2021
DOI: 10.48550/arxiv.2106.01338
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Transverse domain walls in thin ferromagnetic strips

M. Morini,
C. B. Muratov,
M. Novaga
et al.

Abstract: We present a characterization of the domain wall solutions arising as minimizers of an energy functional obtained in a suitable asymptotic regime of micromagnetics for infinitely long thin film ferromagnetic strips in which the magnetization is forced to lie in the film plane. For the considered energy, we provide existence, uniqueness, monotonicity, and symmetry of the magnetization profiles in the form of 180 • and 360 • walls. We also demonstrate how this energy arises as a Γ-limit of the reduced two-dimens… Show more

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Cited by 2 publications
(2 citation statements)
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“…The connection of the energy in (5.17) with the latter is obtained by considering the regime of ν 1. Similarly, the regime that leads to (5.17) is different from the one studied by Kohn and Slastikov in [129], which corresponds to specimens of small lateral extent (see also [173]). Also notice that the energy in (5.16) does not support boundary vortices, which appear in the regime studied by Moser [176].…”
Section: Proposition 1 ([76]mentioning
confidence: 82%
See 1 more Smart Citation
“…The connection of the energy in (5.17) with the latter is obtained by considering the regime of ν 1. Similarly, the regime that leads to (5.17) is different from the one studied by Kohn and Slastikov in [129], which corresponds to specimens of small lateral extent (see also [173]). Also notice that the energy in (5.16) does not support boundary vortices, which appear in the regime studied by Moser [176].…”
Section: Proposition 1 ([76]mentioning
confidence: 82%
“…For thin films, i.e., films whose thickness is smaller than the exchange length ex = 2A/(µ 0 M 2 s ), which is the characteristic length scale at which the exchange and the magnetostatic interactions balance each other, the magnetization vector becomes nearly independent of z, and due to the strong shape anisotropy the magnetization is forced to lie almost entirely in the film plane in magnetically soft materials. There are many possible combinations of the material and geometric parameters that lead to a whole hierarchy of thin film regimes [66,129,176,177,116,126,114,173] (this list is not meant to be exhaustive). For Néel walls in extended films with moderate magnetocrystalline anisotropy, an appropriate model that balances the exchange, anisotropy and the magnetostatic energy as the film thickness vanishes was introduced in [177] (see also [65,39]).…”
Section: Proposition 1 ([76]mentioning
confidence: 99%