Second-harmonic generation from silicon nitride films

2012 ◽  
Author(s):  
Tingyin Ning ◽  
Henna Pietarinen ◽  
Outi Hyvärinen ◽  
Janne Simonen ◽  
Go"ry Genty ◽  
...  
2017 ◽  
Vol 42 (23) ◽  
pp. 5030 ◽  
Author(s):  
K. Koskinen ◽  
R. Czaplicki ◽  
A. Slablab ◽  
T. Ning ◽  
A. Hermans ◽  
...  

2012 ◽  
Vol 100 (16) ◽  
pp. 161902 ◽  
Author(s):  
Tingyin Ning ◽  
Henna Pietarinen ◽  
Outi Hyvärinen ◽  
Janne Simonen ◽  
Goëry Genty ◽  
...  

2012 ◽  
Vol 37 (20) ◽  
pp. 4269 ◽  
Author(s):  
Tingyin Ning ◽  
Henna Pietarinen ◽  
Outi Hyvärinen ◽  
Ravi Kumar ◽  
Tommi Kaplas ◽  
...  

2020 ◽  
Vol 45 (7) ◽  
pp. 1958 ◽  
Author(s):  
Edgars Nitiss ◽  
Ozan Yakar ◽  
Anton Stroganov ◽  
Camille-Sophie Brès

2020 ◽  
Author(s):  
Xiyuan Lu ◽  
Gregory Moille ◽  
Ashutosh Rao ◽  
Daron A. Westly ◽  
Kartik Srinivasan

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Claudio Castellan ◽  
Alessandro Trenti ◽  
Chiara Vecchi ◽  
Alessandro Marchesini ◽  
Mattia Mancinelli ◽  
...  

2015 ◽  
Vol 23 (24) ◽  
pp. 30695 ◽  
Author(s):  
Tingyin Ning ◽  
Chunlei Tan ◽  
Tapio Niemi ◽  
Martti Kauranen ◽  
Goëry Genty

2002 ◽  
Vol 81 (25) ◽  
pp. 4706-4708 ◽  
Author(s):  
S. Lettieri ◽  
S. Di Finizio ◽  
P. Maddalena ◽  
V. Ballarini ◽  
F. Giorgis

2022 ◽  
Author(s):  
Edgars Nitiss ◽  
Jianqi Hu ◽  
Anton Stroganov ◽  
Camille-Sophie Brès

AbstractQuasi-phase-matching has long been a widely used approach in nonlinear photonics, enabling efficient parametric frequency conversions such as second-harmonic generation. However, in silicon photonics the task remains challenging, as materials best suited for photonic integration lack second-order susceptibility (χ(2)), and means for achieving momentum conservation are limited. Here we present optically reconfigurable quasi-phase-matching in large-radius silicon nitride microresonators, resulting in up to 12.5-mW on-chip second-harmonic generated power and a conversion efficiency of 47.6% W−1. Most importantly, we show that such all-optical poling can occur unconstrained from intermodal phase-matching, leading to broadly tunable second-harmonic generation. We confirm the phenomenon by two-photon imaging of the inscribed χ(2) grating structures within the microresonators as well as by in situ tracking of both the pump and second-harmonic mode resonances during all-optical poling. These results unambiguously establish that the photogalvanic effect, responsible for all-optical poling, can overcome phase mismatch constraints, even in resonant systems.


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