3D Photonic Crystals Fabricated by Micromanipulation Technique

2002 ◽  
Vol 722 ◽  
Author(s):  
Kanna Aoki ◽  
Hideki T. Miyazaki ◽  
Hideki Hirayama ◽  
Kyoji Inoshita ◽  
Toshihiko Baba ◽  
...  

AbstractThree-dimensional (3D) photonic crystals with one to four layers of woodpile structures have been fabricated by stacking two-dimensional (2D) photonic plates by micromanipulation. First, air-bridge photonic plates were fabricated as unit structures using conventional IC processing techniques. Then, the 2D photonic plates were stacked using a micromanipulation system. To obtain lattices with precise periodicity, microspheres were inserted into the round openings which were prepared in the frame of the plates. Since neighboring plates have pore openings at the same position, plates were laminated at the proper position automatically. Consequently, positioning error was kept within 50 nm. Optical characteristics of the crystals were evaluated by their reflectance and transmittance at wavenumber between 700 and 7000 cm-1. The formed photonic crystals were expected to have a photonic band gap at around 3030 cm-1. As the number of layers was increased, the reflectance at around 3030 cm-1 increased to 60 %, and the transmittance at the same wavelength region decreased to 30 %.

2003 ◽  
Vol 18 (9) ◽  
pp. 2214-2220 ◽  
Author(s):  
Shingo Kanehira ◽  
Soshu Kirihara ◽  
Yoshinari Miyamoto ◽  
Kazuaki Sakoda ◽  
Mitsuo Wada Takeda

Three-dimensional photonic crystals with a diamond structure, which are composed of the TiO2-based ceramic particles dispersed in an epoxy lattice, were fabricated by stereolithography. The diamond structure showed a photonic band gap in the 14.3–17.0 GHz range along the Γ-K 〈110〉 direction, which is close to the band calculation using the plain wave expansion method. Two types of lattice defects—air cavity and dielectric cavity—were introduced into the diamond structure by removing a unit cell of diamond structure or inserting a block of the lattice medium into the air cavity. The transmission of millimeter waves affected by multiple reflections at the defects was measured in the photonic band gap. Resonant frequencies in the defects were calculated and compared with the measurement results.


2013 ◽  
Vol 28 (2) ◽  
pp. 253-263 ◽  
Author(s):  
U. Erdiven ◽  
F. Karadag ◽  
M. Karaaslan ◽  
E. Unal ◽  
F. Dincer ◽  
...  

2011 ◽  
Vol 83 (20) ◽  
Author(s):  
Simon R. Huisman ◽  
Rajesh V. Nair ◽  
Léon A. Woldering ◽  
Merel D. Leistikow ◽  
Allard P. Mosk ◽  
...  

2012 ◽  
Vol 90 (2) ◽  
pp. 175-180 ◽  
Author(s):  
M. Moghimi ◽  
S. Mirzakuchaki ◽  
N. Granpayeh ◽  
N. Nozhat ◽  
G.H. Darvish

The band gaps of the two-dimensional photonic crystals, created by inhomogeneous triangular photonic crystal of variable central hexagonal holes are derived. The structure is made of air holes in GaAs. We present the best absolute photonic band gap for this structure by changing the holes’ radii. The photonic band gaps are calculated by the plane wave expansion method. The results indicate 95% overlap in the band gaps of both polarizations of TE and TM in triangular lattice.


2004 ◽  
Vol 820 ◽  
Author(s):  
Koichi Awazu ◽  
Makoto Fujimaki ◽  
Xiaomin Wang ◽  
Akihide Sai ◽  
Yoshimichi Ohki

AbstractTwo dimensional photonic crystals of titanium dioxide is expected to have many advantage compared with photonic crystals of semiconductors, e.g., silicon and GaAs. For example, low optical loss in the near infrared region used for optical communication, low thermal expansion, and its refractive index which is close to that for optical fiber are attractive advantages. However, it is difficult to create micro-nano structure in titanium dioxide because micro-fabrication technique for semiconductor is not available for titanium dioxide. As the first step we calculated photonic band gap of titanium dioxide rod-slab on SiO2. Also, band gap percent against thickness of the rod-slab was examined. Finally, we confirmed the most suitable structure of 2D photonic crystals. Deep x-ray lithography technique was employed for create a very deep and precise template of PMMA. Then, liquid-phase deposition was used to faithfully deposit a tightly packed layer of titanium oxide onto the template. Finally, the template is selectively removed to obtain a photonic nano-structure. We also calculate photonic band gap on the 3D-structure of TiO2. A template for the most appropriate structure was fabricated by the method proposed by Yablonovitch. By using of the same method, it was successful to obtain 3D structure of TiO2. Refractive index of obtained TiO2 followed by heating at 700°C was determined to 2.5 which is close to that for anatase phase.


2010 ◽  
Vol 27 (7) ◽  
pp. 074205 ◽  
Author(s):  
Liu Yan-Ping ◽  
Yan Zhi-Jun ◽  
Li Zhi-Gang ◽  
Li Qin-Tao ◽  
Wang Yin-Yue

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