scholarly journals Four wave-mixing in a microstrip kinetic inductance travelling wave parametric amplifier

2020 ◽  
Vol 116 (15) ◽  
pp. 152602
Author(s):  
Samuel Goldstein ◽  
Naftali Kirsh ◽  
Elisha Svetitsky ◽  
Yuval Zamir ◽  
Ori Hachmo ◽  
...  
Keyword(s):  
Four Wave Mixing ◽  
Travelling Wave ◽  
Parametric Amplifier ◽  
Kinetic Inductance ◽  
Wave Mixing

Broadband optical parametric amplifier formed by two pairs of adjacent four-wave mixing sidebands in a tellurite microstructured optical fibre

2016 ◽  
Vol 18 (5) ◽  
pp. 055502 ◽  
Author(s):  
Lei Zhang ◽  
Tong-Hoang Tuan ◽  
Harutaka Kawamura ◽  
Kenshiro Nagasaka ◽  
Takenobu Suzuki ◽  
...  
Keyword(s):  
Optical Fibre ◽  
Four Wave Mixing ◽  
Parametric Amplifier ◽  
Optical Parametric Amplifier ◽  
Wave Mixing ◽  
Optical Parametric

Four-wave mixing in travelling-wave semiconductor laser amplifier

1989 ◽  
Vol 25 (4) ◽  
pp. 272 ◽  
Author(s):  
F. Favre ◽  
D. LeGuen ◽  
J.-C. Simon ◽  
P. Doussiere
Keyword(s):  
Semiconductor Laser ◽  
Four Wave Mixing ◽  
Travelling Wave ◽  
Wave Mixing ◽  
Laser Amplifier ◽  
Semiconductor Laser Amplifier

Experimental realization of a feedback optical parametric amplifier with four-wave mixing

2018 ◽  
Vol 97 (16) ◽  
Author(s):  
Xiaozhou Pan ◽  
Hui Chen ◽  
Tianxiang Wei ◽  
Jun Zhang ◽  
Alberto M. Marino ◽  
...  
Keyword(s):  
Four Wave Mixing ◽  
Parametric Amplifier ◽  
Optical Parametric Amplifier ◽  
Wave Mixing ◽  
Experimental Realization ◽  
Optical Parametric

Broadband wavelength conversion with amplification by four-wave mixing in semiconductor travelling-wave amplifiers

1994 ◽  
Vol 30 (11) ◽  
pp. 859 ◽  
Author(s):  
J. Zhou ◽  
N. Park ◽  
K.J. Vahala ◽  
M.A. Newkirk ◽  
B.I. Miller
Keyword(s):  
Wavelength Conversion ◽  
Four Wave Mixing ◽  
Travelling Wave ◽  
Wave Mixing

Near-degenerate cascaded four-wave mixing in an optical parametric amplifier

1997 ◽  
Vol 22 (21) ◽  
pp. 1603 ◽  
Author(s):  
A. Varanavičius ◽  
A. Dubietis ◽  
A. Beržanskis ◽  
R. Danielius ◽  
A. Piskarskas
Keyword(s):  
Four Wave Mixing ◽  
Parametric Amplifier ◽  
Optical Parametric Amplifier ◽  
Wave Mixing ◽  
Optical Parametric

Kerr-Gated Generation of Few-Cycle Mid-IR Pulses in a Four-Wave Mixing Parametric Amplifier

2014 ◽  
Author(s):  
T. Flöry ◽  
P. Malevich ◽  
A. Pugžlys ◽  
A. Voronin ◽  
A.M. Zheltikov ◽  
...  
Keyword(s):  
Four Wave Mixing ◽  
Parametric Amplifier ◽  
Wave Mixing

scholarly journals Investigation Of Dual-Pump Fiber Optical Parametric Amplifier Performance Driven by Energy Transfer Between Four-Wave Mixing Process

2021 ◽  
Vol 90 (1) ◽  
pp. 52-63
Author(s):  
K. G. Tay ◽  
Noran Azizan Cholan ◽  
Nurul Anati Othman
Keyword(s):  
Fiber Length ◽  
Four Wave Mixing ◽  
Parametric Amplifier ◽  
Optical Parametric Amplifier ◽  
Wave Mixing ◽  
Amplitude Equations ◽  
Central Wavelength ◽  
Optical Parametric ◽  
Fiber Optical ◽  
Fiber Optical Parametric Amplifier

Fiber optical parametric amplifier (FOPA) is operated based on energy transfer from pump waves to signal wave and at the end of the fiber, an idler wave is generated. This process is called four-wave mixing (FWM). Even though effects of higher-order dispersion coefficients, fiber length, fiber nonlinearity, fiber attenuation, pump powers, pump wavelength separation and distance of central pump wavelength with ZDW on gain profiles have been examined by previous researchers, but on different fiber or numerically studied using the Optisys system, analytical model or different amplitude equations. Thus, in this study, the above-mentioned parameters on the gain performance of dual pump fiber optical parametric amplifier (FOPA) using highly nonlinear shifted fiber (HNL-DSF) as a medium will be numerically investigated using ode45 function in Matlab. The gain at a certain wavelength can be obtained by solving 4 coupled amplitude equations with fiber loss and pump depletion that govern the four-wave mixing (FWM) process of pumps, signal and idler waves. Simulations results indicate positive gives poor or no gain, meanwhile, an addition of to negative widens the bandwidth, but there is no significant effect with the addition of . Besides, an increase of fiber length, nonlinearity and pump powers improve gain performance, but an increase of fiber loss decays the gain amplitude. Increment of pump separation will enhance flatness of gain at wavelength far from central wavelength but results in an increase of gain reduction at the central wavelength. Lastly, must be positive, not too small and not bigger than 1.125nm to get a high, broader and lesser ripples gain.

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