Modeling of anisotropic grating structures with active dipole layers

Author(s):  
K. Postava ◽  
T. Fördös ◽  
H. Jaffrès ◽  
L. Halagačka ◽  
H. J. Drouhin ◽  
...  
Keyword(s):  
2015 ◽  
Vol 92 (1) ◽  
Author(s):  
Andreas Kaiser ◽  
Katarina Popowa ◽  
Hartmut Löwen
Keyword(s):  

2011 ◽  
Vol 119 ◽  
pp. 265-277 ◽  
Author(s):  
Juan Antonio Rodríguez-González ◽  
Francisco Jose Ares-Pena

1989 ◽  
Vol 6 (5) ◽  
pp. 533-543 ◽  
Author(s):  
A. Z. Rabinovich ◽  
M. V. Loseva ◽  
N. I. Chernova ◽  
E. P. Pozhidaev ◽  
O. S. Petrashevich ◽  
...  

2018 ◽  
Vol 7 (1) ◽  
pp. 51-56 ◽  
Author(s):  
H. Patidar ◽  
G. K. Mahanti

This paper presents a new approach for circular array of parasitic dipoles composed by one active dipole for reduction of side lobe level with maximum directivity including mutual coupling. The desired goal is obtained by changing the spacing between the parasitic elements and length of the parasitic elements while the position and length of driven element is fixed. In addition to it, reflection coefficient (RC) of the driven element is kept closer to the specified value. Matlab based method of moment code is used to evaluate the performance of circular antenna designs generated by QPSO algorithm. Two examples are presented to show the effectiveness of this proposed approach.  


2003 ◽  
Vol 1 ◽  
pp. 57-61 ◽  
Author(s):  
F. Gronwald

Abstract. We study the influence of both the electromagnetic source singularity and electromagnetic cavity resonances on the current distribution of a dipole antenna within a rectangular cavity. These two types of electromagnetic singularities are triggered by the radius of the dipole antenna and the quality factor of the enclosing cavity, respectively. The key element of our investigation is a novel representation of the electromagnetic Green’s function for a lossy rectangular cavity. It allows to directly obtain the current distribution on the antenna by means of the method of moments. As a result it is recognized that a dominating source singularity, i.e., a small antenna radius, can inhibit resonating effects, even if a cavity resonance is excited and the quality factor of the cavity is high.


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