Maximization of Photonic Bandgaps in Two-Dimensional Superconductor Photonic Crystals

2014 ◽  
Vol 27 (7) ◽  
pp. 1615-1621 ◽  
Author(s):  
Sahar A. El-Naggar ◽  
Hussein A. Elsayed ◽  
Arafa H. Aly
2009 ◽  
Vol 23 (06n07) ◽  
pp. 1300-1305
Author(s):  
KI-HO SONG ◽  
HYUN-YONG LEE ◽  
HOE-YOUNG YANG ◽  
SUNG-WON KIM ◽  
JAE-HEE SEO ◽  
...  

Two-dimensional photonic crystals (2D-PCs) with Ge 2 Sb 2 Te 5 ( GST ) nanohole arrays were prepared by the nanosphere lithography (NSL) process. A primary factor of PCs is that the refractive index (n) and the n-modulation can be realized by using the GST films, which exhibit a reversible phase transformation between amorphous and crystalline states by laser illumination. The polystyrene (PS) spheres with a diameter of 500 nm were spin-coated on Si substrate and subsequently reduced by O 2-plasma treatment. The reduced spheres were utilized as a lift-off mask of the NSL process and their size and separation could be precisely controlled. Amorphous GST films were thermally evaporated and then the reduced PS spheres were removed. The fabricated GST nanohole arrays were observed by SEM and AFM. The nanohole diameters are nearly linearly reduced with increasing plasma-treatment time (t). The reduction rate (δ) for the conditions of this work was evaluated to be ~ 0.92 nm/s. The period (Λ) and filling factor (η) of PCs are structure parameters that determine their photonic bandgaps (PBGs). η-modulation can be easily achieved via a control of t and the Λ can be also modulated by the use of PS spheres with specific diameter. In addition, the PBGs for the fabricated GST 2 D PC were calculated by considering the amorphous and crystalline states of GST .


2013 ◽  
Vol 441 ◽  
pp. 80-83
Author(s):  
Yong Wan ◽  
He Zhang ◽  
Wan Qin Yang ◽  
Chao Li ◽  
Ming Hui Jia

Scattering units or building blocks are the basic elements for photonic crystal lattices. Photonic bandgaps can be tuned and improved in two-dimensional (2D) triangular lattices, as well as in square lattices by introducing axial-symmetry cylinder-segments instead of cylinders as basic scattering units. Owing to the changes of bulks, reflectance effect of electromagnetic waves will be different both in TE modes and in TM modes. The widths of bandgaps for the two polarization modes can be adjusted and matched to overlap in some range.


2011 ◽  
Vol 105 (4) ◽  
pp. 789-793 ◽  
Author(s):  
Jian Shen ◽  
Shiyang Liu ◽  
Rong Cao ◽  
Xin Fan ◽  
Junjie Du ◽  
...  

2014 ◽  
Vol 61 (13) ◽  
pp. 1064-1068 ◽  
Author(s):  
Arafa H. Aly ◽  
Hussein A. Elsayed ◽  
Sahar A. El-Naggar

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