The effects of noise amplification and soliton generation in anomalous dispersion regime of optical fibers

2004 ◽  
Author(s):  
Amirhossein H. Tehranchi ◽  
Nosratollah Granpayeh ◽  
Ebrahim Mortazy
Keyword(s):  
Optical Fibers ◽  
Anomalous Dispersion ◽  
Dispersion Regime ◽  
Noise Amplification ◽  
Soliton Generation

Observation of parametric noise amplification owing to modulation instability in anomalous dispersion regime

1995 ◽  
Vol 31 (13) ◽  
pp. 1088-1090 ◽  
Author(s):  
R.A. Saunders ◽  
R.E. Epworth ◽  
D. Garthe ◽  
W.S. Lee ◽  
B.L. Patel
Keyword(s):  
Modulation Instability ◽  
Anomalous Dispersion ◽  
Dispersion Regime ◽  
Parametric Noise ◽  
Noise Amplification

scholarly journals Dissipative Soliton Resonance in a Thulium-Doped All-Fiber Laser Operating at Large Anomalous Dispersion Regime

2018 ◽  
Vol 10 (5) ◽  
pp. 1-7 ◽  
Author(s):  
Baldemar Ibarra-Escamilla ◽  
Manuel Duran-Sanchez ◽  
Berenice Posada-Ramirez ◽  
Hector Santiago-Hernandez ◽  
Ricardo Ivan Alvarez-Tamayo ◽  
...  
Keyword(s):  
Fiber Laser ◽  
Anomalous Dispersion ◽  
Dissipative Soliton ◽  
Soliton Resonance ◽  
Dispersion Regime

Tunable wavelength conversion based on optofluidic infiltrated photonic crystal fibers

2019 ◽  
Vol 28 (01) ◽  
pp. 1950002 ◽  
Author(s):  
H. Pakarzadeh ◽  
R. Derakhshan ◽  
S. Hosseinabadi
Keyword(s):  
Photonic Crystal ◽  
Wavelength Conversion ◽  
Photonic Crystal Fibers ◽  
Wavelength Region ◽  
Anomalous Dispersion ◽  
Index Formula ◽  
Wavelength Shift ◽  
Dispersion Properties ◽  
Dispersion Regime ◽  
Crystal Fibers

In this paper, wavelength conversion based on optofluidic infiltration of photonic crystal fibers (PCFs) is investigated to achieve the suitable wavelength over wide tunable range. For this purpose, two designs of PCFs (the so-called PCF1 and PCF2) with appropriate dispersion properties are simulated, and wavelength conversion via four-wave mixing process for pump wavelengths in both normal and anomalous dispersion regimes is studied. By changing the refractive index [Formula: see text] of the optical fluid infiltrated into the PCF air-holes and then varying the fiber dispersion properties, the converted wavelength region can be tuned. The results show that for the pump wavelength in the normal dispersion regime, the PCF1 infiltrated with [Formula: see text] and PCF2 infiltrated with [Formula: see text] exhibit the maximum wavelength shift. Moreover, the wavelength shift is much higher than that obtained in the anomalous dispersion regime and it can be further increased by increasing the input pump power.

DARK SOLITONS IN OPTICAL FIBERS WITH HIGHER ORDER EFFECTS

2002 ◽  
Vol 11 (02) ◽  
pp. 197-204 ◽  
Author(s):  
K. NAKKEERAN
Keyword(s):  
Optical Fibers ◽  
Dark Soliton ◽  
Higher Order ◽  
Order Effects ◽  
Nonlinear Wave Propagation ◽  
Bilinear Method ◽  
Fiber System ◽  
Normal Dispersion ◽  
Dispersion Regime ◽  
Higher Order Effects

We consider the higher order nonlinear Schrödinger (HNLS) equation, which governs the nonlinear wave propagation in optical fibers with higher order effects. Lax pair associated with the integrable HNLS equation for the pulse propagation in normal dispersion regime of the fiber media is constructed with the help of Ablowitz–Kaup–Newell–Segur method. Using Hirota bilinear method, dark soliton solution is explicitly derived. Similar study is also carried out for simultaneous propagation of N nonlinear pulses in the normal dispersion regime of the fiber system with higher order effects.

Sub-100 kHz repetition rate erbium-doped fiber laser in anomalous dispersion regime

Laser Physics ◽  
2011 ◽  
Vol 21 (6) ◽  
pp. 1111-1114 ◽  
Author(s):  
J. L. Dong ◽  
Z. C. Luo ◽  
W. C. Xu ◽  
A. P. Luo ◽  
L. Y. Wang ◽  
...  
Keyword(s):  
Fiber Laser ◽  
Repetition Rate ◽  
Anomalous Dispersion ◽  
Dispersion Regime ◽  
Erbium Doped
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