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Proceedings of the American Mathematical Society

Published by the American Mathematical Society since 1950, Proceedings of the American Mathematical Society is devoted to shorter research articles in all areas of pure and applied mathematics.

ISSN 1088-6826 (online) ISSN 0002-9939 (print)

The 2020 MCQ for Proceedings of the American Mathematical Society is 0.85.

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Global well-posedness for the semilinear wave equation with time dependent damping in the overdamping case
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by Masahiro Ikeda and Yuta Wakasugi PDF
Proc. Amer. Math. Soc. 148 (2020), 157-172 Request permission

Abstract:

We study the global existence of solutions to the Cauchy problem for the wave equation with time-dependent damping and a power nonlinearity in the overdamping case: \begin{align*}\left \{\begin {array}{ll} u_{tt} - \Delta u + b(t) u_t = N(u),&t\in [0,T),\ x\in \mathbb {R}^d,\\ u(0) = u_0,\ u_t(0) = u_1,&x\in \mathbb {R}^d. \end{array}\right . \end{align*} Here, $b(t)$ is a positive $C^1$-function on $[0,\infty )$ satisfying \[ b(t)^{-1} \in L^1(0,\infty ), \]whose case is called overdamping. $N(u)$ denotes the $p$th order power nonlinearities. It is well known that the problem is locally well-posed in the energy space $H^1(\mathbb {R}^d)\times L^2(\mathbb {R}^d)$ in the energy-subcritical or energy-critical case $1\le p\le p_1$, where $p_1:=1+\frac {4}{d-2}$ if $d\ge 3$ or $p_1=\infty$ if $d=1,2$. It is known that when $N(u):=\pm |u|^p$, small data blow-up in $L^1$-framework occurs in the case $b(t)^{-1} \notin L^1(0,\infty )$ and $1<p<p_c(< p_1)$, where $p_c$ is a critical exponent, i.e., threshold exponent dividing the small data global existence and the small data blow-up. The main purpose in the present paper is to prove the global well-posedness to the problem for small data $(u_0,u_1)\in H^1(\mathbb {R}^d)\times L^2(\mathbb {R}^d)$ in the whole energy-subcritical case, i.e., $1\le p<p_1$. This result implies that the small data blow-up does not occur in the overdamping case, different from the other case $b(t)^{-1}\notin L^1(0,\infty )$, i.e., the effective or noneffective damping.
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Additional Information
  • Masahiro Ikeda
  • Affiliation: Department of Mathematics, Faculty of Science and Technology, Keio University, 3-14-1 Hiyoshi, Kohoku-ku, Yokohama, 223-8522, Japan – and – Center for Advanced Intelligence Project, RIKEN, Japan
  • MR Author ID: 940764
  • Email: masahiro.ikeda@keio.jp/masahiro.ikeda@riken.jp
  • Yuta Wakasugi
  • Affiliation: Department of Engineering for Production and Environment, Graduate School of Science and Engineering, Ehime University, 3 Bunkyo-cho, Matsuyama, Ehime, 790-8577, Japan
  • MR Author ID: 954066
  • Email: wakasugi.yuta.vi@ehime-u.ac.jp
  • Received by editor(s): August 26, 2017
  • Received by editor(s) in revised form: April 24, 2018, and June 8, 2018
  • Published electronically: September 25, 2019
  • Additional Notes: This work was supported by Grant-in-Aid for JSPS Fellows 26$\cdot$1884 and Grant-in-Aid for Young Scientists (B) 15K17571 and 16K17625.
  • Communicated by: Joachim Krieger
  • © Copyright 2019 American Mathematical Society
  • Journal: Proc. Amer. Math. Soc. 148 (2020), 157-172
  • MSC (2010): Primary 35L71, 35L15, 35A01
  • DOI: https://doi.org/10.1090/proc/14297
  • MathSciNet review: 4042839