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Long span fiber amplifiers

Applied Optics, 1990
We examine the theory of optical amplification in long span single-mode fibers which have low levels of erbium dopant. When pumped from the transmitter end at a suitable wavelength, lightly doped fibers can form a distributed amplifier, capable of overcoming transmission losses due to the intrinsic attenuation of the host glass at the signal wavelength.
P, Urquhart, T J, Whitley
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Optical fiber amplifiers

SPIE Proceedings, 1991
Recent progress on an erbium-doped optical fiber amplifier (EDFA) pumped with a 0.98 micron laser diode is reported. An erbium-doped fiber with a very high gain coefficient of 11.0 dB/mW has been achieved using an extended VAD method. A high power 0.98 micron laser diode with a strained-layer InGaAs quantum well laser structure has been developed as ...
Tetsuhiko Ikegami, Motohiro Nakahara
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Broadband Fiber Optic Amplifiers

Optical Fiber Communication Conference and International Conference on Quantum Information, 2001
Broadband fiber optic amplifiers are key elements of DWDM systems and enablers for optical networks. New amplifier technologies for extending gain-bandwidth and equalizing the power deviation among WDM signals are discussed toward the next generation of ultra.-high-capacity DWDM systems.
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Integrated ytterbium-Raman fiber amplifier

Optics Letters, 2014
An integrated ytterbium-Raman fiber amplifier architecture is proposed for power scaling of a Raman fiber laser. It is an ytterbium (Yb) fiber amplifier seeded with a double or multiple wavelength laser and followed by a passive Raman fiber. The bluest wavelength light gets amplified in the Yb fiber and the power is transferred to redder wavelengths in
Lei, Zhang   +3 more
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Amplifier/compressor fiber Raman lasers

Annual Meeting Optical Society of America, 1987
When pump and Stokes pulses copropagate in a fiber Raman laser (FRL), the weaker Stokes spectrum is severely broadened through pump-induced cross-phase modulation (XPM).1 Thus, in an FRL during Raman amplification, the pulse is chirped through XPM, and then the linear anomalous dispersion of a fiber can compress the pulse.
M N, Islam   +4 more
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Broadband fiber optical parametric amplifiers

Optics Letters, 1996
The bandwidth of a single-pump fiber optical parametric amplifier is governed by the even orders of fiber dispersion at the pump wavelength. The amplifier can exhibit gain over a wide wavelength range when operated near the fiber's zero-dispersion wavelength. It can also be used for broadband wavelength conversion,with gain.
M E, Marhic   +3 more
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All-Fiber Nanosecond Pulse Fiber Amplifier

International Summer Session: Lasers and Their Applications, 2011
A nanosecond pulse is realized through just one stage amplifier, which has 10.10W in average power, 1064nm wavelength, 11kHz in repetition frequency, 150ns in impulse duration, 0.9mJ in single pulse power, 6kW in peak power. The optic-optic conversion efficiency is 67%.
Feng Yu   +5 more
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Theoretical investigation on Raman Fiber Amplifiers

Asia Communications and Photonics Conference and Exhibition, 2010
The characterization of RFAs with bi-directional Raman pumped or co-propagating Raman pumped is studied. The effection to RFAs for pump power, initial signal power and fiber length is analyzed, which is to optimize and improve gain of RFASSs, so as to improve the performance of the amplifier.
Shuhua Li   +3 more
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Raman fiber amplifiers

Optical Amplifiers and their Applications, 1999
A brief history, state ofthe art and main tendencies in development and application ofRaman fiber amplifiers are discussed.
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Erbium-doped Fiber Amplifier

Proceedings of Japan International Electronic Manufacturing Technology Symposium, 2005
Erbium-doped fiber amplifiers(EDFAs) are remarkable technology as direct optical amplification devices. It has been recently demonstrated that the EDFA can be practically applicable to optical trunk transmission systems and optical distribution systems.
T. Kakinuma, S. Shikii
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