Rayleigh backscattering and amplified spontaneous emission in high-power ytterbium-doped fiber amplifiers

1999 ◽  
Vol 16 (5) ◽  
pp. 695 ◽  
Author(s):  
Ram Oron ◽  
Amos A. Hardy
Keyword(s):  
Spontaneous Emission ◽  
High Power ◽  
Amplified Spontaneous Emission ◽  
Fiber Amplifiers ◽  
Rayleigh Backscattering

Suppressing Amplified Spontaneous Emission in High-Power Pulsed Er-Yb Codoped Fiber Amplifiers

2012 ◽  
Vol 39 (10) ◽  
pp. 1002004
Author(s):  
何洋 He Yang ◽  
韩群 Han Qun ◽  
宁继平 Ning Jiping ◽  
盛朝霞 Sheng Zhaoxia ◽  
任坤 Ren Kun
Keyword(s):  
Spontaneous Emission ◽  
High Power ◽  
Amplified Spontaneous Emission ◽  
Fiber Amplifiers

Signal Wavelength Effect on Overmodulation in Thulium Doped Fiber Amplifiers with Amplified Spontaneous Emission: A Simulink Pedestal

2018 ◽  
Vol 0 (0) ◽  
Author(s):  
Mohd Mansoor Khan ◽  
Ramesh Kumar Sonkar
Keyword(s):  
Spontaneous Emission ◽  
Transfer Functions ◽  
Optical Fiber Communication ◽  
Amplified Spontaneous Emission ◽  
Fiber Amplifiers ◽  
Corner Frequency ◽  
Optimum Operating ◽  
Test Bed ◽  
Signal Wavelength ◽  
Communication Signal

AbstractThulium-doped fiber amplifiers (TDFAs) can provide high power optical amplification in the wavelength range of 1,460–1,545 nm (S and near-C bands). They can be employed for dense wavelength division multiplexing (DWDM) in optical fiber communication over a broad range, unlike the Erbium-doped fiber amplifiers (EDFAs), which are active in the C-band only in the conventional “erbium window.” Line service surveillance and management of digital optical information in DWDM TDFA networks can be done by low-frequency amplitude modulation (~100 kHz) of TDFA pump and communication signal, termed as overmodulation. Governing equations for overmodulation gain dynamics in TDFAs using the Bononi and Rusch (1998) model was first derived in a companion paper (2017). The research provides a methodical test bed analysis using MatLab Simulink model with a different outlook in the respective field. The transfer functions for signal-to-signal and signal-to-amplified spontaneous emission were implemented to develop a simulator. An undesirable 30 % increment in the output modulation index at 8 dBm and 1,490 nm were obtained by simulating overmodulation sensitivity at different levels of mean input signal power and signal wavelength respectively at corner frequency. The optimum operating wavelength for TDFAs obtained was 1,490 nm.

High power amplified spontaneous emission from an oligomer in solution

2015 ◽  
Vol 168 ◽  
pp. 109-113 ◽  
Author(s):  
Saradh Prasad ◽  
K.H. Ibnaouf ◽  
M.S. AlSalhi ◽  
D. Devaraj ◽  
V. Masilamani
Keyword(s):  
Spontaneous Emission ◽  
High Power ◽  
Amplified Spontaneous Emission

80 nm spectrally flattened, high power erbium amplified spontaneous emission fibre source

2000 ◽  
Vol 36 (15) ◽  
pp. 1263 ◽  
Author(s):  
R.P. Espindola ◽  
G. Ales ◽  
J. Park ◽  
T.A. Strasser
Keyword(s):  
Spontaneous Emission ◽  
High Power ◽  
Amplified Spontaneous Emission

Research Progress on Amplified Spontaneous Emission Suppression in Pulsed Fiber Amplifiers

2017 ◽  
Vol 54 (2) ◽  
pp. 020004
Author(s):  
罗亿 Luo Yi ◽  
王小林 Wang Xiaolin ◽  
粟荣涛 Su Rongtao ◽  
张汉伟 Zhang Hanwei ◽  
周朴 Zhou Pu ◽  
...  
Keyword(s):  
Spontaneous Emission ◽  
Amplified Spontaneous Emission ◽  
Fiber Amplifiers ◽  
Research Progress

Amplified spontaneous emission and power amplification in high-power DF laser systems

2010 ◽  
Vol 8 (8) ◽  
pp. 764-767 ◽  
Author(s):  
陈星 Xing Chen ◽  
刘文广 Wenguang Liu ◽  
姜宗福 Zongfu Jiang
Keyword(s):  
Spontaneous Emission ◽  
High Power ◽  
Amplified Spontaneous Emission ◽  
Power Amplification ◽  
Laser Systems
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