Large magnonic band gaps and defect modes in one-dimensional comblike structures

1999 ◽  
Vol 59 (13) ◽  
pp. 8709-8719 ◽  
Author(s):  
H. Al-Wahsh ◽  
A. Akjouj ◽  
B. Djafari-Rouhani ◽  
J. O. Vasseur ◽  
L. Dobrzynski ◽  
...  
2011 ◽  
Vol 43 (6) ◽  
pp. 1016-1019 ◽  
Author(s):  
Tingting Tang ◽  
Wenli Liu ◽  
Xiuying Gao ◽  
Xiujun He ◽  
Jun Yang

2003 ◽  
Vol 15 (10) ◽  
pp. 1593-1598 ◽  
Author(s):  
A Mir ◽  
A Akjouj ◽  
J O Vasseur ◽  
B Djafari-Rouhani ◽  
N Fettouhi ◽  
...  

2021 ◽  
Author(s):  
Ali Baseri ◽  
Alireza Keshavarz

Abstract Although there has been a focus on THz lters so far, there is a signifcant defciency in advancing low-temperature THz lters. According to the needs, we proposed a tunable THz lter that selectively permits the desired incident frequencies to be propagated in relevance with our purpose. The presence of a low-temperature nano superconductor and an undoped semiconductor layers in the proposed structure resulted in a multi-channel THz lter, which could be highly tuned with several parameters such as lattice constants, applied temperature, etc. The achieved transmittance spectra revealed that the emerged transmittance couples and stacks follow exact regulations. Furthermore, the structure exhibited omnidirectional band-gaps for both TE and TM polarized waves. Moreover, the use of a central defect layer gave some transmittance defect modes in the forbidden areas. This structure could be used in some THz devices such as switches, optimized sensors as well as in space industry and telecommunications.


2002 ◽  
Vol 112 (4) ◽  
pp. 1353-1358 ◽  
Author(s):  
J. N. Munday ◽  
C. Brad Bennett ◽  
W. M. Robertson
Keyword(s):  

2010 ◽  
Vol 663-665 ◽  
pp. 725-728 ◽  
Author(s):  
Yuan Ming Huang ◽  
Qing Lan Ma ◽  
Bao Gai Zhai ◽  
Yun Gao Cai

Considered the model of the one-dimensional photonic crystals (1-D PCs) with double defects, the refractive indexes (n2’, n3’ and n2’’, n3’’) of the double defects were 2.0, 4.0 and 4.0, 2.0 respectively. With parameter n2=1.5, n3=2.5, by theoretical calculations with characteristic matrix method, the results shown that for a certain number (14 was taken) of layers of the 1-D PCs, when the double defects abutted, there was a defect band gap in the stop band gap, while when the double defects separated, there occurred two defect band gaps in the stop band gap; besides, with the separation of the two defects, the transmittance of the double defect band gaps decreased gradually. In addition, in this progress, the frequency range of the stop band gap has a little increase from 0.092 to 0.095.


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