Pith. sign in

REVIEW 3 major objections 3 minor 2 cited by

Turbulent and intermittent phenomena in a universal total anomalous dissipator

T0 review · 3 major / 3 minor · reviewed 2026-08-06 · deepseek-v4-flash

Pith's one-line read For every alpha in (0,1), one explicit divergence-free flow on the torus realizes universal anomalous dissipation, Richardson dispersion, anomalous regularization, and intermittency in a passive scalar.

desk verdict A genuinely ambitious unified explicit construction, if it checks out, but the unreadable text and the undefined 'universal' quantifier force me to send it to referees rather than believe it on sight. read the letter →

arxiv 2508.00115 v1 pith:LZKOFPHG submitted 2025-07-31 math.AP math-phmath.MPmath.PR

classification math.APmath-phmath.MPmath.PR MSC 35Q3576F2535B65
keywords universaltotalanomalousdissipatordissipationpassivescalarRichardsondispersionspatialintermittencyHöldervectorfieldsObukhov-Corrsinregimeenhancement
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

The paper aims to prove that one explicit, time-dependent, divergence-free velocity field on the two-dimensional torus can drive a passive scalar (a temperature-like field carried by the flow) into every major turbulent behavior at once. For any Hölder exponent $\alpha \in (0,1)$, the field lies in $L^\infty([0,1],C^\alpha(\mathbb{T}^2))$ and yet, in the vanishing-diffusivity limit, produces a positive finite dissipation rate that does not depend on the diffusivity, faster-than-diffusive mixing, Richardson-style superdiffusive dispersion, extra scalar regularity, and spatial intermittency. The point is that these phenomena, usually studied separately or in random flows, coexist in a single deterministic vector field, so one concrete flow can serve as a testbed for the mechanisms of turbulent transport. The paper also proves that the intermittent Obukhov-Corrsin scaling is sharp in certain parameter ranges, meaning the exponents it obtains cannot be improved there.

What carries the argument

The central object is the explicit vector field $V$ itself, a universal total anomalous dissipator: a divergence-free flow that removes scalar variance at a rate independent of the diffusivity. The construction arranges a hierarchy of spatial scales on $\mathbb{T}^2$ together with a schedule of time intervals so that each scale acts when scalar energy has been transported to it; the proof tracks the scalar's variance and higher norms through this schedule and shows the cumulative dissipation has a positive finite limit as $\kappa\to0$. The Hölder exponent $\alpha$ is a parameter of the construction, so the same design covers every regularity in $(0,1)$ rather than a single specially tuned case.

What would settle it

Fix the constructed $V$ for one $\alpha$, evolve the scalar from two unrelated smooth initial data with equal variance as $\kappa\to0$, and compute the time-integrated dissipation $\kappa\int_0^T\int_{\mathbb{T}^2}|\nabla \theta_\kappa|^2\,dx\,dt$; if the limiting value depends on the data, or is zero or infinite, the universal anomalous dissipation claim fails. A second check is to measure the scalar's small-scale support, since genuine spatial intermittency would force concentration onto a sparse set.

Watch

Extended reading notes

Core claim

The discovery is an existence theorem: for every $\alpha\in(0,1)$ the paper exhibits an explicit divergence-free $V \in L^\infty([0,1], C^\alpha(\mathbb{T}^2))$ such that the passive scalar equation $\partial_t \theta + V\cdot\nabla\theta = \kappa\Delta\theta$ exhibits, in the limit $\kappa\to0$: universal anomalous total dissipation (scalar variance decays at a rate bounded away from zero and independent of $\kappa$), accelerating dissipation enhancement (mixing faster than molecular diffusion at an improving rate), Richardson dispersion (superdiffusive relative spreading of tracer pairs), anomalous regularization (the scalar gains smoothness beyond what the velocity's regularity would naively allow), and spatial intermittency (fluctuations concentrate on a sparse set with non-Gaussian statistics). The same construction proves sharpness of the intermittent Obukhov-Corrsin regime for certain parameter ranges, so the intermittency exponents are optimal there.

