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Propagation of Electromagnetic Waves

1993
In this chapter we deal with the fundamentals of wave propagation. The relationships derived are quite general. However, we are chiefly interested in III–V semiconductor materials. Of special significance are optical frequencies in the neighborhood of the bandgap, and hence for AlGaAs wavelengths from yellow-red to the near infra-red region of the ...
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Propagation of Electromagnetic Waves

1958
The propagation of electromagnetic waves has a vectorial character, its basic equations being the vectorial differential equations of Maxwell. In Gaussian units the latter read: $${\begin{array}{*{20}{c}} {{\text{curl }}E + \frac{1}{c}\frac{{\partial B}}{{\partial t}} = 0;{\text{ curl }}H - \frac{1}{c}\frac{{\partial D}}{{\partial t}} = \frac{{4\pi
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Electromagnetic Waves and Propagation

2000
After summarizing Maxwell’s equations in Chapter 11, we are now ready to discuss their implications. In particular, we will deal directly or indirectly with the displacement current term in Maxwell’s equations.
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Electromagnetic Wave Propagation Assessment

1993
Abstract : The roots of electromagnetic propagation research and development in AGARD go back to 1956 when the Ionospheric Research Committee was formed. In 1970, the present Electromagnetic Wave Propagation Panel was established covering the entire spectrum from very low radio through optical and higher frequencies. An example of a recent effort is an
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Plane Electromagnetic Wave Propagation

2018
This chapter is dedicated to the propagation of plane EM wave in different media. Here Maxwell’s equations for time-periodic plane waves are given alongside with consideration of the propagation of waves in lossless, low-loss and highly absorbing media.
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Propagation of Electromagnetic Waves

1991
The propagation of electromagnetic waves in three dimensional dielectric wave guides is described by the Maxwell system of equations $$ \nabla \times \bar{E} = - {{\mu }_{0}}\left( z \right)\frac{{\partial \bar{H}}}{{\partial t}}, $$ (1.1) , $$\nabla \times \bar H = - { \in _0}\left( z \right)\frac{{\partial \bar E}}{{\partial t}},$$ (1 ...
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Propagation of Electromagnetic Waves

1995
Abstract The experimental methods presented in this monograph concern the interaction of light with complex materials for the purpose of elucidating aspects of structure and dynamics. The interactions range from simple transmission and reflection, to scattering and nonlinear responses.
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The Propagation of Electromagnetic Waves

2018
In the previous chapter, electromagnetic waves were introduced as a fundamental phenomenon. All electromagnetic radiation fields can be described using the equations and elementary solutions presented there. The general and exact solution is, however, either too complex or cannot be determined at all.
Reinhart Poprawe   +2 more
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Searches for continuous-wave gravitational radiation

Living Reviews in Relativity, 2023
Keith Riles
exaly  

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