arXivDaily arXiv每日学术速递 周一至周五更新
arXiv周末暂无论文更新,休息一下吧,周末愉快~~
arXiv 2309.03429math.AP
收藏

对偶分数阶抛物型方程的 Liouville 定理与径向对称性

A Liouville Theorem and Radial Symmetry for dual fractional parabolic equations

Yahong Guo, Lingwei Ma, Zhenqiu Zhang

AI总结:

本文研究对偶分数阶抛物型方程,证明了正有界解的径向对称性,并通过引入新扰动技术建立了全空间齐次方程及Marchaud分数阶方程的Liouville定理。

摘要:

在本文中,我们首先研究对偶分数阶抛物型方程 \partial^α_t u(x,t)+(-Δ)^s u(x,t) = f(u(x,t)) in B_1(0)×R,该方程受限于外部消失条件。我们证明,对于每个 t∈R,正有界解 u(·,t) 在 R^n 的单位球内必须关于原点径向对称且严格递减。为了克服由算子 ∂^α_t+(-Δ)^s 的双重非局部性带来的挑战,引入了一些新颖的技术。然后,我们在全空间中建立齐次方程 ∂^α_t u(x,t)+(-Δ)^s u(x,t) = 0 in R^n×R 的 Liouville 定理。我们首先证明无界域中反对称函数的极值原理,从而推导出 u(x,t) 关于 x 必须是常数。接着,我们只需建立 Marchaud 分数阶方程 ∂^α_t u(t) = 0 in R 的 Liouville 定理。为了规避由算子 ∂^α_t 的非局部和单边性质引起的困难,我们引入了一些新思路和更简单的方法。我们不再扰动反对称函数,而是直接在解 u(t) 本身采用扰动技术。该方法为建立单边算子 ∂^α_t(包括更一般的 Marchaud 时间导数)的 Liouville 定理提供了一条更简洁直观的途径。

英文摘要:

In this paper, we first study the dual fractional parabolic equation \begin{equation*} \partial^α_t u(x,t)+(-Δ)^s u(x,t) = f(u(x,t))\ \ \mbox{in}\ \ B_1(0)\times\R , \end{equation*} subject to the vanishing exterior condition. We show that for each $t\in\R$, the positive bounded solution $u(\cdot,t)$ must be radially symmetric and strictly decreasing about the origin in the unit ball in $\R^n$. To overcome the challenges caused by the dual non-locality of the operator $\partial^α_t+(-Δ)^s$, some novel techniques were introduced. Then we establish the Liouville theorem for the homogeneous equation in the whole space \begin{equation*}\label{B} \partial^α_t u(x,t)+(-Δ)^s u(x,t) = 0\ \ \mbox{in}\ \ \R^n\times\R . \end{equation*} We first prove a maximum principle in unbounded domains for anti-symmetric functions to deduce that $u(x,t)$ must be constant with respect to $x.$ Then it suffices for us to establish the Liouville theorem for the Marchaud fractional equation \begin{equation*} \partial^α_t u(t) = 0\ \ \mbox{in}\ \ \R . \end{equation*} To circumvent the difficulties arising from the nonlocal and one-sided nature of the operator $\partial_t^α$, we bring in some new ideas and simpler approaches. Instead of disturbing the anti-symmetric function, we employ a perturbation technique directly on the solution $u(t)$ itself. This method provides a more concise and intuitive route to establish the Liouville theorem for one-sided operators $\partial_t^α$, including even more general Marchaud time derivatives.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