Abstract
The Barnett effect refers to the magnetization induced by rotation of a demagnetized ferromagnet. We describe the location and stability of stationary states in rotating nanostructures using the Landau-Lifshitz-Gilbert equation. The conditions for an experimental observation of the Barnett effect in different materials and sample geometries are discussed.
Original language | English |
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Article number | 122504 |
Journal | Applied Physics Letters |
Volume | 95 |
Issue number | 12 |
DOIs | |
Publication status | Published - 2009 |