Silicon waveguide TE0/TE1 mode conversion Bragg grating for constituting a resonator device

Author(s):  
Hideaki Okayama ◽  
Yosuke Onawa ◽  
Daisuke Shimura ◽  
Hiroki Yaegashi ◽  
Hironori Sasaki
Photonics ◽  
2021 ◽  
Vol 8 (3) ◽  
pp. 87
Author(s):  
Peihong Guan ◽  
Min Tang ◽  
Min Cao ◽  
Yuean Mi ◽  
Mei Liu ◽  
...  

The transverse asymmetry of the index modulation profile in the asymmetric few-mode fiber Bragg grating (FM-FBG) was investigated. The transverse asymmetry of the index modulation profile will lead to mode conversion between modes with the different azimuthal orders, and this asymmetry is characterized by the attenuation coefficient α. We evaluated that the value of attenuation coefficient α was 0.2 μm−1, and grating amplitude χ was 2.8 × 10−4 for FM-FBG inscribed by UV single-side illumination. We found that the optimized value of α was 0.16 μm−1, at which the maximum mode conversion efficiency of LP01–LP11 can be achieved. The results of this paper provide great potential application in few-mode fiber (FMF) devices and mode division multiplexing (MDM) optical communication.


2018 ◽  
Vol 32 (22) ◽  
pp. 1850258 ◽  
Author(s):  
Wenlong Liu ◽  
Xuebin Liu ◽  
Qiangqiang Yan ◽  
Simiao Qiang ◽  
Haifeng Pi ◽  
...  

Breaking Lorentz reciprocity is one necessary condition of optical isolator design. Unidirectional wavelength-mode conversion will be realized in a time-dependent system through a short operating range. Based on plasma dispersion effect, generate space-asymmetric periodical time-space modulation on silicon waveguide, and non-reciprocal propagation is realized in the waveguide. The designed unidirectional wavelength-mode conversion waveguide demonstrated that in the forward direction, input 1.55 [Formula: see text]m fundamental mode light signal and then output 1.5492 [Formula: see text]m is of 1st-order mode, while in the backward direction, input 1.5492 [Formula: see text]m is of 1st-order mode light signal and then output 1.5484 [Formula: see text]m is of fundamental mode. Based on this non-reciprocal structure, mode conversion waveguide and two-ring resonance filters were designed then, to accomplish on-chip optical isolation. The scale of the designed isolator is 160 [Formula: see text]m × 60 [Formula: see text]m, and the isolation is 21 dB, revealing perfect application potential.


2017 ◽  
Vol 42 (11) ◽  
pp. 2142 ◽  
Author(s):  
Hideaki Okayama ◽  
Yosuke Onawa ◽  
Daisuke Shimura ◽  
Hiroki Yaegashi ◽  
Hironori Sasaki

2016 ◽  
Vol 55 (8) ◽  
pp. 082202 ◽  
Author(s):  
Hideaki Okayama ◽  
Yosuke Onawa ◽  
Daisuke Shimura ◽  
Hiroki Yaegashi ◽  
Hironori Sasaki

Author(s):  
Pao Tai Lin ◽  
Vivek Singh ◽  
Yan Cai ◽  
Lin Zhang ◽  
Neil Sunil Patel ◽  
...  

2008 ◽  
Author(s):  
Jacob B. Khurgin ◽  
Marcel W. Pruessner ◽  
Todd H. Stievater ◽  
William S. Rabinovich

2018 ◽  
Vol 410 ◽  
pp. 930-935 ◽  
Author(s):  
Yuean Mi ◽  
Guobin Ren ◽  
Yixiao Gao ◽  
Haisu Li ◽  
Bofeng Zhu ◽  
...  

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