J. Phys. Colloques
Volume 49, Numéro C8, Décembre 1988Proceedings of the International Conference on Magnetism
|Page(s)||C8-905 - C8-906|
J. Phys. Colloques 49 (1988) C8-905-C8-906
NOTE ON ENERGY FORMULATION OF THE FMR RESONANCE CONDITIONM. Marysko1, L. Baselgia2, M. Warden2, F. Waldner2, S. L. Hutton3, J. E. Drumheller3, Y. Q. He4 et P. E. Wigen4
1 Institute of Physics, Czechoslovak Academy of Science Na Slovance 2 CS-18040 Praha 8, Czechoslovakia
2 Physics Institute, University of Zurich, CH-8001 Zurich, Switzerland
3 Department of Physics, Montana State University, Bozeman, MT59717, U.S.A.
4 Department of Physics, The Ohio State University, Columbus, OH43210, U.S.A.
As is known the classical FMR resonance condition by Smit and Beljers cannot be directly used zero angle between the magnetization and polar axis. This difficulty can be avoided using the new form of resonance condition which has been derived by the transformation from the rectangular coordinate system.