The interaction of an obliquely incidents-polarized plane electromagnetic wave at a warm moving magnetized plasma half-space

1975 ◽  
Vol 33 (1) ◽  
pp. 147-163 ◽  
Author(s):  
P. K. Mukherjee ◽  
S. P. Talwar
Keyword(s):  
Electromagnetic Wave ◽  
Half Space ◽  
Plane Electromagnetic Wave ◽  
Magnetized Plasma

Reflection of waves at an interface in a streaming plasma

1968 ◽  
Vol 2 (3) ◽  
pp. 381-393
Author(s):  
P. C. Clemmow ◽  
E. Ott
Keyword(s):  
Electromagnetic Wave ◽  
Half Space ◽  
Cold Plasma ◽  
Plane Electromagnetic Wave ◽  
Plasma Stream ◽  
Relativistic Velocity ◽  
Reflected Wave ◽  
First Approximation ◽  
Transmitted Waves ◽  
The Face

A uniform, unbounded, cold plasma stream, with relativistic velocity (0,U, 0), traverses a vacuum half-spacey> 0 and a dielectric half-spacey< 0. A plane electromagnetic wave in the plasma stream iny> 0 is incident obliquely on the face of the dielectric. The criterion for determining which characteristic waves are present in each half space is discussed, and it is shown that, for the polarization in which B is parallel toy= 0, there is one reflected wave and three transmitted waves. One of the latter can be an amplifying wave. A first approximation to the transmission and reflexion coefficients is found in the case when the density of the stream is low.

scholarly journals REFLECTION OF ELECTROMAGNETIC WAVE FROM THE BORDER OF ELASTIC ENVIRONMENT FROM PIEZOACTIVE MATERIAL

2020 ◽  
Vol 6 (5) ◽  
pp. 2-5
Author(s):  
M.V. Belubekyan ◽  
◽  
V.G. Garakov ◽  
Keyword(s):  
Electromagnetic Wave ◽  
Piezoelectric Material ◽  
Half Space ◽  
Plane Electromagnetic Wave ◽  
Dielectric Medium ◽  
Hexagonal Symmetry ◽  
Reflection And Refraction ◽  
Elastic Shear ◽  
Transparency Condition ◽  
Wave Incidence

A plane electromagnetic wave incident on the interface of a dielectric medium made of a piezoactive material leads to the excitation of elastic shear waves. Piezoelectric material is assumed to have 6mm class hexagonal symmetry. The case of a half-space and a finite layer is considered. Coefficients of reflection and refraction are determined. In the problem of an electromagnetic wave incidence on a half-space made of a piezoelectric material of hexagonal symmetry, class 6 mm, the nature of the piezoelectric effect influence on the transparency condition is established. In the case of reflection from a finite piezolayer, reflection coefficients are determined for different variants of boundary conditions.

Reflexion of a plane wave at a plasma half-space

1970 ◽  
Vol 4 (1) ◽  
pp. 67-81 ◽  
Author(s):  
P. C. Clemmow ◽  
V. B. Karunarathne
Keyword(s):  
Electromagnetic Wave ◽  
Boundary Conditions ◽  
Half Space ◽  
Diffuse Scattering ◽  
Oblique Incidence ◽  
Plane Electromagnetic Wave ◽  
Current Source ◽  
Normal Incidence ◽  
Plane Boundary ◽  
Method Of Solution

The problem of a monochromatic plane electromagnetic wave incident from vacuum on the plane boundary of a plasma half-space is considered. The method of solution is based on the representation of the disturbance in the plasma half- space as that generated by some current source in the complementary half-space into which, for the purpose of the representation, the plasma is conceived to extend. The specular reflexion boundary conditions and the diffuse scattering boundary conditions are treated in turn, first for normal incidence and then for oblique incidence.

scholarly journals Accessibility to the Lower Hybrid Resonance

1973 ◽  
Vol 28 (3-4) ◽  
pp. 438-442 ◽  
Author(s):  
S. Puri ◽  
M. Tutter
Keyword(s):  
Electromagnetic Wave ◽  
Cold Plasma ◽  
Plane Electromagnetic Wave ◽  
Transverse Magnetic ◽  
Magnetized Plasma ◽  
Dielectric Tensor ◽  
Lower Hybrid ◽  
Vacuum Plasma ◽  
Hybrid Resonance ◽  
Lower Hybrid Resonance

AbstractAccessibility of a plane electromagnetic wave into an inhomogeneous, magnetized plasma column is studied using the complete cold plasma dielectric tensor. It is found that TM (transverse magnetic) waves incident at small angles with the vacuum-plasma interface are almost completely transmitted into the plasma even though the criterion for accessibility to the lower-hybrid resonance is not satisfied. The significance of this result for coupling rf energy into plasma filled waveguides is discussed.

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