Abstract
The magnetostatic interaction energy between two magnetic elements of arbitrary shape is presented as a convolution between the cross-correlation of the particle shapes and the dipolar tensor field. A generalized dipole–dipole interaction is derived, where the magnetic moments associated with the two particles interact through a magnetometric tensor field, carrying all the shape information. Example computations are given in order to verify the correctness of the formalism. The well-known result of the interaction between prisms, employed in most micromagnetic simulations, is correctly retrieved. The numerical accuracy of the method is also compared to a simple analytical result. Finally, one additional example computation, two interlaced interacting rings, is presented to show the generality of the formalism.
| Original language | English |
|---|---|
| Journal | Journal of Magnetism and Magnetic Materials |
| Volume | 285 |
| Issue number | 1-2 |
| Pages (from-to) | L1-L10 |
| ISSN | 0304-8853 |
| DOIs | |
| Publication status | Published - 2005 |
| Externally published | Yes |
Keywords
- Magnetostatic energy
- Shape amplitude
- Magnetic nanoparticles
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