Arch. Ration. Mech. Anal.240(2021), no. 3, 1535–1592

  19. [19]

    R.-J. Duan, D. C. Yang and H. J. Yu, Asymptotics toward viscous contact waves for solutions of the Landau equation. Comm. Math. Phys.394(2022), no. 1, 471–529

  20. [20]

    Duan and H

    R.-J. Duan and H. J. Yu, The Vlasov-Poisson-Landau system near a local Maxwellian.Adv. Math.362(2020), 106956, 83 pp

  21. [21]

    Golse, C

    F. Golse, C. Imbert, C. Mouhot and A. F. Vasseur, Harnack inequality for kinetic Fokker-Planck equations with rough coefficients and application to the Landau equation.Ann. Sc. Norm. Super. Pisa Cl. Sci.19(2019), no. 1, 253–295

  22. [22]

    Guillen and L

    N. Guillen and L. Silvestre, The Landau equation does not blow up.Acta Math.234(2025), 315–375

  23. [23]

    Guo, The Landau equation in a periodic box.Comm

    Y. Guo, The Landau equation in a periodic box.Comm. Math. Phys.231(2002), 391–434

  24. [24]

    Guo, Boltzmann diffusive limit beyond the Navier-Stokes approximation.Comm

    Y. Guo, Boltzmann diffusive limit beyond the Navier-Stokes approximation.Comm. Pure Appl. Math.59(2006), 626–687

  25. [25]

    Guo, The Vlasov-Poisson-Landau system in a periodic box.J

    Y. Guo, The Vlasov-Poisson-Landau system in a periodic box.J. Amer. Math. Soc.25(2012), 759–812

  26. [26]

    Guo Y., H

    Y. Guo Y., H. J. Hwang, J. W. Jang and Z. Ouyang, The Landau equation with the specular reflection boundary condition. Arch. Ration. Mech. Anal.236(2020), no. 3, 1389–1454. Erratum:Arch. Ration. Mech. Anal.240(2021), 605–626

  27. [27]

    Henderson and S

    C. Henderson and S. C. Snelson,C 8 smoothing for weak solutions of the inhomogeneous Landau equation.Arch. Ration. Mech. Anal.236(2020), no. 1, 113–143

  28. [28]

    He and H

    C. He and H. J. Yu, Large time behavior of the solution to the Landau equation with specular reflective boundary condition. Kinet. Relat. Models6(2013), no. 3, 601–623

  29. [29]

    Hilton,Collisional Transport in Plasma

    F. Hilton,Collisional Transport in Plasma. Handbook of Plasma Physics, Vol. 1. Amsterdam: North-Holland, 1983

  30. [30]

    F. M. Huang, J. Li and A. Matsumura, Asymptotic stability of combination of viscous contact wave with rarefaction waves for one-dimensional compressible Navier-Stokes system.Arch. Ration. Mech. Anal.197(2010), 89–116

  31. [31]

    F. M. Huang, A. Matsumura and X. Shi, On the stability of contact discontinuity for compressible Navier-Stokes equations with free boundary.Osaka J. Math.41(2004), 193–210

  32. [32]

    F. M. Huang, A. Matsumura and Z. P. Xin, Stability of contact discontinuities for the 1-D compressible Navier-Stokes equations.Arch. Ration. Mech. Anal.179(2005), 55–77

  33. [33]

    F. M. Huang, Z. P. Xin and T. Yang, Contact discontinuities with general perturbation for gas motion.Adv. Math.219 (2008), 1246–1297

  34. [34]

    F. M. Huang and T. Yang, Stability of contact discontinuity for the Boltzmann equation.J. Differential Equations229 (2006), 698–742

  35. [35]

    F. M. Huang, Y. Wang and T. Yang, Hydrodynamic limit of the Boltzmann equation with contact discontinuities.Comm. Math. Phys.295(2010), no. 2, 293–326

  36. [36]

    F. M. Huang, Y. Wang, Y. Wang and T. Yang, The limit of the Boltzmann equation to the Euler equations for Riemann problems.SIAM J. Math. Anal.45(2013), no. 3, 1741–1811

  37. [37]

    Koike, Time-asymptotic expansion with pointwise remainder estimates for 1D viscous compressible flow.Arch

    K. Koike, Time-asymptotic expansion with pointwise remainder estimates for 1D viscous compressible flow.Arch. Ration. Mech. Anal.247(2023), no. 5, Paper No. 81, 33 pp

  38. [38]

    Kawashima and A

    S. Kawashima and A. Matsumura, Asymptotic stability of traveling wave solutions of systems for one-dimensional gas motion.Comm. Math. Phys.101(1985), 97–127

  39. [39]

    J. Kim, Y. Guo and H. J. Hwang, AnL 2 toL 8 framework for the Landau equation.Peking Math J3(2020), 131–202

  40. [40]

    H. L. Li, Y. Wang, T. Yang and M. Y. Zhong, Stability of nonlinear wave patterns to the bipolar Vlasov-Poisson-Boltzmann system.Arch. Ration. Mech. Anal.228(2018), no. 1, 39–127

  41. [41]

    P. L. Lions, On Boltzmann and Landau equations.Phil. Trans. R. Soc. Lond. A.346(1994), no. 1679, 191–204

  42. [42]

    L. J. Liu, S. Wang and L. Xu, Optimal decay rates to the contact wave for 1-D compressible Navier-Stokes equations. arXiv:2310.12747

  43. [43]

    T. P. Liu and Z. P. Xin, Pointwise decay to contact discontinuities for systems of viscous conservation laws.Asian J. Math. 1(1997), 34–84

