Application of Mathematical Programming in Problem of Electromagnetic Waves Nonlinear Scattering on Circular Cylinder

Author(s):  
Andrey I. Panychev
1969 ◽  
Vol 47 (11) ◽  
pp. 1159-1166 ◽  
Author(s):  
K. Aoki

This paper discusses eigenvalues of the electromagnetic field along an infinitely long and conductive circular cylinder imbedded in a magnetoionic medium under assumptions that the medium is lossless and the field frequency is not equal to the cyclotron frequency. It is shown that they are classified into two kinds: (i) k1 and k2 are pure imaginary and (ii) k22 = (complex conjugate of k12), where k1 and k2 are the radial propagation constants and that no eigenvalues exist in the region bounded by [Formula: see text] where ωp and ωc are the plasma and cyclotron frequencies normalized to the field frequency. Some numerical results in the case of (radius of the cylinder/wavelength) [Formula: see text] are also shown.


1979 ◽  
Vol 57 (12) ◽  
pp. 2132-2135
Author(s):  
S. R. Valluri ◽  
P. Bhartia

The differential scattered power is calculated for the nonlinear interaction of two electromagnetic waves in a vacuum. It is calculated for both parallel [Formula: see text] and perpendicular [Formula: see text] polarization cases and expressed as a function of the scattering angle θ′. In an earlier paper we have treated the nonlinear interaction by the introduction of the Lagrangian for the ultrastrong field case. A detailed discussion of the power indicates the position of the maxima and minima at various angles and hence would enable the experimentalist to set up the required orientation of the detecting apparatus. The promise of continuous, intense, and monochromatic polarized radiation from electron synchrotrons and storage rings motivates the study and experimental confirmation is hoped for.


Nanophotonics ◽  
2020 ◽  
Vol 9 (9) ◽  
pp. 2771-2781 ◽  
Author(s):  
Cheng Zhang ◽  
Jin Yang ◽  
Liu Xi Yang ◽  
Jun Chen Ke ◽  
Ming Zheng Chen ◽  
...  

AbstractTime-domain digital coding metasurfaces have been proposed recently to achieve efficient frequency conversion and harmonic control simultaneously; they show considerable potential for a broad range of electromagnetic applications such as wireless communications. However, achieving flexible and continuous harmonic wavefront control remains an urgent problem. To address this problem, we present Fourier operations on a time-domain digital coding metasurface and propose a principle of nonlinear scattering-pattern shift using a convolution theorem that facilitates the steering of scattering patterns of harmonics to arbitrarily predesigned directions. Introducing a time-delay gradient into a time-domain digital coding metasurface allows us to successfully deviate anomalous single-beam scattering in any direction, and thus, the corresponding formula for the calculation of the scattering angle can be derived. We expect this work to pave the way for controlling energy radiations of harmonics by combining a nonlinear convolution theorem with a time-domain digital coding metasurface, thereby achieving more efficient control of electromagnetic waves.


The assumption that the illuminated region and the penumbra of a body scatter independently at high frequencies is used to obtain scattering coefficients for perfectly reflecting convex bodies in plane electromagnetic and sound waves. The formulae involve only the scattering coefficients of the circular cylinder and the geometry of the shadow boundary. One general result is that the electromagnetic scattering coefficient of a solid of revolution, when the direction of propagation of the incident wave is along the axis of revolution, is the average of the sound-hard and sound-soft scattering coefficients.


2021 ◽  
Vol 2052 (1) ◽  
pp. 012041
Author(s):  
A V Sochilin ◽  
S I Eminov

Abstract The vector equation for the diffraction of electromagnetic waves on the surface of a rectilinear circular cylinder without ends with respect to surface currents is considered. As a result of transformations from the original equation, one-dimensional systems of integral equations are obtained. For all four integral operators describing the systems, the main parts are highlighted. Using the remarkable properties of one-dimensional diffraction operators, the Fredholm equation of the second kind in Sobolev spaces is obtained.


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