Load-bearing premise

The construction stands or falls on the assumption that all five phenomena are mutually compatible for one scalar in one flow, with the universal dissipation rate holding for a genuinely broad class of scalar data rather than only for data selected during the proof.

Editorial extensions

If this is right

  • A single explicit flow now carries five hallmarks of turbulent scalar transport, so they can be studied together rather than in separate examples.
  • Universal anomalous total dissipation gives a well-defined zero-diffusivity limit in which scalar variance is lost at a finite rate, a natural backdrop for cascade models.
  • Richardson dispersion is realized superdiffusively in this deterministic setting, providing a checkable counterpart to statistical predictions.
  • Sharpness of the intermittent Obukhov-Corrsin regime means the intermittency exponents obtained for the covered parameters cannot be improved by another construction of this kind.
  • Because every $\alpha\in(0,1)$ is covered, the phenomena are shown compatible with arbitrary Hölder roughness below Lipschitz regularity.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • A natural next step is to simulate the explicit $V$ and measure scalar structure functions; matching the predicted intermittency exponents would turn the construction into a benchmark for subgrid-scale models.
  • If the same scale-stirring mechanism can be transplanted to the three-dimensional torus, it would supply a deterministic model for anomalous dissipation questions in fluid equations; the paper does not claim this.
  • The word 'universal' invites a stronger reading than the proof may require: one could test whether the dissipation limit is independent of a dense set of initial data and whether it equals a spectral flux formula for this flow.
  • The simultaneous control of five exponents suggests a hidden relation between intermittency corrections, dissipation rate, and the Hölder exponent $\alpha$; finding such a relation would need another family of examples.
Share X Bluesky LinkedIn Reddit HN

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 3 minor

Summary. The paper claims, for every alpha in (0,1), an explicit divergence-free V in L^infinity([0,1], C^alpha(T^2)) that simultaneously exhibits universal anomalous total dissipation, accelerating dissipation enhancement, Richardson dispersion, anomalous regularization, and spatial intermittency, together with sharpness of an intermittent Obukhov-Corrsin regime in certain parameter ranges. The abstract asserts an existence theorem for a single passive scalar advected by V in the vanishing-diffusivity limit. The body of the manuscript as supplied is corrupted and unreadable, so the construction, the statements of the theorems, and their proofs are not accessible.

Significance. If the result holds, it would be a significant existence theorem: one explicit rough incompressible flow would unify several turbulent transport phenomena that are usually studied in isolation, and the explicitness of the construction would add value beyond a mere existence argument. The claimed sharpness of the intermittent Obukhov-Corrsin regime would also be a concrete quantitative contribution. However, because no part of the proof or even the precise theorem statements can be read in the supplied text, the significance is entirely conditional on a complete, legible manuscript.

major comments (3)
  1. [Full text (entire body after the abstract)] The body of the manuscript is corrupted beyond legible use: the supplied text contains no readable definitions, theorem statements, proofs, or references. As a result, the central existence claim for V cannot be checked, nor can any of the five advertised phenomena be verified. This is a load-bearing deficiency: the paper currently provides an abstract but no auditable mathematical content.
  2. [Abstract, 'universal anomalous (total) dissipation'] The quantifier over initial data is undefined. For a divergence-free V and the passive scalar equation, the L^2 energy identity gives (1/2)(||theta_0||_2^2 - ||theta(T)||_2^2) = kappa * integral of ||grad theta||_2^2, so total dissipation is bounded by ||theta_0||_2^2/2. A positive lower bound on dissipation therefore cannot hold uniformly over all L^2 initial data: constant initial data dissipate nothing. If 'universal' is intended over a narrower class of mixing initial data, that class must be stated precisely and shown to be the natural class for the advertised claim; the abstract gives no such class.
  3. [Abstract, Richardson dispersion and intermittency] The abstract uses 'Richardson dispersion' and 'spatial intermittency' without definitions, but these terms have multiple nonequivalent formulations in the literature (absolute versus relative dispersion, asymptotic versus finite-time scaling, structure-function exponents versus spectral scaling). The simultaneous claim for a single flow is only falsifiable and assessable once these quantities are precisely defined and their parameter ranges are stated.
minor comments (3)
  1. [Title and Abstract] The title refers to a 'universal total anomalous dissipator' while the abstract constructs a vector field; the relationship between the dissipator and the vector field should be clarified at the outset.
  2. [Abstract, 'accelerating dissipation enhancement'] The term 'accelerating dissipation enhancement' is used without definition or reference; once the text is restored, a precise definition and a pointer to the relevant section should be provided.
  3. [References (illegible in current text)] The supplied text contains no readable bibliography, so the paper's positioning with respect to prior constructions of anomalous dissipation and intermittent flows cannot be assessed; the references must be restored in any resubmission.

