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- W2022982571 abstract "From the second variation of the integral of all free energies in thin magnetic films, an effective field <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>h_{eff}(alpha)</tex> is deduced, which for real polycrystalline films is analogous to the Stoner-Wohlfarth field <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>h(alpha)</tex> of ideal single-domain films. The effective field is composed of the single-domain field, two different stray fields, and a field caused by local anisotropies. The <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>h_{eff}(alpha)</tex> varies from point to point. As in the single-domain theory, <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>h_{eff}(alpha) > 0</tex> means that the magnetization direction over the entire film is stable; in regions with <tex xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>h_{eff}(alpha) = 0</tex> , the local magnetization becomes unstable and turns by a very small angle to another stable state. After that, the domain structure is blocked by the intrinsic stray field. The blocking condition, which is the external single-domain field at which blocking occurs, is calculated as a function of film structure. The critical curve for stray-field blocking shows that the critical Stoner-Wohlfarth curve of the single-domain theory must not be used in discussing experiments on real polycrystalline films." @default.
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- W2022982571 date "1966-09-01" @default.
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- W2022982571 title "Stray fields in thin magnetic films" @default.
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- W2022982571 doi "https://doi.org/10.1109/tmag.1966.1065919" @default.
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