Stefan Bretzel, Gerrit E. W. Bauer, Yaroslav Tserkovnyak, Arne Brataas
Published 2009-07-15Version 1
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.
Comments: 4 pages, 2 figures
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