Comparison of Raman and degenerated optical parametric oscillators for a high‐energy and high‐repetition‐rate eye‐safe laser

1996 ◽  
Vol 35 (12) ◽  
pp. 3579 ◽  
Author(s):  
Gilles Roy
Keyword(s):  
Repetition Rate ◽  
High Energy ◽  
High Repetition Rate ◽  
Optical Parametric Oscillators ◽  
Parametric Oscillators ◽  
High Repetition ◽  
Optical Parametric

Compact, efficient and widely tunable 2-μm high-repetition-rate optical parametric oscillators

2018 ◽  
Vol 426 ◽  
pp. 119-125 ◽  
Author(s):  
Jialin Mei ◽  
Kai Zhong ◽  
Yang Liu ◽  
Jie Shi ◽  
Hongzhan Qiao ◽  
...  
Keyword(s):  
Repetition Rate ◽  
High Repetition Rate ◽  
Optical Parametric Oscillators ◽  
Parametric Oscillators ◽  
High Repetition ◽  
Optical Parametric

Management of thermal effects in high-repetition-rate pulsed optical parametric oscillators

2010 ◽  
Vol 35 (21) ◽  
pp. 3667 ◽  
Author(s):  
Antoine Godard ◽  
Myriam Raybaut ◽  
Thomas Schmid ◽  
Michel Lefebvre ◽  
Anne-Marie Michel ◽  
...  
Keyword(s):  
Repetition Rate ◽  
Thermal Effects ◽  
High Repetition Rate ◽  
Optical Parametric Oscillators ◽  
Parametric Oscillators ◽  
High Repetition ◽  
Optical Parametric

scholarly journals Modelling Dispersion Compensation in a Cascaded-Fiber-Feedback Optical Parametric Oscillator

Optics ◽  
2021 ◽  
Vol 2 (2) ◽  
pp. 96-102
Author(s):  
Ewan Allan ◽  
Craig Ballantine ◽  
Sebastian C. Robarts ◽  
David Bajek ◽  
Richard A. McCracken
Keyword(s):  
Pulse Propagation ◽  
Dispersion Compensation ◽  
Numerical Aperture ◽  
Tunable Laser ◽  
High Energy ◽  
Order Effects ◽  
Optical Parametric Oscillators ◽  
Fiber System ◽  
Parametric Oscillators ◽  
Optical Parametric

Fiber-feedback optical parametric oscillators (OPOs) incorporate intracavity fibers to provide a compact high-energy wavelength-tunable laser platform; however, dispersive effects can limit operation to the sub-picosecond regime. In this research article, we modeled pulse propagation through systems of cascaded fibers, incorporating SMF-28 and ultra-high numerical aperture (UHNA) fibers with complementary second-order dispersion coefficients. We found that the pulse duration upon exiting the fiber system is dominated by uncompensated third-order effects, with UHNA7 presenting the best opportunity to realise a cascaded-fiber-feedback OPO.

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