resonant optical parametric oscillator
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2022 ◽  
Vol 20 (2) ◽  
pp. 021403
Author(s):  
Miao Wang ◽  
Jian Ma ◽  
Tingting Lu ◽  
Shanjiang Hu ◽  
Xiaolei Zhu ◽  
...  

2021 ◽  
Author(s):  
Li Wang ◽  
Weidong Chen ◽  
André Schirrmacher ◽  
Edlef Büttner ◽  
Andrey A. Boyko ◽  
...  

2021 ◽  
Author(s):  
Han Rao ◽  
Christian Markus Dietrich ◽  
José Ricardo Cardoso de Andrade ◽  
Ayhan Demircan ◽  
Ihar Babushkin ◽  
...  

2020 ◽  
Vol 45 (20) ◽  
pp. 5644
Author(s):  
Christian M. Dietrich ◽  
Ihar Babushkin ◽  
José R. Cardoso de Andrade ◽  
Han Rao ◽  
Ayhan Demircan ◽  
...  

2020 ◽  
Vol 10 (8) ◽  
pp. 2698
Author(s):  
Dandan Nie ◽  
Jinxia Feng ◽  
Yuanji Li ◽  
Kuanshou Zhang

We demonstrated a two-color quantum correlation between the down-conversion beams with a telecommunication wavelength at 1.5 μm and mid-infrared wavelength at 3.3 μm generated by a singly resonant optical parametric oscillator (SRO) operated above the pump threshold with a magnesium-oxide doped periodically-poled lithium niobate crystal in the cavity. A maximum of 1.8 dB noise reduction of the intensity difference of the twin beams was measured at the analysis frequency of 5 MHz. Based on a theoretical model for the quantum correlation between the twin beams given by a semi-classical approach, the influence of the analysis frequency and pump parameter on the quantum correlation between the twin beams was discussed theoretically and experimentally. The quantum correlation between the twin beams was degraded at the analysis frequencies above 5 MHz due to the limitation of the bandwidth of SRO cavity and was degraded at the analysis frequencies below 5 MHz due to the excess intensity noise of the pump. The two-color quantum correlated twin beams at 1.5 and 3.3 μm have potential applications in high-precision measurements beyond the shot noise level.


2020 ◽  
Vol 238 ◽  
pp. 11003
Author(s):  
Safia Mohand Ousaid ◽  
Mahmoud Chakaroun ◽  
Kai-hsun Chang ◽  
Thierry Billeton ◽  
L-Han Peng ◽  
...  

In this work, we demonstrate that it is possible to obtain an optical parametric oscillator with a simultaneous amplification of multiple frequencies using only a nonlinear photonic crystal with highly polished end-faces, preventing the utilization of external cavity mirrors.


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