Abstract

We investigate the energy of an isolated magnetized domain Ω⊂RnΩ\subset \mathbb{R}^n for n=2,3n=2,3. In non-dimensionalized variables, the energy given by E(Ω) = ∫Rn∣∇χΩ∣ dx+∫Rn∣∇hΩ∣2 dx \mathcal{E}(Ω) \ = \ \int_{\mathbb{R}^n} |\nabla χ_Ω| \ dx + \int_{\mathbb{R}^n} |\nabla h_Ω|^2 \ dx penalizes the interfacial area of the domain as well as the energy of the corresponding magnetostatic field. Here, the magnetostatic potential hΩh_Ω is determined by ΔhΩ=∂1χΩΔh_Ω= \partial_1 χ_Ω, corresponding to uniform magnetization within the domain. We consider the macroscopic regime ∣Ω∣→∞|Ω| \rightarrow \infty, in which we derive compactness and ΓΓ-limit which is formulated in terms of the cross-sectional area of the anisotropically rescaled configuration. We then give the solutions for the limit problems.

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