Abstract
We determine by a scaling calculation the limiting form of the free energy governing a ferromagnetic film of vanishing thickness. Our theory generalizes Stoner and Wohlfarth's results for flat ellipsoids to arbitrary-shaped very thin films.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 213-223 |
| Number of pages | 11 |
| Journal | Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences |
| Volume | 453 |
| Issue number | 1956 |
| DOIs | |
| State | Published - Jan 1 1997 |
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