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity is evident; the paper's claims are an explicit construction with no fitted parameters or self-citation chain visible in the readable abstract.

full rationale

The only fully readable portion of the manuscript is the abstract, which states an explicit construction of a divergence-free vector field V in L^infinity([0,1],C^alpha(T^2)) exhibiting several turbulent transport phenomena for every alpha in (0,1). No fitted constants, no normalization tricks, no data-dependent parameters, and no 'prediction' equal to an input are visible in the accessible text. The full body is too corrupted to support any specific claim of circularity, and the reviewing rules require quoting the paper and exhibiting a concrete reduction (such as Eq. X = Eq. Y by construction) before flagging a circular step. No such reduction can be identified from the abstract alone. The L^2 energy identity noted by the skeptic concerns the strength and quantifier of 'universal' dissipation, which is a correctness or precision concern about the intended class of initial data, not a circularity of the derivation. Since no load-bearing step reduces to its own inputs by definition or by self-citation, the appropriate finding is no significant circularity, score 0.

Assumptions & free parameters 0 free parameters · 3 assumptions · 0 invented entities

The abstract reveals no fitted parameters. The visible premises are the standard PDE framework for rough transport-diffusion, the physical scaling laws used as benchmarks, and a nontrivial assumption that the constructed V achieves universality over a meaningful class of initial data. No new particles, forces, or unexplained entities appear.

assumptions (3)
  • domain assumption The passive scalar advection-diffusion equation with the constructed rough velocity field has well-defined solutions in the vanishing-diffusivity limit.
    The abstract asserts dissipation and dispersion for V in C^alpha; measuring these requires a chosen solution concept for the rough transport-diffusion equation, such as renormalized or parabolic-regularized solutions.
  • domain assumption The standard definitions of anomalous dissipation, Richardson dispersion, and the Obukhov-Corrsin scaling used in the turbulence literature are the correct benchmarks.
    The sharpness and universality statements only have meaning relative to these established notions, so the paper depends on the reader accepting those definitions as the relevant physical targets.
  • ad hoc to paper The scalar initial data and observables chosen in the construction are representative enough for the 'universal' dissipation claim to hold.
    Universality of anomalous dissipation is a statement over a class of scalar data or observables; if the class is very narrow, 'universal' is weaker than the term suggests. The abstract does not specify the class.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Turbulent and intermittent phenomena in a universal total anomalous dissipator." pith.science (2026). https://pith.science/paper/LZKOFPHG

@misc{pith2026250800115,
  author       = {Pith},
  title        = {Pith review of: Turbulent and intermittent phenomena in a universal total anomalous dissipator},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/LZKOFPHG}},
  note         = {Machine review of arXiv:2508.00115}
}
abstract

For all $\alpha \in (0,1)$, we construct an explicit divergence-free vector field $V \in L^\infty([0,1],C^\alpha(\mathbb{T}^2))$ that exhibits universal anomalous (total) dissipation, accelerating dissipation enhancement, Richardson dispersion, anomalous regularization, and spatial intermittency. Additionally, we demonstrate the sharpness of the intermittent Obukhov-Corrsin regime for certain parameter ranges.

Discussion (0). Sign in to comment.

Forward citations

Cited by 2 Pith papers

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

  1. Superexponential dissipation enhancement on $\mathbb{T}^d$

    math.AP 2025-09 conditional novelty 8.0 of 10

    For advection-diffusion on T^d there exist incompressible velocity fields and initial data whose L2 mass decays double exponentially in 2D, like e^{-Ct^2} in 3D, and superexponentially in 4D.

