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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: Montefusco, Eugenio | Pellacci, Benedetta | Squassina, Marco
Article Type: Research Article
Abstract: The semiclassical limit of a weakly coupled nonlinear focusing Schrödinger system in presence of a nonconstant potential is studied. The initial data is of the form (u1 , u2 ) with ui =ri ((x−x˜)/ε)e(i/ε)x·ξ˜ , where (r1 , r2 ) is a real ground state solution, belonging to a suitable class, of an associated autonomous elliptic system. For ε sufficiently small, the solution (ϕ1 , ϕ2 ) will been shown to have, locally in time, the form (r1 ((x−x(t))/ε)e(i/ε)x·ξ(t) , r2 ((x−x(t))/ε)e(i/ε)x·ξ(t) ), where (x(t), ξ(t)) is the solution of the Hamiltonian system x˙(t)=ξ(t), ξ˙(t)=−∇V(x(t)) with x(0)=x˜ …and ξ(0)=ξ˜. Show more
Keywords: weakly coupled nonlinear Schrödinger systems, concentration phenomena, semiclassical limit, orbital stability of ground states, soliton dynamics
DOI: 10.3233/ASY-2009-0959
Citation: Asymptotic Analysis, vol. 66, no. 2, pp. 61-86, 2010
Authors: Pompe, Waldemar
Article Type: Research Article
Abstract: We prove existence of a solution to the nonautonomous, noncoercive, quasistatic models in the viscoplasticity theory. This extends the results shown earlier by the author in Math. Methods Appl. Sci. 27 (2004), 1347–1365 and Math. Methods Appl. Sci. 31 (2008), 775–792, for the autonomous case. As a special case we obtain existence of the solution to the nonautonomous kinematic hardening model, where the constitutive nonlinearity has a polynomial or a rapid growth at infinity.
Keywords: viscoplasticity models, Orlicz spaces, semigroups of contractions
DOI: 10.3233/ASY-2009-0960
Citation: Asymptotic Analysis, vol. 66, no. 2, pp. 87-102, 2010
Authors: Alfaro, Manuel | Peña, Ana | Rezola, M. Luisa | Moreno-Balcázar, Juan José
Article Type: Research Article
Abstract: We consider a generalization of the classical Hermite polynomials by the addition of terms involving derivatives in the inner product. This type of generalization has been studied in the literature from the point of view of the algebraic properties. Thus, our aim is to study the asymptotics of this sequence of nonstandard orthogonal polynomials. In fact, we obtain Mehler–Heine type formulas for these polynomials and, as a consequence, we prove that there exists an acceleration of the convergence of the smallest positive zeros of these generalized Hermite polynomials towards the origin.
Keywords: asymptotics, Hermite polynomials, Mehler–Heine type formulas, zeros, Bessel functions
DOI: 10.3233/ASY-2009-0961
Citation: Asymptotic Analysis, vol. 66, no. 2, pp. 103-117, 2010
Authors: Vasconcellos, Carlos F. | da Silva, Patricia N.
Article Type: Correction
Abstract: In this erratum of the article: “Stabilization of the linear Kawahara equation with localized damping”, published in Asymptotic Analysis 58(4) (2008), 229–252, DOI 10.3233ASY-2008-0895, we shall fix a mistake which was done when we proved the existence and we defined the countable set of the lengths L where the decay of the energy fails, a set named 𝒩, see Lemma 2.1, p. 235. We considered the equation defined by λu0 +u0 ‴+u0 '''''=0, which is wrong since the parameter η in the Kawahara equation was completely forgotten and it makes changing in the result. In fact, η is a negative …constant and the correct equation is λu0 +u0 ‴+ηu0 '''''=0. Then, as η<0 we can prove, in this case, that the set 𝒩 is empty. Therefore, we obtain that the energy associated with linear Kawahara equation decays exponentially for all lengths L, even in absence of the damping. In the new proof for Lemma 2.1, remain the same idea and the same arguments of the original proof, but the signal of parameter η produces different final result. Show more
DOI: 10.3233/ASY-2010-0987
Citation: Asymptotic Analysis, vol. 66, no. 2, pp. 119-124, 2010
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