Acousto-optic cavity coupling in 2D phoxonic crystal with combined convex and concave holes

被引:6
|
作者
Jin, Jun [1 ,2 ]
Jiang, Shan [1 ,3 ]
Hu, Hongping [1 ,2 ]
Zhan, Lamin [4 ]
Wang, Xiaohong [4 ]
Laude, Vincent [5 ]
机构
[1] Huazhong Univ Sci & Technol, Sch Aerosp Engn, Dept Mech, Wuhan 430074, Peoples R China
[2] Huazhong Univ Sci & Technol, Hubei Key Lab Engn Struct Anal & Safety Assessmen, Wuhan 430074, Peoples R China
[3] Huazhong Univ Sci & Technol, State Key Lab Digital Mfg Equipment & Technol, Wuhan 430074, Peoples R China
[4] Huazhong Univ Sci & Technol, Sch Opt & Elect Informat, Wuhan 430074, Peoples R China
[5] Univ Bourgogne Franche Comte, CNRS, UMR 6174, Franche Comte Elect Mecan Therm & Opt, F-25030 Besancon, France
基金
中国国家自然科学基金;
关键词
STIMULATED BRILLOUIN-SCATTERING; PHONONIC BANDGAPS; SILICON; ENHANCEMENT; PHOTONS; LIGHT;
D O I
10.1063/5.0060412
中图分类号
O59 [应用物理学];
学科分类号
摘要
A two-dimensional cross-like phoxonic crystal (PxC) model is proposed, which exhibits simultaneously large complete photonic crystal (PtC) and phononic crystal (PnC) bandgaps. The most salient trait of the structure is the wide range of geometrical parameters compatible with large complete bandgaps. After geometrical optimization, photonic and phononic bandgaps with gap-to-midgap ratios of 11.5% and 90.7% are obtained, respectively. These values are close to the best topology-optimized reported values but are obtained with simple shapes compatible with nanoscale fabrication technology. These characteristics make the convex-concave topology a promising candidate for PxC devices. A cavity is then introduced by filling up one cross-like hole in the 7 x 7 super-cell. PtC and PnC bands with defects appear in the respective large complete bandgaps, confining phonons and photons in the same cavity. Acousto-optic (AO) coupling between photonic and phononic defect modes is further investigated by the finite element method, taking both photoelastic and moving interface mechanisms into consideration. The symmetries of both photonic and phononic modes play a dominant role in the coupling strength. Results show that the strongest linear coupling between a photonic transverse magnetic mode and phononic breathing mode is obtained due to the in-phase superposition in the x and y directions. A quadratic nonlinear coupling is observed when photonic modes are coupled with the phononic stretching mode due to the inverse superposition of x and y directions. Finally, the optomechanical coupling rates relative to zero-point motion are estimated.
引用
收藏
页数:15
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