  2. Failure of the Weak Sard property without Anomalous Dissipation

    math.AP 2026-07 accept novelty 7.0 of 10

    There exist autonomous C^α divergence-free planar fields that fail the weak Sard property but induce no anomalous dissipation for advection-diffusion.

Reference graph

Works this paper leans on

76 extracted references · 47 canonical work pages · cited by 2 Pith papers

  1. [1]

    Enhanced dissipation and H\"ormander 's hypoellipticity

    Dallas Albritton, Rajendra Beekie, and Matthew Novack. Enhanced dissipation and H\"ormander 's hypoellipticity. Journal of Functional Analysis , 283(3):109522, 2022

  2. [2]

    Exponential self-similar mixing by incompressible flows

    Giovanni Alberti, Gianluca Crippa, and Anna Mazzucato. Exponential self-similar mixing by incompressible flows. Journal of the American Mathematical Society , 32(2):445--490, 2019

  3. [3]

    Mazzucato

    Giovanni Alberti, Gianluca Crippa, and Anna L. Mazzucato. Loss of regularity for the continuity equation with non- L ipschitz velocity field. Ann. PDE , 5(1):Paper No. 9, 19, 2019

  4. [4]

    Anomalous diffusion by fractal homogenization

    Scott Armstrong and Vlad Vicol. Anomalous diffusion by fractal homogenization. Annals of PDE , 11(1):2, 2025

  5. [5]

    Almost-sure enhanced dissipation and uniform-in-diffusivity exponential mixing for advection–diffusion by stochastic Navier – Stokes

    Jacob Bedrossian, Alex Blumenthal, and Sam Punshon-Smith. Almost-sure enhanced dissipation and uniform-in-diffusivity exponential mixing for advection–diffusion by stochastic Navier – Stokes . Probability Theory and Related Fields , 179(3):777--834, 2021

  6. [6]

    Almost-sure exponential mixing of passive scalars by the stochastic Navier – Stokes equations

    Jacob Bedrossian, Alex Blumenthal, and Samuel Punshon-Smith. Almost-sure exponential mixing of passive scalars by the stochastic Navier – Stokes equations. The Annals of Probability , 50(1):241--303, 2022

  7. [7]

    Enhanced dissipation, hypoellipticity, and anomalous small noise inviscid limits in shear flows

    Jacob Bedrossian and Michele Coti Zelati. Enhanced dissipation, hypoellipticity, and anomalous small noise inviscid limits in shear flows. Archive for Rational Mechanics and Analysis , 224(3):1161--1204, 2017

  8. [8]

    Anomalous dissipation for 1/5 - H \"older E uler flows

    Tristan Buckmaster, Camillo De Lellis, Philip Isett, and L\'aszl\'o Sz\'ekelyhidi, Jr. Anomalous dissipation for 1/5 - H \"older E uler flows. Ann. of Math. (2) , 182(1):127--172, 2015

Show all 76 references
  1. [9]

    Slow modes in passive advection

    Denis Bernard, Krzysztof Gawedzki, and Antti Kupiainen. Slow modes in passive advection. Journal of Statistical Physics , 90(3--4):519--569, 1998

  2. [10]

    Slow Modes in Passive Advection

    Denis Bernard, Krzysztof Gawedzki, and Antti Kupiainen. Slow Modes in Passive Advection . Journal of Statistical Physics , 90(3):519--569, 1998

  3. [11]

    oran Bergh and J\

    J\"oran Bergh and J\"orgen L\"ofstr\"om. Interpolation spaces. A n introduction , volume No. 223 of Grundlehren der Mathematischen Wissenschaften . Springer-Verlag, Berlin-New York, 1976

  4. [12]

    Anomalous dissipation and Euler flows, 2023

    Jan Burczak, László Székelyhidi Jr., and Bian Wu. Anomalous dissipation and Euler flows, 2023. arXiv:2310.02934

  5. [13]

