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The move from Fujita type exponent to a shift of it for a class of semilinear evolution equations with time-dependent damping

  • Marcelo Rempel Ebert,
  • Jorge Marques,
  • Wanderley Nunes do Nascimento

摘要

In this paper, we derive suitable optimal \(L^p-L^q\) L p - L q decay estimates, \(1\le p\le 2\le q\le \infty \) 1 p 2 q , for the solutions to the \(\sigma \) σ -evolution equation, \(\sigma >1\) σ > 1 , with scale-invariant time-dependent damping and power nonlinearity  \(|u|^p\) | u | p , \(\begin{aligned} u_{tt}+(-\Delta )^\sigma u + \frac{\mu }{1+t} u_t= |u|^{p}, \quad t\ge 0, \quad x\in {{\mathbb {R}}}^n, \end{aligned}\) u tt + ( - Δ ) σ u + μ 1 + t u t = | u | p , t 0 , x R n , where  \(\mu >0\) μ > 0 ,   \(p>1\) p > 1 . The critical exponent \(p=p_c\) p = p c for the global (in time) existence of small data solutions to the Cauchy problem is related to the long time behavior of solutions, which changes accordingly \(\mu \in (0, 1)\) μ ( 0 , 1 ) or \(\mu >1\) μ > 1 . Under the assumption of small initial data in \(L^m({{\mathbb {R}}}^n)\cap L^2({{\mathbb {R}}}^n), m=1,2\) L m ( R n ) L 2 ( R n ) , m = 1 , 2 , we find the critical exponent at low space dimension n with respect to \(\sigma \) σ , namely, \(\begin{aligned} p_c= \max \left\{ {{\bar{p}}}(\gamma _{m}), {{\bar{p}}} (\gamma _{m}+\mu -1) \right\} , \quad \gamma _{m}{\mathrm {\,:=\,}}\frac{n}{m\sigma }, \quad \mu >1-\gamma _m, \end{aligned}\) p c = max p ¯ ( γ m ) , p ¯ ( γ m + μ - 1 ) , γ m : = n m σ , μ > 1 - γ m , where \( {{\bar{p}}}(\gamma ){\mathrm {\,:=\,}}1+ \frac{2}{\gamma }\) p ¯ ( γ ) : = 1 + 2 γ is the well known Fujita exponent. Hence, \(p_c={{\bar{p}}}(\gamma _{m})\) p c = p ¯ ( γ m ) if \(\mu >1\) μ > 1 , whereas \(p_c={{\bar{p}}} (\gamma _{m}+\mu -1)\) p c = p ¯ ( γ m + μ - 1 ) is a shift of Fujita type exponent if \(\mu \in (0, 1)\) μ ( 0 , 1 ) .