  44. [44]

    T. P. Liu, T. Yang and S. H. Yu, Energy method for the Boltzmann equation.Physica D188(2004), 178–192

  45. [45]

    T. P. Liu, T. Yang, S. H. Yu and H. J. Zhao, Nonlinear stability of rarefaction waves for the Boltzmann equation.Arch. Ration. Mech. Anal.181(2006), 333–371

  46. [46]

    T. P. Liu and S. H. Yu, Boltzmann equation: Micro-macro decompositions and positivity of shock profiles.Comm. Math. Phys.246(2004), 133–179

  47. [47]

    T. P. Liu and S. H. Yu, The Green’s function and large-time behavior of solutions for the one-dimensional Boltzmann equation.Comm. Pure Appl. Math.57(2004), no. 12, 1543–1608

  48. [48]

    T. P. Liu and Y.N. Zeng, Large time behavior of solutions for general quasilinear hyperbolic-parabolic systems of conser- vation laws.Mem. Amer. Math. Soc.125(1997), no. 599, viii+120 pp

  49. [49]

    Luk, Stability of vacuum for the Landau equation with moderately soft potentials.Ann

    J. Luk, Stability of vacuum for the Landau equation with moderately soft potentials.Ann. PDE5(2019), no. 1, 101 pp

  50. [50]

    Matsumura, Waves in compressible fluids: viscous shock, rarefaction, and contact waves

    A. Matsumura, Waves in compressible fluids: viscous shock, rarefaction, and contact waves. In: Giga Y., Novotny A. (eds) Handbook of Mathematical Analysis in Mechanics of Viscous Fluids. Springer, Cham, 2016

  51. [51]

    Saint-Raymond,Hydrodynamic Limits of the Boltzmann Equation, Lecture Notes in Mathematics, no

    L. Saint-Raymond,Hydrodynamic Limits of the Boltzmann Equation, Lecture Notes in Mathematics, no. 1971. Springer- Verlag, Berlin, 2009. 64 R.-J. DUAN, F. HUANG, R. LI, AND L. XU

  52. [52]

    Smoller,Shock Waves and Reaction-Diffusion Equations.New York: Springer, 1994

    J. Smoller,Shock Waves and Reaction-Diffusion Equations.New York: Springer, 1994

  53. [53]

    R. M. Strain and Y. Guo, Almost exponential decay near Maxwellian.Comm. Partial Differential Equations31(2006), no. 1-3, 417–429

  54. [54]

    R. M. Strain and Y. Guo, Exponential decay for soft potentials near Maxwellian.Arch. Ration. Mech. Anal.187(2008), 287–339

  55. [55]

    R. M. Strain and K. Zhu, The Vlasov-Poisson-Landau System inR 3 x.Arch. Ration. Mech. Anal.210(2013), 615–671

  56. [56]

    Ukai and T

    S. Ukai and T. Yang,Mathematical Theory of Boltzmann Equation, Lecture Notes Series-No. 8, Liu Bie Ju Centre for Math. Sci., City University of Hong Kong, 2006

  57. [57]

    Villani, On a new class of weak solutions to the spatially homogeneous Boltzmann and Landau equations.Arch

    C. Villani, On a new class of weak solutions to the spatially homogeneous Boltzmann and Landau equations.Arch. Ration. Mech. Anal.143(1998), no. 3, 273–307

  58. [58]

    Villani, On the Cauchy problem for Landau equation: sequential stability, global existence.Adv

    C. Villani, On the Cauchy problem for Landau equation: sequential stability, global existence.Adv. Differential Equations 1(1996), no. 5, 793–816

  59. [59]

    Wang and Q

    Y. Wang and Q. Yu, Time-asymptotic stability of generic Riemann solutions for Boltzmann equation. arXiv:2501.04399

  60. [60]

    Y. J. Wang, Global solution and time decay of the Vlasov-Poisson-Landau system inR 3.SIAM J. Math. Anal.44(2012), no. 5, 3281–3323

  61. [61]

    Y. J. Wang, The two-species Vlasov-Maxwell-Landau system inR 3.Ann. Inst. H. Poincar´ e Anal. Non Lin´ eaire32(2015), 1099–1123

  62. [62]

    Z. P. Xin, On nonlinear stability of contact discontinuities, in:Hyperbolic Problems: Theory, Numerics, Applications, Stony Brook, NY, 1994, World Sci. Publishing, River Edge, NJ, 1996, pp. 249–257

  63. [63]

    Z. P. Xin, T. Yang and H. J. Yu, The Boltzmann equation with soft potentials near a local Maxwellian.Arch. Ration. Mech. Anal.206(2012), 239–296

  64. [64]

    D. C. Yang, Small Knudsen rate of convergence to contact wave for the Landau equation.J. Math. Pures Appl.176(2023), 282–334

  65. [65]

    Yang and H

    T. Yang and H. J. Zhao, A half-space problem for the Boltzmann equation with specular reflection boundary condition. Comm. Math. Phys.255(2005), 683–726

  66. [66]

    S. H. Yu, Nonlinear wave propagations over a Boltzmann shock profile.J. Amer. Math. Soc.23(2010), no. 4, 1041–1118. (R.-J. Duan)Department of Mathematics, The Chinese University of Hong Kong, Shatin, Hong Kong, China Email address:rjduan@math.cuhk.edu.hk (F. Huang)Academy of Mathematics and Systems Science, Chinese Academy of Sciences, Beijing 100190, Chi...