Limits of applicability of the geometrical optics approximation for electromagnetic waves exiting from an inhomogeneous layer of magnetoactive plasma

1977 ◽  
Vol 20 (2) ◽  
pp. 216-218
Author(s):  
N. G. Denisov
1989 ◽  
Vol 41 (1) ◽  
pp. 31-36 ◽  
Author(s):  
A. M. Hussein

An investigation is made of wave generation and radiation of third harmonics by s-polarized electromagnetic waves incident on a narrow inhomogeneous layer of a magnetoactive plasma. The amplitudes of the radiated third-harmonic waves are calculated. In contrast with second harmonics, third harmonics are radiated for the case of normally incident waves on an unmagnetized plasma.


1985 ◽  
Vol 33 (1) ◽  
pp. 151-155 ◽  
Author(s):  
A. M. Hussein

Amplitudes of electromagnetic waves with combination frequencies, radiating from a narrow inhomogeneous layer of the magnetoactive plasma due to interaction of the surface waves, are determined. The method used allows for discontinuity of the tangential components of the wave electric field at the combination frequencies at the plasma boundary.


Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter examines solutions to the Maxwell equations in a vacuum: monochromatic plane waves and their polarizations, plane waves, and the motion of a charge in the field of a wave (which is the principle upon which particle detection is based). A plane wave is a solution of the vacuum Maxwell equations which depends on only one of the Cartesian spatial coordinates. The monochromatic plane waves form a basis (in the sense of distributions, because they are not square-integrable) in which any solution of the vacuum Maxwell equations can be expanded. The chapter concludes by giving the conditions for the geometrical optics limit. It also establishes the connection between electromagnetic waves and the kinematic description of light discussed in Book 1.


1993 ◽  
Vol 49 (2) ◽  
pp. 227-235 ◽  
Author(s):  
S. T. Ivanov ◽  
K. M. Ivanova ◽  
E. G. Alexov

Electromagnetic wave propagation along the interface between a magnetoactive plasma and a metallic screen is investigated analytically and numerically. It is shown that the waves have a Rayleigh character: they are superpositions of two partial waves. It is concluded that electromagnetic waves propagate only at frequencies lower than min (ωp, ωc), where ωpis the plasma frequency and ωcis the cyclotron frequency. The field topology is found, and the physical character of the waves is discussed.


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