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Enhanced visible light generation in an active microcavity via third-harmonic conversion beyond the non-depletion approximation

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成果类型:
期刊论文
作者:
Yu, Rong*;Ding, Chunling;Wang, Jiangpeng;Zhang, Duo
通讯作者:
Yu, Rong
作者机构:
[Yu, Rong; Ding, Chunling] Wuhan Inst Technol, Sch Sci, Wuhan 430205, Hubei, Peoples R China.
[Wang, Jiangpeng] Huazhong Univ Sci & Technol, Sch Phys, Wuhan 430074, Hubei, Peoples R China.
[Zhang, Duo] Wuhan Polytech Univ, Sch Elect & Elect Engn, Wuhan 430023, Hubei, Peoples R China.
通讯机构:
[Yu, Rong] W
Wuhan Inst Technol, Sch Sci, Wuhan 430205, Hubei, Peoples R China.
语种:
英文
关键词:
Differential equations;Efficiency;Equations of motion;Light;Microcavities;Power transmission;Resonators;Spectrum analysis;Analytical expressions;Depletion approximation;Heisenberg-Langevin equations;High conversion efficiency;State-of-the-art technology;Telecommunication wavelengths;Third-order non-linearity;Three orders of magnitude;Harmonic generation
期刊:
Journal of Applied Physics
ISSN:
0021-8979
年:
2017
卷:
122
期:
24
页码:
244303
基金类别:
We gratefully acknowledge useful advice and fruitful discussion with Professor Xiaoxue Yang and Jiahua Li during the manuscript preparation. In the present research, R.Y. is supported by the National Natural Science Foundation of China under Grant No. 11505131. C.D. is supported by the National Natural Science Foundation of China under Grants No. 11705131 and No. U1504111. J.W. is supported in part by the National Natural Science Foundation of China under Grants No. 11675058 and the National Key Research and Development Program of China under Grant No. 2016YFA0301200. D.Z. is supported by the National Natural Science Foundation of China under Grant No. 11404250.
机构署名:
本校为其他机构
院系归属:
电气与电子工程学院
摘要:
We explore the possibility of using an active doubly resonant microtoroid resonator to produce high-efficiency third-harmonic generation (THG) by exploiting optical third-order nonlinearity. In a microresonator, the active fundamental mode is coherently driven with a continuous-wave input laser at the telecommunication wavelength (1550 nm), and then, the visible THG signal (517 nm) is monitored via an individual bus waveguide. We thoroughly compare our results with those obtained from the conventional passive (i.e., loss) microtoroid resonator ...

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