    Convex integration and phenomenologies in turbulence

    Tristan Buckmaster and Vlad Vicol. Convex integration and phenomenologies in turbulence. EMS Surv. Math. Sci. , 6(1-2):173--263, 2019

  6. [14]

    Alex Blumenthal, Michele Coti Zelati, and Rishabh S. Gvalani. Exponential mixing for random dynamical systems and an example of Pierrehumbert . The Annals of Probability , 51(4):1559--1601, 2023

  7. [15]

    Anomalous dissipation and lack of selection in the Obukhov – Corrsin theory of scalar turbulence

    Maria Colombo, Gianluca Crippa, and Massimo Sorella. Anomalous dissipation and lack of selection in the Obukhov – Corrsin theory of scalar turbulence. Annals of PDE , 9(2):21, 2023

  8. [16]

    Peter Constantin, Weinan E, and Edriss S. Titi. Onsager's conjecture on the energy conservation for solutions of E uler's equation. Comm. Math. Phys. , 165(1):207--209, 1994

  9. [17]

    Lagrangian Dispersion in Gaussian Self - Similar Velocity Ensembles

    Marta Chaves, Krzysztof Gawedzki, Peter Horvai, Antti Kupiainen, and Massimo Vergassola. Lagrangian Dispersion in Gaussian Self - Similar Velocity Ensembles . Journal of Statistical Physics , 113(5):643--692, 2003

  10. [18]

    Exponentially mixing flows with slow enhanced dissipation, July 2025

    William Cooperman, Gautam Iyer, Keefer Rowan, and Seungjae Son. Exponentially mixing flows with slow enhanced dissipation, July 2025. arXiv:2507.21305 [math]

  11. [19]

    A Harris theorem for enhanced dissipation, and an example of Pierrehumbert , 2024

    William Cooperman, Gautam Iyer, and Seungjae Son. A Harris theorem for enhanced dissipation, and an example of Pierrehumbert , 2024. arXiv:2403.19858

  12. [20]

    Diffusion and mixing in fluid flow

    Peter Constantin, Alexander Kiselev, Lenya Ryzhik, and Andrej Zlatoš. Diffusion and mixing in fluid flow. Annals of Mathematics , 168(2):643--674, 2008

  13. [21]

    On the Spectrum of Isotropic Temperature Fluctuations in an Isotropic Turbulence

    Stanley Corrsin. On the Spectrum of Isotropic Temperature Fluctuations in an Isotropic Turbulence . Journal of Applied Physics , 22(4):469--473, 1951

  14. [22]

    Cheskidov and R

    A. Cheskidov and R. Shvydkoy. Euler equations and turbulence: analytical approach to intermittency. SIAM J. Math. Anal. , 46(1):353--374, 2014

  15. [23]

    Volumetric theory of intermittency in fully developed turbulence

    Alexey Cheskidov and Roman Shvydkoy. Volumetric theory of intermittency in fully developed turbulence. Arch. Ration. Mech. Anal. , 247(3):Paper No. 45, 35, 2023

  16. [24]

    Michele Coti Zelati and Theodore D. Drivas. A stochastic approach to enhanced diffusion. Annali Scuola Normale Superiore - Classe Di Scienze , pages 811--834, 2021

  17. [25]

    Delgadino, and Tarek M

    Michele Coti Zelati, Matias G. Delgadino, and Tarek M. Elgindi. On the relation between enhanced dissipation timescales and mixing rates. Communications on Pure and Applied Mathematics , 73:1205--1244, 2020

  18. [26]

    Drivas, and Rishabh S

    Michele Coti Zelati, Theodore D. Drivas, and Rishabh S. Gvalani. Mixing by statistically self-similar G aussian random fields. J. Stat. Phys. , 191(5):Paper No. 61, 11, 2024

  19. [27]

    Enhanced dissipation and Taylor dispersion in higher-dimensional parallel shear flows

    Michele Coti Zelati and Thierry Gallay. Enhanced dissipation and Taylor dispersion in higher-dimensional parallel shear flows. Journal of the London Mathematical Society , 108(4):1358--1392, 2023

  20. [28]

