1989
DOI: 10.1007/bf02117685
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Fibre raman amplifier properties for applications to long-distance optical communications

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Cited by 21 publications
(5 citation statements)
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“…At first, the pumps transmit from the end point to the starting point of fiber without depletion due to signals but with attenuation and depletion due to pump interaction. Then the attenuated pumps transmit together with signals to the end point according to (2) and transfer power to signal 12] . In this paper, Simulated annealing algorithm is adopted to give automatic pump power configuration in multiwave backward-pumped dispersion compensation FRA.…”
Section: Theory Model and Design Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…At first, the pumps transmit from the end point to the starting point of fiber without depletion due to signals but with attenuation and depletion due to pump interaction. Then the attenuated pumps transmit together with signals to the end point according to (2) and transfer power to signal 12] . In this paper, Simulated annealing algorithm is adopted to give automatic pump power configuration in multiwave backward-pumped dispersion compensation FRA.…”
Section: Theory Model and Design Methodsmentioning
confidence: 99%
“…Development in transmission fiber now provides an applicable low-loss window from 1.2-1.7µm, but no suitable rare earth-doped fiber amplifiers have been developed which can continuously cover this practically 70Thz range [1] .Distributed Fiber Raman Amplifier using the transmission line as a Raman gain medium is a promising technology available for the long haul communication systems [2][3] . Now high-power fiber lasers that can satisfy the demand of the high-pumps for FRA have become commercially available, and fiber Raman amplifiers are recently attracting much attention due to wider amplification bandwidth, flexible center wavelength, and low noise performance [4][5][6][7][8] .…”
Section: Introductionmentioning
confidence: 99%
“…This is readily confirmed by substituting eqn (6) into a nonlinear relation (2). This substitution yields P(t) = x 0 E 0 cos mt + x 1 E 0 2 co.s 2 mt+ x 2 £ 0 3 cos 3 mt+ ... (8) which can be transformed to the format. P(t) = P 0 + P 1 cosmt + P 2 cos2mt+ P 3 cos3mt+ ... where P 0 = 112 x 0 E 0 2 P(t) = z 0 E 0 + 3/4 z 2 EQ 3 p2 = l/2 X1 Eo 2 P3 = l/4 X2 Eo 3 (9) (lOa)…”
Section: Second Order and Third Order Nonlinear Mediummentioning
confidence: 95%
“…It has also been shown that the optical signal-to-noise ratio (OSNR) and transmission distance can be improved significantly by employing a remotely pumped EDF installed in a transmission span [10][11][12]. Furthermore, it has been shown theoretically that DRA or distributed optical amplification yields a higher OSNR than discrete amplification, which is realized by optical amplifiers such as EDFAs [13][14]. Then, a number of transmission experiments were undertaken using distributed EDFAs [15][16][17].…”
Section: Introductionmentioning
confidence: 99%