Polarization beam splitter based on two-dimensional modified annular photonic crystals with square and triangular lattices

2018 ◽  
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Taymaz Fathollahi-Khalkhali ◽  
Mohammad Reza Moghadam
2004 ◽  
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Author(s):  
Chen Xi-Yao ◽  
Yao Pei-Jun ◽  
Chen Bo ◽  
Li Feng ◽  
Zhang Jiang-Ying ◽  
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2007 ◽  
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Zhang Jie ◽  
Zhao De-Yin ◽  
Zhou Chuan-Hong ◽  
Jiang Xun-Ya

2009 ◽  
Vol 29 (3) ◽  
pp. 818-821 ◽  
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孔伟金 Kong Weijin ◽  
云茂金 Yun Maojin ◽  
王美 Wang Mei ◽  
单福凯 Shan Fukai

2008 ◽  
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pp. 709-712 ◽  
Author(s):  
沈义峰 Yifeng Shen ◽  
孙建 Jian Sun ◽  
沈晓鹏 Xiaopeng Shen ◽  
王娟 Juan Wang ◽  
孙露露 Lulu Sun ◽  
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2007 ◽  
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Kui Han ◽  
Yifeng Shen ◽  
Haipeng Li ◽  
Yuxi Wu ◽  
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2004 ◽  
Vol 817 ◽  
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M. Galli ◽  
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AbstractWe report on a complete optical investigation on two-dimensional silicon-on-insulator (SOI) waveguide photonic crystals obtained by electron beam lithography and reactive ion etching. The dispersion of photonic modes is fully investigated both above and below the light-line by means of angle- and polarization-resolved micro-reflectance and attenuated total reflectance measurements.The investigated samples consisted in a) large area (300 × 300 μm2) two-dimensional (2D) triangular lattices of air holes containing repeated line–defects; b) small area triangular lattices of holes with different number of periods and /or line defects integrated in a ridge type waveguide structure.In the case of large area samples, variable-angle reflectance and ATR is measured from the sample surface in a wide spectral range from 0.2 to 2 eV both in TE and TM polarizations. The sharp resonances observed in the polarized reflectance and ATR spectra allow mapping of the photonic dispersion of both radiative and guided modes. Experimentally determined and compared to those calculated by means of an expansion on the basis of the waveguide modes.In the case of ridge type waveguide-integrated photonic crystals, transmission is measured in the 0.9-1.7 eV spectral range by an edge-coupling technique. Transmission spectra exhibit significant attenuation corresponding to the photonic gaps along the Γ–M and Γ–K directions respectively, even when a small number of hole periods is integrated in the ridge waveguide. Good agreement is obtained by comparing the measured transmission spectra with the calculated photonic bands.


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