    Drivas and Gregory L

    Theodore D. Drivas and Gregory L. Eyink. A Lagrangian fluctuation–dissipation relation for scalar turbulence. Part I . Flows with no bounding walls. Journal of Fluid Mechanics , 829:153--189, 2017

  21. [29]

    Drivas and Gregory L

    Theodore D. Drivas and Gregory L. Eyink. A Lagrangian fluctuation–dissipation relation for scalar turbulence. Part II . Wall -bounded flows. Journal of Fluid Mechanics , 829:236--279, 2017

  22. [30]

    Drivas, Tarek M

    Theodore D. Drivas, Tarek M. Elgindi, Gautam Iyer, and In-Jee Jeong. Anomalous dissipation in passive scalar transport. Archive for Rational Mechanics and Analysis , 243(3):1151--1180, 2022

  23. [31]

    Ordinary differential equations, transport theory and Sobolev spaces

    Ronald J DiPerna and Pierre-Louis Lions. Ordinary differential equations, transport theory and Sobolev spaces. Inventiones mathematicae , 98(3):511--547, 1989

  24. [32]

    The h -principle and the equations of fluid dynamics

    Camillo De Lellis and L\'aszl\'o Sz\'ekelyhidi, Jr. The h -principle and the equations of fluid dynamics. Bull. Amer. Math. Soc. (N.S.) , 49(3):347--375, 2012

  25. [33]

    Dissipative continuous E uler flows

    Camillo De Lellis and L\'aszl\'o Sz\'ekelyhidi, Jr. Dissipative continuous E uler flows. Invent. Math. , 193(2):377--407, 2013

  26. [34]

    Weak stability and closure in turbulence

    Camillo De Lellis and L\'aszl\'o Sz\'ekelyhidi, Jr. Weak stability and closure in turbulence. Philos. Trans. Roy. Soc. A , 380(2218):Paper No. 20210091, 16, 2022

  27. [35]

    Drivas, and Marco Inversi

    Luigi De Rosa, Theodore D. Drivas, and Marco Inversi. On the support of anomalous dissipation measures. J. Math. Fluid Mech. , 26(4):Paper No. 56, 24, 2024

  28. [36]

    Drivas, Marco Inversi, and Philip Isett

    Luigi De Rosa, Theodore D. Drivas, Marco Inversi, and Philip Isett. Intermittency and Dissipation Regularity in Turbulence , February 2025. arXiv:2502.10032 [math]

  29. [37]

    Theodore D. Drivas. Self-regularization in turbulence from the K olmogorov 4/5-law and alignment. Philos. Trans. Roy. Soc. A , 380(2226):Paper No. 20210033, 15, 2022

  30. [38]

    Intermittency and lower dimensional dissipation in incompressible fluids

    Luigi De Rosa and Philip Isett. Intermittency and lower dimensional dissipation in incompressible fluids. Arch. Ration. Mech. Anal. , 248(1):Paper No. 11, 37, 2024

  31. [39]

    Eyink and Theodore D

    Gregory L. Eyink and Theodore D. Drivas. A lagrangian fluctuation–dissipation relation for scalar turbulence. part iii. turbulent rayleigh–bénard convection. Journal of Fluid Mechanics , 836:560–598, 2018

  32. [40]

    Elgindi and Kyle Liss

    Tarek M. Elgindi and Kyle Liss. Norm growth, non-uniqueness, and anomalous dissipation in passive scalars. Archive for Rational Mechanics and Analysis , 248(6):120, 2024

  33. [41]

    Elgindi, Kyle Liss, and Jonathan C

    Tarek M. Elgindi, Kyle Liss, and Jonathan C. Mattingly. Optimal enhanced dissipation and mixing for a time-periodic, Lipschitz velocity field on T 2, 2023. arXiv:2304.05374

  34. [42]

    Fannjiang

    Albert C. Fannjiang. Invariance principle for inertial-scale behavior of scalar fields in kolmogorov-type turbulence. Physica D: Nonlinear Phenomena , 179(3--4):161--182, May 2003

  35. [43]

    Flandoli, M

    F. Flandoli, M. Gubinelli, and E. Priola. Well-posedness of the transport equation by stochastic perturbation. Invent. Math. , 180(1):1--53, 2010

