Measurements of Slow Light Effects in Silicon Photonics Resonators Based on 1D Photonic Crystal

Author(s):  
Damian Goldring ◽  
Uriel Levy ◽  
David Mendlovic
2014 ◽  
Vol 7 (3) ◽  
pp. 376-384 ◽  
Author(s):  
Charles Caer ◽  
Xavier Le Roux ◽  
Samuel Serna ◽  
Weiwei Zhang ◽  
Laurent Vivien ◽  
...  

2015 ◽  
Author(s):  
Yosuke Hinakura ◽  
Yosuke Terada ◽  
Takuya Tamura ◽  
Toshihiko Baba

Author(s):  
Weiqi Xue ◽  
Yi Yu ◽  
Luisa Ottaviano ◽  
Elizaveta Semenova ◽  
Kresten Yvind ◽  
...  

2020 ◽  
Vol 28 (12) ◽  
pp. 17286 ◽  
Author(s):  
Jie You ◽  
Zilong Tao ◽  
Yukun Luo ◽  
Jie Yang ◽  
Jianghua Zhang ◽  
...  

Author(s):  
Y. Cao ◽  
R. Hudgins ◽  
T.J. Suleski ◽  
M. A. Fiddy ◽  
J. Raquet ◽  
...  

Nanophotonics ◽  
2016 ◽  
Vol 5 (3) ◽  
pp. 440-455 ◽  
Author(s):  
Nobuyuki Matsuda ◽  
Hiroki Takesue

AbstractIntegrated quantum photonics is now seen as one of the promising approaches to realize scalable quantum information systems. With optical waveguides based on silicon photonics technologies, we can realize quantum optical circuits with a higher degree of integration than with silica waveguides. In addition, thanks to the large nonlinearity observed in silicon nanophotonic waveguides, we can implement active components such as entangled photon sources on a chip. In this paper, we report recent progress in integrated quantum photonic circuits based on silicon photonics. We review our work on correlated and entangled photon-pair sources on silicon chips, using nanoscale silicon waveguides and silicon photonic crystal waveguides. We also describe an on-chip quantum buffer realized using the slow-light effect in a silicon photonic crystal waveguide. As an approach to combine the merits of different waveguide platforms, a hybrid quantum circuit that integrates a silicon-based photon-pair source and a silica-based arrayed waveguide grating is also presented.


2013 ◽  
Vol 278-280 ◽  
pp. 1047-1050
Author(s):  
Qing Xia ◽  
Hui Chen

Encoder with a hexagonal lattice photonic crystal was performed by OCDMA simulation model. Filtering of photonic crystal cavity was used for encoding in spectral domain, and the distance between the dot defects was used for encoding in time domain because of its slow light effects caused by dispersion, whose time delay reached orders of ns magnitude. According to the simulation, the BER of OCDMA system with PC encoder is 10-23, while BER is 10-18 in the system with FBG encoder. By contrast, it is indicated that PC encoder requires strict demands on its own structure. With mismatching of encoder and decoder in receiving terminal, BER decrease to 10-7, and the performance of OCDMA system is serious affected.


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