Abstract

Abstract In this paper, we study the fractional p-Laplacian evolution equation with arbitrary initial energy, $$\begin{array}{} \displaystyle u_t(x,t) + (-{\it\Delta})_p^s u(x,t) = f(u(x,t)), \quad x\in {\it\Omega}, \,t \gt 0, \end{array} $$ where $\begin{array}{} (-{\it\Delta})_p^s \end{array} $ is the fractional p-Laplacian with $\begin{array}{} p \gt \max\{\frac{2N}{N+2s},1\} \end{array} $ and s ∈ (0, 1). Specifically, by the modified potential well method, we obtain the global existence, uniqueness, and blow-up in finite time of the weak solution for the low, critical and high initial energy cases respectively.

Highlights

  • Let Ω ⊂ RN (N) be a bounded domain with smooth boundary, T ∈(, ∞], p N N+ s} and s ∈ (, )

  • In this paper, we study the fractional p-Laplacian evolution equation with arbitrary initial energy, ut(x, t) + (−∆)sp u(x, t) = f (u(x, t)), x ∈ Ω, t >, where

  • We study the following fractional p-Laplacian evolution equation with the zero

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Summary

Introduction

When p ≠ , Gal and Warm [8] studied the existence of the strong solution and the blow-up for the initial data with nite energy and a positive low bound. Authors did not study the problem for J(u ) > d and blow-up in nite time for arbitrary initial energy. We consider the global existence and blow-up in nite time for the problem (1.1) for the more general f (u) when the initial energy J(u ) is arbitrary. In this paper, motivated by the works mentioned above, we consider the global existence, uniqueness and blow-up property of problem (1.1) with arbitrary initial energy J(u ). The following theorem indicates that there exists blow-up solutions to problem (1.1) for any high initial energy.

Functional Space and Preliminaries
RN RN
Preliminaries of potential well
Therefore d
De ne
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