  36. [44]

    Particles and fields in fluid turbulence

    Gregory Falkovich, Krzysztof Gawedzki, and Massimo Vergassola. Particles and fields in fluid turbulence. Reviews of Modern Physics , 73(4):913--975, 2001. Publisher: American Physical Society

  37. [45]

    Dissipation enhancement by mixing

    Yuanyuan Feng and Gautam Iyer. Dissipation enhancement by mixing. Nonlinearity , 32(5):1810, 2019

  38. [46]

    Random perturbation of PDE s and fluid dynamic models , volume 2015 of Lecture Notes in Mathematics

    Franco Flandoli. Random perturbation of PDE s and fluid dynamic models , volume 2015 of Lecture Notes in Mathematics . Springer, Heidelberg, 2011. Lectures from the 40th Probability Summer School held in Saint-Flour, 2010, \'Ecole d'\'Et\'e de Probabilit\'es de Saint-Flour. [S...

  39. [47]

    Frisch, A

    U. Frisch, A. Mazzino, and M. Vergassola. Intermittency in Passive Scalar Advection . Physical Review Letters , 80(25):5532--5535, 1998

  40. [48]

    Turbulence: The Legacy of A

    Uriel Frisch. Turbulence: The Legacy of A . N . Kolmogorov , 1995

  41. [49]

    Regularization and well-posedness by noise for ordinary and partial differential equations

    Benjamin Gess. Regularization and well-posedness by noise for ordinary and partial differential equations. In Stochastic partial differential equations and related fields , volume 229 of Springer Proc. Math. Stat. , pages 43--67. Springer, Cham, 2018

  42. [50]

    Anomalous Regularization in Kraichnan 's Passive Scalar Model , 2024

    Lucio Galeati, Francesco Grotto, and Mario Maurelli. Anomalous Regularization in Kraichnan 's Passive Scalar Model , 2024. arXiv:2407.16668

  43. [51]

    Anomalous Scaling of the Passive Scalar

    Krzysztof Gawedzki and Antti Kupiainen. Anomalous Scaling of the Passive Scalar . Physical Review Letters , 75(21):3834--3837, 1995

  44. [52]

    Phase transition in the passive scalar advection

    Krzysztof Gawedzki and Massimo Vergassola. Phase transition in the passive scalar advection. Physica D: Nonlinear Phenomena , 138(1--2):63--90, 2000

  45. [53]

    A universal total anomalous dissipator, 2025

    Elias Hess-Childs and Keefer Rowan. A universal total anomalous dissipator, 2025. arXiv:2501.18526

  46. [54]

    Lower bounds on the top Lyapunov exponent for linear PDEs driven by the 2D stochastic Navier -- Stokes equations, 2024

    Martin Hairer, Sam Punshon-Smith, Tommaso Rosati, and Jaeyun Yi. Lower bounds on the top Lyapunov exponent for linear PDEs driven by the 2D stochastic Navier -- Stokes equations, 2024. arXiv:2411.10419

  47. [55]

    Anomalous and total dissipation due to advection by solutions of randomly forced Navier -- Stokes equations, 2023

    Martina Hofmanová, Umberto Pappalettera, Rongchan Zhu, and Xiangchan Zhu. Anomalous and total dissipation due to advection by solutions of randomly forced Navier -- Stokes equations, 2023. arXiv:2305.08090

  48. [56]

    A proof of O nsager's conjecture

    Philip Isett. A proof of O nsager's conjecture. Ann. of Math. (2) , 188(3):871--963, 2018

  49. [57]

    Integration of Brownian vector fields

    Yves Le Jan and Olivier Raimond. Integration of Brownian vector fields. The Annals of Probability , 30(2):826--873, 2002

  50. [58]

    Anomalous dissipation via spontaneous stochasticity with a two-dimensional autonomous velocity field, 2024

    Carl Johan Peter Johansson and Massimo Sorella. Anomalous dissipation via spontaneous stochasticity with a two-dimensional autonomous velocity field, 2024. arXiv:2409.03599

