The Nonstationary Behaviour of the Electron Current Density in the Weakly Inonized Plasma at High Field Frequencies

1991 ◽  
Vol 31 (6) ◽  
pp. 581-594 ◽  
Author(s):  
S. Gundermann ◽  
R. Winkler
2007 ◽  
Vol 17 (03) ◽  
pp. 593-598 ◽  
Author(s):  
N. N. BELETSKII ◽  
S. A. BORYSENKO ◽  
V. M. YAKOVENKO ◽  
G. P. BERMAN ◽  
S. A. WOLF

The magnetoresistance of Fe/MgO/Fe magnetic tunnel junctions (MTJs) was studied taking into consideration image forces. For MTJs with an MgO insulator, explanations are given of the giant tunneling magnetoresistance (TMR) effect and the effect of the increasing TMR with an increase in MgO insulator thickness. It is demonstrated that the electron current density through MTJs can be high enough to switch the magnetization of a ferromagnetic electrode.


1955 ◽  
Vol 99 (4) ◽  
pp. 1192-1195 ◽  
Author(s):  
W. P. Dyke ◽  
J. P. Barbour ◽  
E. E. Martin ◽  
J. K. Trolan

1979 ◽  
Vol 34 (5) ◽  
pp. 648-652
Author(s):  
K. Ueda ◽  
G. Lehmpfuhl ◽  
E. Reuber

Abstract An accurate photographic method for measuring intensities on a fluorescent screen is described. Simultaneously with the fluorescent screen a calibrated 7-step grey scale is recorded on the film. Using a scanning photometer the intensity distribution can be digitized and by comparison with the grey scale converted to electron current density. As an example LEED-intensities from a Si (lll)-surface obtained with the photographic technique are compared with spot-photometer measurements.


1977 ◽  
Vol 34 (4) ◽  
pp. 217-222 ◽  
Author(s):  
Takahiko Nishida ◽  
Kazuhiko Izui ◽  
Shigemi Furuno

1994 ◽  
Author(s):  
S. E. Jones ◽  
J. Kesner ◽  
S. C. Luckhardt ◽  
F. Paoletti ◽  
S. Bernabei ◽  
...  

2017 ◽  
Vol 26 (09) ◽  
pp. 1750094 ◽  
Author(s):  
Alireza Sepehri ◽  
Richard Pincak ◽  
Kazuharu Bamba ◽  
Salvatore Capozziello ◽  
Emmanuel N. Saridakis

We propose a model describing the evolution of the free electron current density in graphene. Based on the concept of Mp-branes, we perform the analysis using the difference between curvatures of parallel and anti-parallel spins. In such a framework, an effective graviton emerges in the form of gauge field exchange between electrons. In a plain graphene system, the curvatures produced by both kinds of spins neutralize each other. However, in the presence of defects, the inequality between curvatures leads to the emergence of current density, modified gravity and conductivity. Depending on the type of the defects, the resulting current density can be negative or positive.


Sign in / Sign up

Export Citation Format

Share Document