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Norm Growth, Non-uniqueness, and Anomalous Dissipation in Passive Scalars

Tarek M. Elgindi, Kyle Liss

TL;DR

The paper constructs a divergence-free velocity field on the torus with near-Lipschitz spatial regularity that induces anomalous dissipation for the advection-diffusion equation for every smooth initial data. The approach reduces anomalous dissipation to an $H^1$-growth mechanism for the transport equation, implemented via a carefully designed sequence of alternating shear maps and a forward-backward growth argument, complemented by a balanced-growth upper bound. It also shows that, with a modification of the velocity field, one can obtain scalar regularity bounds approaching the Obukhov-Corrsin threshold, linking dissipation anomalies to turbulence-style scaling. The study situates these constructions among prior works on anomalous dissipation and non-uniqueness, discusses potential extensions to autonomous flows and higher dimensions, and poses open questions about regularity thresholds and forward-backward dynamics in this context.

Abstract

We construct a divergence-free velocity field $u:[0,T] \times \mathbb{T}^2 \to \mathbb{R}^2$ satisfying $$u \in C^\infty([0,T];C^α(\mathbb{T}^2)) \quad \forall α\in [0,1)$$ such that the corresponding drift-diffusion equation exhibits anomalous dissipation for every smooth initial data. We also show that, given any $α_0 < 1$, the flow can be modified such that it is uniformly bounded only in $C^{α_0}(\mathbb{T}^2)$ and the regularity of solutions satisfy sharp (time-integrated) bounds predicted by the Obukhov-Corrsin theory. The proof is based on a general principle implying $H^1$ growth for all solutions to the transport equation, which may be of independent interest.

Norm Growth, Non-uniqueness, and Anomalous Dissipation in Passive Scalars

TL;DR

The paper constructs a divergence-free velocity field on the torus with near-Lipschitz spatial regularity that induces anomalous dissipation for the advection-diffusion equation for every smooth initial data. The approach reduces anomalous dissipation to an -growth mechanism for the transport equation, implemented via a carefully designed sequence of alternating shear maps and a forward-backward growth argument, complemented by a balanced-growth upper bound. It also shows that, with a modification of the velocity field, one can obtain scalar regularity bounds approaching the Obukhov-Corrsin threshold, linking dissipation anomalies to turbulence-style scaling. The study situates these constructions among prior works on anomalous dissipation and non-uniqueness, discusses potential extensions to autonomous flows and higher dimensions, and poses open questions about regularity thresholds and forward-backward dynamics in this context.

Abstract

We construct a divergence-free velocity field satisfying such that the corresponding drift-diffusion equation exhibits anomalous dissipation for every smooth initial data. We also show that, given any , the flow can be modified such that it is uniformly bounded only in and the regularity of solutions satisfy sharp (time-integrated) bounds predicted by the Obukhov-Corrsin theory. The proof is based on a general principle implying growth for all solutions to the transport equation, which may be of independent interest.
Paper Structure (24 sections, 12 theorems, 117 equations, 1 figure)

This paper contains 24 sections, 12 theorems, 117 equations, 1 figure.

Key Result

Theorem 1

Fix $T > 0$. There exists a divergence-free velocity field $u:[0,T] \times \mathbb{T}^2 \to \mathbb{R}^2$ with such that, for every mean-zero and smooth initial data $f_0,$ the solutions $f^\kappa$ exhibit anomalous dissipation on $[0,T]$. Solutions to the corresponding transport equation are non-unique while $u$ satisfies for all $t\in [0,T]$ and $z,z'\in\mathbb{T}^2$, with $\omega(s)=s(1+|\log

Figures (1)

  • Figure 1: Numerical simulation of the transport equation \ref{['eq:AE']} with $u$ a regularized version of the alternating shear flow used in the proof of Theorem \ref{['thrm:main']} and initial condition $f_0(x,y) = \sin(x)$, displayed in the upper left image. Moving from left to right, the scalar is shown after each successive shearing direction is applied.

Theorems & Definitions (26)

  • Theorem 1
  • Remark 1.1
  • Remark 1.2
  • Remark 1.3
  • Remark 1.4
  • Theorem 2
  • Lemma 1.1
  • Proposition 2.1
  • Lemma 2.2: $H^1$ growth
  • Lemma 2.3
  • ...and 16 more