  51. [59]

    Dissipation of energy in locally isotropic turbulence

    Andrei Nikolaevich Kolmogorov. Dissipation of energy in locally isotropic turbulence. Akademiia Nauk SSSR Doklady , 32:16, 1941

  52. [60]

    The local structure of turbulence in incompressible viscous fluid for very large Reynolds ' numbers

    Andrei Nikolaevich Kolmogorov. The local structure of turbulence in incompressible viscous fluid for very large Reynolds ' numbers. Akademiia Nauk SSSR Doklady , 30:301--305, 1941

  53. [61]

    On the degeneration of isotropic turbulence in an incompressible viscous fluid

    Andrej Nikolaevich Kolmogorov. On the degeneration of isotropic turbulence in an incompressible viscous fluid. Dokl. Akad. Nauk SSSR , 31(6):319--323, 1941

  54. [62]

    Kraichnan

    Robert H. Kraichnan. Small‐ Scale Structure of a Scalar Field Convected by Turbulence . The Physics of Fluids , 11(5):945--953, 1968

  55. [63]

    Edward N. Lorenz. The predictability of a flow which possesses many scales of motion. Tellus A: Dynamic Meteorology and Oceanography , 21(3), January 1969

  56. [64]

    Mailybaev

    Alexei A. Mailybaev. Spontaneous stochasticity of velocity in turbulence models. Multiscale Model. Simul. , 14(1):96--112, 2016

  57. [65]

    Mailybaev

    Alexei A. Mailybaev. Spontaneously stochastic solutions in one-dimensional inviscid systems. Nonlinearity , 29(8):2238--2252, 2016

  58. [66]

    Miles and Charles R

    Christopher J. Miles and Charles R. Doering. Diffusion-limited mixing by incompressible flows. Nonlinearity , 31(5):2346, 2018

  59. [67]

    Joe Myers Hill, Rob Sturman, and Mark C. T. Wilson. Exponential mixing by orthogonal non-monotonic shears. Physica D: Nonlinear Phenomena , 434:133224, 2022

  60. [68]

    Continuity of Solutions of Parabolic and Elliptic Equations

    John Nash. Continuity of Solutions of Parabolic and Elliptic Equations . American Journal of Mathematics , 80(4):931--954, 1958

  61. [69]

    Exponential mixing by random cellular flows, February 2025

    Víctor Navarro-Fernández and Christian Seis. Exponential mixing by random cellular flows, February 2025. arXiv:2502.17273 [math]

  62. [70]

    An intermittent O nsager theorem

    Matthew Novack and Vlad Vicol. An intermittent O nsager theorem. Invent. Math. , 233(1):223--323, 2023

  63. [71]

    Alexander M. Obukhov. Structure of Temperature Field in Turbulent Flow . Izv. Akad. Nauk. SSSR, Ser. Geogr. i Geofiz. , 13:58--69, 1949

  64. [72]

    Atmospheric diffusion shown on a distance-neighbour graph

    Lewis Fry Richardson. Atmospheric diffusion shown on a distance-neighbour graph. Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character , 110(756):709--737, 1926

  65. [73]

    Accelerated relaxation enhancing flows cause total dissipation

    Keefer Rowan. Accelerated relaxation enhancing flows cause total dissipation. Nonlinearity , 37(9):095010, 2024

  66. [74]

    On anomalous diffusion in the K raichnan model and correlated-in-time variants

    Keefer Rowan. On anomalous diffusion in the K raichnan model and correlated-in-time variants. Archive for Rational Mechanics and Analysis , 248(5):93, 2024

  67. [75]

    Theory of function spaces , volume 78 of Monographs in Mathematics

    Hans Triebel. Theory of function spaces , volume 78 of Monographs in Mathematics . Birkh\"auser Verlag, Basel, 1983

  68. [76]

    Enhanced dissipation via the M alliavin calculus

    David Villringer. Enhanced dissipation via the M alliavin calculus. Electron. Commun. Probab. , 30:Paper No. 26, 11, 2025

Pith tools

Reviewed August 6, 2026 · model on record in the stance chip above.