Theory of ferromagnetic resonance line shape in insulators

1960 ◽  
Vol 10 (11) ◽  
pp. 775-781 ◽  
Author(s):  
J. Loos
1971 ◽  
Vol 49 (3) ◽  
pp. 387-390 ◽  
Author(s):  
S. T. Wang ◽  
C. W. Searle

The resonance line shape and line width of the family La(1−x)PbxMnO3 have been examined from 77 to 430 °K in a frequency range from 13 to 25 GHz. The distorted line shape is in qualitative agreement with a calculation that includes the effect of the skin depth. The antiresonance condition has been observed and it is also in qualitative agreement with theory.


1965 ◽  
Vol 140 (3A) ◽  
pp. A972-A985 ◽  
Author(s):  
K. Motizuki ◽  
M. Sparks ◽  
P. E. Seiden

2006 ◽  
Vol 73 (13) ◽  
Author(s):  
B. Abdo ◽  
E. Segev ◽  
O. Shtempluck ◽  
E. Buks

1990 ◽  
Vol 158 (1) ◽  
pp. K55-K58 ◽  
Author(s):  
E. I. Neimark ◽  
I. N. Nurutdinova ◽  
A. B. Roitsin
Keyword(s):  

1976 ◽  
Vol 19 (5) ◽  
pp. 643-645
Author(s):  
A. V. Zatovskii

1969 ◽  
Vol 47 (23) ◽  
pp. 2703-2708 ◽  
Author(s):  
C. W. Searle ◽  
S. T. Wang

Ferromagnetic resonance has been observed in single crystals of the family La1−xPbxMnO3with 0.25 < x < 0.45 from 13 to 25 GHz and in the temperature range from 77 to 430 °K. The line width, ΔH, exhibits a sharp minimum accompanied by an isotropic shift in the resonance line at a critical temperature, Tc. Tc is dependent on the concentration of Mn4+ and has been related to the Curie temperature. The shift in the peak of the resonance line at Tc can be described by effects related to the formation of a spin-polarized conduction band. The line shape is asymmetric at high temperatures, ~Tc, and at low temperatures, T ~ 77 °K. This asymmetric behavior of the line is probably due to transport properties of the conduction-band electrons.


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