| Issue |
J. Phys. Colloques
Volume 49, Number C8, Décembre 1988
Proceedings of the International Conference on Magnetism
|
|
|---|---|---|
| Page(s) | C8-905 - C8-906 | |
| DOI | https://doi.org/10.1051/jphyscol:19888411 | |
Proceedings of the International Conference on Magnetism
J. Phys. Colloques 49 (1988) C8-905-C8-906
DOI: 10.1051/jphyscol:19888411
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.
J. Phys. Colloques 49 (1988) C8-905-C8-906
DOI: 10.1051/jphyscol:19888411
NOTE ON ENERGY FORMULATION OF THE FMR RESONANCE CONDITION
M. Marysko1, L. Baselgia2, M. Warden2, F. Waldner2, S. L. Hutton3, J. E. Drumheller3, Y. Q. He4 et P. E. Wigen41 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.
Abstract
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.