Analysis of evanescent field of TE and TM mode in the grounded slab metamaterial waveguide structure

Optik ◽  
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Vol 126 (23) ◽  
pp. 3706-3712 ◽  
Author(s):  
Santosh Kumar ◽  
Anamika Kumari ◽  
Bhagirathi Pradhan
2016 ◽  
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pp. 1552-1557 ◽  
Author(s):  
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Bouchra Mokhtari ◽  
Noureddine Cherkaoui Eddeqaqi ◽  
Mohammed Musa Shabat ◽  
Jacques Atangana

2011 ◽  
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Zhangjing Yi ◽  
Rongjin Yan ◽  
Timothy A. Erickson ◽  
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Kevin L. Lear

2015 ◽  
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pp. 409-415 ◽  
Author(s):  
Nan Zhang ◽  
Peiheng Zhou ◽  
Linbo Zhang ◽  
Xiaolong Weng ◽  
Jianliang Xie ◽  
...  

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Vol 30 (23) ◽  
pp. 2068-2071 ◽  
Author(s):  
Wanying Li ◽  
Yi Su ◽  
Xiang Zhai ◽  
Xiongjun Shang ◽  
Shengxuan Xia ◽  
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2020 ◽  
Vol 20 (15) ◽  
pp. 8469-8476 ◽  
Author(s):  
Svetlana Nikolaevna Khonina ◽  
Nikolay Lvovich Kazanskiy ◽  
Muhammad Ali Butt

2014 ◽  
Vol 4 (3) ◽  
pp. 585-594
Author(s):  
Hana Mohammed Mousa

This paper tackles the simulation of an asymmetric  TM mode absorption  in a lossy metamaterial (left-handed) slab (LHM) sandwiched between a lossy substrate and coverd by a losseless dielectric cladding. The asymmetry solutions of the eigen value equation describe  lossy –guided modes with complex –valued propagation constants .  The dispersion relations , normalized field and the longitudinal attenuation  were numerically solved for a given set of parameters: frequency range; film’s thicknesses; and TM mode order. I found out that high order modes which are guided in thinner films are generally have more loss of power than low-order modes since the mode attenuation along z-axis increases to negative values by the mode's order increase and the film thickness decrease . Moreover,  LHM , at  incident wavelength =1.9, refractive index=and  at thickness ,   guides the power better  than  RHM  or metal one. This LHM   is appropriate for solar cell applications. For arbitrary LHM, at frequency band of wavelengt(600, 700 to 1200 )nm,  the best absorption is attained at longer wavelengths and for lower order modes at wider films.


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