Abstract:We consider a thin multidomain of R 3 consisting of two vertical cylinders, one placed upon the other: the first one with given height and small cross section, the second one with small thickness and given cross section. The first part of this paper is devoted to analyze, in this thin multidomain, a "static Landau-Lifshitz equation", when the volumes of the two cylinders vanish. We derive the limit problem, which decomposes into two uncoupled problems, well posed on the limit cylinders (with dimensions 1 and 2… Show more
“…Therefore, converges (14) follow and these converges hold true for the whole sequence. Convergence (15) is a consequence of (14).…”
Section: Convergence Results Of the Magnetostatic Energymentioning
confidence: 99%
“…Reformulating the problem on a fixed domain through appropriate rescalings of the kind proposed by Ciarlet and Destuynder [5] and using the main ideas used by [3,4,8,12,13] and [14], we derive the limit problem in both cases. Specifically, in the case of nanowires, we prove that (see Theorem 1)…”
The aim of the work described in this paper is to determine, via an asymptotic analysis, the limiting form of the free energy governing in the first case 3D ferromagnetic nanowires of infinite length in the limit and in the second case 3D thin films which become infinite when their thickness is vanished. A 1D limit problem on the nanowires and a 2D limit problem on the thin films are obtained.Mathematics Subject Classification. 78A25 · 49S05 · 78M35.
“…Therefore, converges (14) follow and these converges hold true for the whole sequence. Convergence (15) is a consequence of (14).…”
Section: Convergence Results Of the Magnetostatic Energymentioning
confidence: 99%
“…Reformulating the problem on a fixed domain through appropriate rescalings of the kind proposed by Ciarlet and Destuynder [5] and using the main ideas used by [3,4,8,12,13] and [14], we derive the limit problem in both cases. Specifically, in the case of nanowires, we prove that (see Theorem 1)…”
The aim of the work described in this paper is to determine, via an asymptotic analysis, the limiting form of the free energy governing in the first case 3D ferromagnetic nanowires of infinite length in the limit and in the second case 3D thin films which become infinite when their thickness is vanished. A 1D limit problem on the nanowires and a 2D limit problem on the thin films are obtained.Mathematics Subject Classification. 78A25 · 49S05 · 78M35.
“…[11][12][13][14]) who studied the junction of ferromagnetic bodies. In [13], they considered two orthogonal ferromagnetic thin films and they proved that the limit magnetization is coupled when the volumes of the two thin films vanish with the same rate.…”
Section: Introductionmentioning
confidence: 99%
“…In [13], they considered two orthogonal ferromagnetic thin films and they proved that the limit magnetization is coupled when the volumes of the two thin films vanish with the same rate. In [12] and [11], they developed an asymptotic analysis of minimizing maps with values in S 2 for the energy Ω n (|DM | 2 − 2F n M )dx, neglecting the term with non-local magnetostatic energy.…”
“…We explicitly remark that formula (1.5) was obtained in [13] in the case n = 3 and p = 1. For junction 1D-2D we refer to [10] and [15]. For junction 1D-1D we refer to [11].…”
Starting from a n D, n ≥ 2, non-convex and nonlocal micromagnetic energy, we determine, via an asymptotic analysis, the free energy of a pD ferromagnetic domain, 1 ≤ p < n.
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