SearcharxivSearch

arXiv subjects

Halit Sevki Aslan

Publications and source records attributed to Halit Sevki Aslan.

6 recordsLinked to original sources

Dispersive estimates for wave-type equations with time-dependent damping

In this paper, we study the Cauchy problem for a class of semilinear evolution equations with scale-invariant time-dependent dissipation \begin{equation*} \begin{cases} u_{tt} + L_{w^2}u + \dfracμ{1+t}u_t = Δ^θ f(u), & t>0,\ x\in\mathbb{R}^n,\\ u(0,x) = 0,\qquad u_t(0,x) = u_1(x), & x\in\mathbb{R}^n, \end{cases} \end{equation*} where $μ>0$, $f(u)=|u|^α$ with $α>1$, $θ\in\{0,1\}$, and the operator $L_{w^2}$ is defined on the Fourier transform by multiplication by $w(ξ)^2$. We prove the global (in time) existence of small data solutions for $α>α_{\mathrm{crit}}$, where the critical exponent $α_{\mathrm{crit}}$ depends on the choice of the operator $L_{w^2}$, the parameter $μ$, and the nonlinear term. In particular, we consider two model cases. For Boussinesq-type operators with $w(ξ)=\sqrt{|ξ|^2+|ξ|^4}$, combined with the derivative-type nonlinearity $Δ|u|^α$, we obtain a Strauss-type critical exponent. On the other hand, for plate-type operators with $w(ξ)=|ξ|^σ$, $σ\geq2$, and power-type nonlinearity $|u|^α$, the critical exponent is of Fujita type.

math.AP

Evolution models with time-dependent coefficients in friction and viscoelastic damping terms

We study the following Cauchy problem for the linear wave equation with both time-dependent friction and time-dependent viscoelastic damping: \begin{equation} \label{EqAbstract}\tag{$\ast$} \begin{cases} u_{tt}- Δu + b(t)u_t - g(t)Δu_t=0, &(t,x) \in (0,\infty) \times \mathbb{R}^n, \\ u(0,x)= u_0(x),\quad u_t(0,x)= u_1(x), &x \in \mathbb{R}^n. \end{cases} \end{equation} Our goal is to derive decay estimates for higher order energy norms of solutions to this problem. We focus on the interplay between the time-dependent coefficients in both damping terms and their influence on the qualitative behavior of solutions. The analysis is based on a classification of the damping mechanisms, frictional damping $b(t)u_t$ and viscoelastic damping $-g(t)Δu_t$ as well, and employs the WKB-method in the extended phase space.

math.AP

On the Cauchy problem for semilinear thermoelastic plate systems in the $L^q$ framework

We mainly consider semilinear thermoelastic plate systems with general power nonlinearities in the whole space $\mathbb{R}^n$. By applying the Fourier analysis, some sharp $(L^q\cap L^m)-L^q$ estimates of solutions (with any $1\leqslant m\leqslant q\leqslant +\infty$) to the classical thermoelastic plate system are derived, which cover all known results in $\mathbb{R}^n$. Then, we investigate global in time existence of small data $L^q$ solutions (with any $q\in[1,+\infty]$) and blow-up of weak solutions for the semilinear thermoelastic plate systems under suitable conditions on the power exponents, which justify critical exponents for several classes of nonlinearities.

math.AP

$L^p-L^q$ estimates for solutions to the plate equation with mass term

In this paper, we study the Cauchy problem for the linear plate equation with mass term and its applications to semilinear models. For the linear problem we obtain $L^p-L^q$ estimates for the solutions in the full range $1\leq p\leq q\leq \infty$, and we show that such estimates are optimal. In the sequel, we discuss the global in time existence of solutions to the associated semilinear problem with power nonlinearity $|u|^α$. For low dimension space $n\leq 4$, and assuming $L^1$ regularity on the second datum, we were able to prove global existence for $α> \max\{α_c(n), \tildeα_c(n)\}$ where $α_c = 1+4/n$ and $\tilde α_c = 2+2/n$. However, assuming initial data in $H^2(\mathbb{R}^n)\times L^2(\mathbb{R}^n)$, the presence of the mass term allows us to obtain global in time existence for all $1<α\leq (n+4)/[n-4]_+$. We also show that the latter upper bound is optimal, since we prove that there exist data such that a non-existence result for local weak solutions holds when $α> (n+4)/[n-4]_+$.

math.AP

Visco-elastic damped wave models with time-dependent coefficient

In this paper, we study the following Cauchy problem for linear visco-elastic damped wave models with a general time-dependent coefficient $g=g(t)$: \begin{equation} \label{EqAbstract} \tag{$\star$} \begin{cases} u_{tt}- Δu + g(t)(-Δ)u_t=0, &(t,x) \in (0,\infty) \times \mathbb{R}^n, \\ u(0,x)= u_0(x),\quad u_t(0,x)= u_1(x), &x \in \mathbb{R}^n. \end{cases} \end{equation} We are interested to study the influence of the damping term $g(t)(-Δ)u_t$ on qualitative properties of solutions to \eqref{EqAbstract} as decay estimates for energies of higher order and the parabolic effect. The main tools are related to WKB-analysis. We apply elliptic as well as hyperbolic WKB-analysis in different parts of the extended phase space.

math.AP

The influence of oscillations on energy estimates for damped wave models with time-dependent propagation speed and dissipation

The aim of this paper is to derive higher order energy estimates for solutions to the Cauchy problem for damped wave models with time-dependent propagation speed and dissipation. The model of interest is \begin{equation*} u_{tt}-λ^2(t)ω^2(t)Δu +ρ(t)ω(t)u_t=0, \quad u(0,x)=u_0(x), \,\, u_t(0,x)=u_1(x). \end{equation*} The coefficients $λ=λ(t)$ and $ρ=ρ(t)$ are shape functions and $ω=ω(t)$ is an oscillating function. If $ω(t)\equiv1$ and $ρ(t)u_t$ is an "effective" dissipation term, then $L^2-L^2$ energy estimates are proved in [2]. In contrast, the main goal of the present paper is to generalize the previous results to coefficients including an oscillating function in the time-dependent coefficients. We will explain how the interplay between the shape functions and oscillating behavior of the coefficient will influence energy estimates.

math.AP