Transmission coefficient of an electron through a saddle-point potential in a magnetic field

1987 ◽  
Vol 36 (15) ◽  
pp. 7969-7976 ◽  
Author(s):  
H. A. Fertig ◽  
B. I. Halperin
1989 ◽  
Vol 39 (6) ◽  
pp. 3780-3784 ◽  
Author(s):  
Ruud van Damme ◽  
Frederik W. Wiegel ◽  
Michael J. Harrison

2011 ◽  
Vol 20 (4) ◽  
pp. 040304 ◽  
Author(s):  
Tao Yang ◽  
Zhi-Yuan Zhai ◽  
Xiao-Yin Pan

2020 ◽  
Vol 60 (5) ◽  
pp. 054005 ◽  
Author(s):  
M. Wensing ◽  
J. Loizu ◽  
H. Reimerdes ◽  
B.P. Duval ◽  
M. Wischmeier ◽  
...  

2020 ◽  
Vol 25 ◽  
pp. 100839
Author(s):  
M. Wensing ◽  
H. de Oliveira ◽  
J. Loizu ◽  
C. Colandrea ◽  
O. Février ◽  
...  

2021 ◽  
Vol 91 (6) ◽  
pp. 995
Author(s):  
А.Б. Ринкевич ◽  
Е.А. Кузнецов ◽  
Д.В. Перов ◽  
М.А. Миляев ◽  
Л.Н. Ромашев

Variations of microwave transmission coefficient through Fe films and Fe/Cr superlattices have been studied caused by ferromagnetic resonance at frequencies from 26 to 38 GHz. The shape of resonance line is described in frames of the model where its asymmetry is obtained by adding of lorenzian dispersion line to the absorption line. It has been shown that the shape of resonance line for superlattices with continuous Fe and Cr layers and also for Fe films is well described in this model. For the superlattices with thin Fe or Cr layers only qualitative agreement is observed. In magnetic fields less than the field of ferromagnetic resonance, essential distinction is observed of experimental magnetic field dependence of transmission coefficient comparing to the model, for superlattices which have giant magnetoresistive effect.


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