opal crystal
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2019 ◽  
Vol 48 (12) ◽  
pp. 8149-8155
Author(s):  
Nguyen Duy Thien ◽  
Nguyen Quang Hoa ◽  
Nguyen Ngoc Tu ◽  
Sai Cong Doanh ◽  
Nguyen Ngoc Long ◽  
...  

Author(s):  
Ivan V. Nemtsev ◽  
Igor A. Tambasov ◽  
Alexander A. Ivanenko ◽  
Victor Ya. Zyryanov

2012 ◽  
Vol 101 (15) ◽  
pp. 151121 ◽  
Author(s):  
Shunsuke Murai ◽  
Situ Yao ◽  
Tadashi Nakamura ◽  
Takahiro Kawamoto ◽  
Koji Fujita ◽  
...  

2011 ◽  
Vol 360 (2) ◽  
pp. 331-334 ◽  
Author(s):  
Ming-Zheng Lin ◽  
Guan-Hui Li ◽  
Ming-Yau Chern ◽  
Chung-Wen Lan

2002 ◽  
Vol 44 (9) ◽  
pp. 1774-1778 ◽  
Author(s):  
V. A. Berezovets ◽  
V. N. Bogomolov ◽  
I. I. Farbshtein ◽  
V. I. Nizhankovskii

2001 ◽  
Vol 694 ◽  
Author(s):  
Bonnie Gersten ◽  
Jennifer Synowczynski

AbstractThe transfer matrix method (TMM) software (Translight, A. Reynolds [1]) was used to evaluate the photonic band gap (PBG) properties of the periodic arrangement of high permittivity ferroelectric composite (40 wt% Ba0.45Sr0.55TiO3 /60 wt% MgO composite, εR= 80, tanδ = 0.0041 at 10 GHz) in air (or Styrofoam, εR~ 1) matrix compared to a lower permittivity material (Al2O3, εR= 11.54, tanδ = 0.00003 at 10 GHz) in air. The periodic structures investigated included a one-dimensional (1D) stack and a three-dimensional (3D) face centered cubic (FCC) opal structure. The transmission spectrum was calculated for the normalized frequency for all incident angles for each structure. The results show that the bandgaps frequency increased and the bandgap width increased with increased permittivity. The effects of orientation of defects in the opal crystal were investigated. It was found by introducing defects propagation bands were introduced. It was concluded that a full PBG is possible with the high permittivity material.


2001 ◽  
Vol 692 ◽  
Author(s):  
Bonnie Gersten ◽  
Jennifer Synowczynski

AbstractThe transfer matrix method (TMM) software (Translight, A. Reynolds [1]) was used to evaluate the photonic band gap (PBG) properties of the periodic arrangement of high permittivity ferroelectric composite (40 wt% Ba0.45Sr0.55TiO3/60 wt% MgO composite, εR = 80, tanδ?= 0.0041 at 10 GHz) in air (or Styrofoam, εR ∼ 1) matrix compared to a lower permittivity material (Al2O3, εR = 11.54, tanδ?= 0.00003 at 10 GHz) in air. The periodic structures investigated included a one-dimensional (1D) stack and a three-dimensional (3D) face centered cubic (FCC) opal structure. The transmission spectrum was calculated for the normalized frequency for all incident angles for each structure. The results show that the bandgaps frequency increased and the bandgap width increased with increased permittivity. The effects of orientation of defects in the opal crystal were investigated. It was found by introducing defects propagation bands were introduced. It was concluded that a full PBG is possible with the high permittivity material.


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