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Haina Li

Publications and source records attributed to Haina Li.

5 recordsLinked to original sources
arXiv2026

Failure of analyticity-radius growth in energy-canceling fluid models

We prove that exact quadratic energy cancellation alone does not force growth of the spatial analyticity radius. On $\mathbb{T}^3$, we construct an explicit symmetric, translation-invariant, first-order bilinear operator $Q$ that preserves the divergence-free class and, for every smooth real-valued divergence-free vector field $v$, satisfies $ \int_{\mathbb{T}^3} Q(v,v)\cdot v\,dx=0.$ For every prescribed sufficiently small time $T>0$, the equation $\partial_t u-\Delta u=Q(u,u)$ admits a global smooth, real-valued, mean-zero, divergence-free solution $u$ such that $\operatorname{rad}(u(0))=\operatorname{rad}(u(T))=1$. The construction reduces the dynamics on an invariant cyclic-shear class to viscous Burgers and tunes a Cole-Hopf heat profile so that its nearest complex zero returns to its initial distance from the real torus. For every $1<\alpha<2$ and every prescribed sufficiently small $T>0$, we also construct a symmetric sparse frequency set, its associated Fourier projection, and trigonometric-polynomial initial data for the projected dissipative surface quasi-geostrophic equation. The resulting unique global smooth solution $\theta$ has infinite analyticity radius initially but satisfies $0<\operatorname{rad}(\theta(T))\leq1$. An additively separated Fourier cascade yields coefficientwise exponential lower bounds, while uniform comparison estimates control the feedback interactions. Thus entire analyticity need not persist even from trigonometric-polynomial data. Together, the two constructions show that an exact energy identity alone does not determine the frequency geometry governing analyticity-radius growth.

math.AP↗
arXiv2025

Global smooth solutions to Navier-Stokes equations with large initial data in critical space

In this paper, we investigate the existence of a unique global smooth solution to the three-dimensional incompressible Navier-Stokes equations and provide a concise proof. We establish a new global well-posedness result that allows the initial data to be arbitrarily large within the critical space $\dot{B}^{-1}_{\infty,\infty}$, while still satisfying the nonlinear smallness condition.

math.AP↗
arXiv2024

New Regularity Criteria for Navier-Stokes and SQG Equations in Critical Spaces

In this paper, we investigate some priori estimates to provide the critical regularity criteria for incompressible Navier-Stokes equations on $\mathbb{R}^3$ and super critical surface quasi-geostrophic equations on $\mathbb{R}^2$. Concerning the Navier-Stokes equation, we demonstrate that a Leray-Hopf solution $u$ is regular if $u\in L_T^{\frac{2}{1-\alpha}} \dot{B}^{-\alpha}_{\infty,\infty}(\mathbb{R}^3)$, or $u$ in Lorentz space $ L_T^{p,r} \dot{B}^{-1+\frac{2}{p}}_{\infty,\infty}(\mathbb{R}^3)$, with $4\leq p\leq r<\infty$. Additionally, an alternative regularity condition is expressed as $u\in L_{T}^{\frac{2}{1-\alpha}} \dot{B}^{-\alpha}_{\infty,\infty}(\mathbb{R}^3)+{L_T^\infty\dot{B}^{-1}_{\infty,\infty}}(\mathbb{R}^3)$($\alpha\in(0,1)$), contingent upon a smallness assumption on the norm $L_T^\infty\dot{B}^{-1}_{\infty,\infty}$. For the SQG equation, we derive that a Leray-Hopf weak solution $\theta\in L_T^{\frac{\alpha}{\varepsilon}} \dot{C}^{1-\alpha+\epsilon}(\mathbb{R}^2)$ is smooth for any $\varepsilon$ small enough. Similar to the case of Navier-Stokes equation, we derive regularity criterion in more refined spaces, i.e. Lorentz spaces $L_T^{\frac{\alpha}{\epsilon},r}\dot{C}^{1-\alpha+\epsilon}(\mathbb{R}^2)$ and addition of two critical spaces $L_{T}^{\frac{\alpha}{\epsilon}}\dot{C}^{1-\alpha+\epsilon}(\mathbb{R}^2)+{L_T^\infty\dot{C}^{1-\alpha}(\mathbb{R}^2)}$, with smallness assumption on $L_T^\infty\dot{C}^{1-\alpha}(\mathbb{R}^2)$.

math.AP↗