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The journal Asymptotic Analysis fulfills a twofold function. It aims at publishing original mathematical results in the asymptotic theory of problems affected by the presence of small or large parameters on the one hand, and at giving specific indications of their possible applications to different fields of natural sciences on the other hand.
Asymptotic Analysis thus provides mathematicians with a concentrated source of newly acquired information which they may need in the analysis of asymptotic problems.
Authors: Iftimie, Dragoş
Article Type: Research Article
Abstract: In this paper we show that the quasigeostrophic system is well approximated by the primitive systems. More precisely, we prove that if the initial data are weakly well‐prepared then the maximal time existence of the regular solution of the primitive system goes to infinity and the regular solution goes to the solution of the quasigeostrophic system, strongly on an arbitrary time interval. By weakly well‐prepared initial data we mean that the initial data of the primitive systems is converging to an initial data with zero oscillating part, without any assumptions on the speed.
Citation: Asymptotic Analysis, vol. 21, no. 2, pp. 89-97, 1999
Authors: Cerqueti, Katiuscia
Article Type: Research Article
Abstract: We consider the problem \cases{ - \Delta u = N(N-2) u^p +\varepsilon u & \mbox{in} $\varOmega$,\cr u >0 & \mbox{in} $\varOmega$,\cr u =0 & \mbox{on} $\curpartial\varOmega$,\cr} where \varOmega is a bounded smooth domain of \mathbf{R}^N \ (N \geq 5) which is symmetric with respect to the coordinate hyperplanes \{x_i = 0\} , i = 1, \ldots, N , and it is convex in the x_i ‐directions for i = 1, \ldots, N ; here 0 < \varepsilon < \lambda_1 (\lambda_1 …being the first eigenvalue of the Laplace operator in H_0^1 (\varOmega) ) and p = ({N+2})/({N-2}) . For \varepsilon small, we prove uniqueness and nondegeneracy of the solution u_\varepsilon with the property that \lim_{\varepsilon \rightarrow0} \frac{\int_\varOmega|\nabla u_\varepsilon|^2 \,\mathrm{d} x }{ (\int_\varOmega|u_\varepsilon|^{p+1}\,\mathrm{d} x)^{2/p+1} } = S_N, where S_N is the best Sobolev constant in \mathbf{R}^N . Show more
Citation: Asymptotic Analysis, vol. 21, no. 2, pp. 99-115, 1999
Authors: Bayada, Guy | Chambat, Michèle | Ciuperca, Ionel
Article Type: Research Article
Abstract: We consider a fluid flow in a thin domain with moving boundary. Using a rescaling of the domain in time and in height, we obtain the generalized Reynolds equation for the limit pressure.
Citation: Asymptotic Analysis, vol. 21, no. 2, pp. 117-132, 1999
Authors: Hayashi, Nakao | Miao, Changxing | Naumkin, Pavel I.
Article Type: Research Article
Abstract: We study the global in time existence of small solutions to the generalized derivative nonlinear Schrödinger equations of the form \begin{equation} \cases {\mathrm{i}\curpartial_t u + (1/2)\Delta u = \mathcal{N}(u,\nabla u,\overline u,\nabla \overline u), &$(t,x) \in \mathbf{R}\times {\mathbf{R}}^n$,\cr \noalign{\vskip4pt} u(0,x) = u_0 (x),\quad x\in\mathbf{R}^n,\cr} \end{equation} where the space dimension n \geqslant 3 , the initial data u_0 are sufficiently small, \bar u is the complex conjugate of u and the nonlinear term \mathcal{N} is a smooth complex valued function \mathbf{C}\times \mathbf{C}^n\times \mathbf{C}\times …\mathbf{C}^n\rightarrow \mathbf{C} . We assume that {\mathcal N} is a quadratic function in the neighborhood of the origin and always includes at least one derivative, that is, |{\mathcal N}(u,w,\bar u,\bar w)| \leqslant C|w|(|u|+|w|) , for small u and w in the case of space dimensions n = 3, 4 . As a typical example we consider the case of the polynomial type nonlinearity of the form {\mathcal N}(u,w,\bar u,\bar w) = \sum_{\tiny{\matrix{2 \leqslant |\alpha| + |\beta| + |\gamma| \leqslant l\cr \noalign{\vskip2pt} m \leqslant |\beta| + |\gamma| \leqslant l}}} \normalsize\lambda_{\alpha\beta\gamma} u^{\alpha_1}\bar u^{\alpha_2} w^{\beta}\bar w^{\gamma} with w = (w_j)_{1\leqslant j\leqslant n} , \lambda_{\alpha\beta\gamma} \in \mathbf{C} , l\geqslant 2, m \geqslant 1 for n=3,4 , and m \geqslant 0 for n\geqslant 5 . We prove the global existence of solutions to the Cauchy problem (A) under the condition that the initial data u_0 \in \mathbf{H}^{[n/2]+5,0} \cap \mathbf{H}^{[n/2]+3,2} , where \mathbf{H}^{m,s} = \{ \phi \in \mathbf{L}^2;\ \|\phi\|_{m,s} = \|(1+x^2)^{s/2} (1-\Delta)^{m/2}\phi\|_{\mathbf{L}^2} <\infty\} is the weighted Sobolev space. We also show the existence of the usual scattering states. Our result for n=3,4 is an improvement of Hayashi and Hirata, Nonlinear Anal. 31 (1998), 671–685. Show more
Keywords: Derivative nonlinear Schrödinger equations, global small solutions, general space dimensions
Citation: Asymptotic Analysis, vol. 21, no. 2, pp. 133-147, 1999
Authors: Bambusi, Dario | Graffi, Sandro | Paul, Thierry
Article Type: Research Article
Abstract: Let \mathcal{H} be a holomorphic Hamiltonian of quadratic growth on \mathbb{R}^{2n} , b a holomorphic exponentially localized observable, H,B the corresponding operators on L^2(\mathbb{R}^n) generated by Weyl quantization, and U(t)=\exp{\mathrm{i}Ht/\hbar} . It is proved that the L^2 norm of the difference between the Heisenberg observable B_t=U(t)BU(-t) and its semiclassical approximation of order N-1 is majorized by K^N N^{(6n+1)N}\hbar^{-4/9}(-\hbar\log\hbar)^N for t\in [0,T_n(\hbar)] , where T_n(\hbar):=-2\log\hbar/[\alpha(6n+3)(N-1)] and \alpha:=\Vert\mathrm{Hess}_{(x,\xi)}\,\mathcal{H}\Vert . Choosing a suitable N(\hbar) the error is majorized by …C\hbar^{\log\vert\log\hbar\vert} , 0\leq t\leq \vert\log\hbar\vert/\log\vert\log\hbar\vert (here K and C are explicit constants independent of N,\hbar ). Show more
Citation: Asymptotic Analysis, vol. 21, no. 2, pp. 149-160, 1999
Authors: El Hajji, Mohamed | Donato, Patrizia
Article Type: Research Article
Abstract: In Nonlinear Partial Differential Equations and Their Applications, Vol. 13 (to appear), Briane, Damlamian and Donato extend to the case of perforated domains the H ‐covergence introduced by Murat and Tartar (Sém. Anal. Fonct. Numér., 1977/1978; Topics in the Mathematical Modelling of Composite Materials, 1997) for the diffusion equation. In this paper, we define in the same spirit a notion of H^0 ‐convergence for the linearized elasticity system in perforated domains. This definition allows to obtain compactness, locality and corrector results.
Keywords: Homogenization, elasticity, H‐convergence, H^0‐convergence
Citation: Asymptotic Analysis, vol. 21, no. 2, pp. 161-186, 1999
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