Instabilities and generation of a quasistationary magnetic field by the interaction of relativistically intense electromagnetic wave with a plasma

2010 ◽  
Vol 17 (8) ◽  
pp. 082104 ◽  
Author(s):  
S. S. A. Gillani ◽  
N. L. Tsintsadze ◽  
H. A. Shah ◽  
M. Razzaq
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Wave ◽  
Intense Electromagnetic Wave

scholarly journals Hall Effect on the Doped Semiconductor Superlattice with an In-plane Magnetic Field Under Influence of an Intense Electromagnetic Wave

2014 ◽  
Vol 24 (3S1) ◽  
pp. 45-50
Author(s):  
Nguyen Quang Bau ◽  
Bui Dinh Hoi ◽  
Tran Cong Phong
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Wave ◽  
Hall Effect ◽  
Hall Coefficient ◽  
Electron Systems ◽  
Characteristic Parameters ◽  
Semiconductor Superlattice ◽  
Intense Electromagnetic Wave ◽  
Dc Electric Field ◽  
The Magnetic Field

The Hall effect is studied theoretically in a doped semiconductor superlattice (DSSL) subjected to a crossed dc electric field and magnetic field in the presence of an intense electromagnetic wave (EMW). By using the quantum kinetic equation for electrons interacting with acoustic phonons at low temperature, we obtain expressions for the magnetoresistance as well as the Hall coefficient in dependence on the external fields and characteristic parameters of the DSSL. Analytical results are numerically evaluated for the GaAs:Si/GaAs:Be DSSL. The dependence of the magnetoresistance on the magnetic field is consistent with the result obtained for some two-dimensional electron systems. The Hall coefficient depends weakly on the magnetic field and its value in the presence of the EMW is smaller than that of the case without EMW.

Investigation of the magnetoresistivity in compositional superlattices under the influence of an intense electromagnetic wave

2016 ◽  
Vol 30 (04) ◽  
pp. 1650004 ◽  
Author(s):  
Bui Dinh Hoi ◽  
Nguyen Quang Bau ◽  
Nguyen Dinh Nam
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Wave ◽  
Growth Direction ◽  
Electron Systems ◽  
Semiconductor Superlattice ◽  
Intense Electromagnetic Wave ◽  
Superlattice Structure ◽  
Dc Electric Field ◽  
Electron Acoustic ◽  
Increasing Temperature

The magnetoresistivity (MR) is theoretically calculated in a compositional semiconductor superlattice (CSSL), subjected to a crossed DC electric field and magnetic field, in the presence of an intense electromagnetic wave (EMW). The magnetic field is oriented along the growth direction of the CSSL and the electron–acoustic phonon interaction is taken into account at low temperature. Numerical results for the GaN/AlGaN CSSL show the Shubnikov–de Haas (SdH) oscillations in the MR whose period does not depend on the temperature and amplitude decreases with increasing temperature. The temperature dependence of the relative amplitude of these oscillations is in good agreement with other theories and experiments in some two-dimensional (2D) electron systems. The influence of the EMW as well as superlattice structure on the MR is discussed and compared with available theoretical and experimental results.

scholarly journals Manipulating the Electromagnetic Wave with a Magnetic Field

10.5772/14005 ◽  
2011 ◽  
Author(s):  
Shiyang Liu ◽  
Zhifang Lin ◽  
S. T.
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Wave

Diffraction by a perfectly conducting wedge in an anisotropic plasma

1965 ◽  
Vol 61 (3) ◽  
pp. 767-776 ◽  
Author(s):  
T. R. Faulkner
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Wave ◽  
Difference Equation ◽  
Integral Representation ◽  
Surface Waves ◽  
Uniform Magnetic Field ◽  
Anisotropic Plasma ◽  
Contour Integral ◽  
Anisotropic Dielectric

SummaryThe problem considered is the diffraction of an electromagnetic wave by a perfectly conducting wedge embedded in a plasma on which a uniform magnetic field is impressed. The plasma is assumed to behave as an anisotropic dielectric and the problem is reduced, by employing a contour integral representation for the solution, to solving a difference equation. Surface waves are found to be excited on the wedge and expressions are given for their amplitudes.

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