Advances in Optical Amplifiers Part 1 pdf
... the threshold density N th = 1. 5 × 10 18 cm −3 , v g = 8.5 × 10 9 cm/s, optical confinement 10 Advances in Optical Amplifiers Part 1 Chapter 1 Chapter 2 Chapter 3 Part 2 Chapter 4 Chapter 5 Chapter ... February, 2 011 Printed in India A free online edition of this book is available at www.intechopen.com Additional hard copies can be obtained from orders@intechweb.o...
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... The 16 Advances in Optical Amplifiers Advances in Optical Amplifiers 40 ( ) ,0 22 2 () 1( ) (). m m TE TM s g gz Az A z E − = ++ (19 ) Referring to the coupled mode equations developed in ... ISSN 0 018 -9 219 Bányai, L. & Koch, S. W. (2005). Semiconductor Quantum Dots (Second Edition). World Scientific, ISBN 9 810 213 905, London, 22 Advances in Optical...
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... Jul. 19 99, pp. 11 66 -11 71, ISSN 0733-8724 Advances in Optical Amplifiers 358 Light incident on the boundary between two films encounters a refractive index discontinuity, causing partial ... the resulting signal wavelength range was between 14 90 and 16 11 nm. The 11 5 exiting channels from 15 14 to 16 06 nm are plotted as Curve a on Fig. 4. The pump powers, speci...
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Advances in Optical Amplifiers Part 3 doc
... by substituting (15 )- (19 ) and ( 21) -(25) in equations (5) and (6). () () () int int , ,', int ' int 1 4 exp( ' ) 1cos(('))exp 1 exp( ) 2 1 ' exp( ) exp( ) 1 cos( ( ' ... operating in the Advances in Optical Amplifiers 52 counter propagating mode, Proceedings of IEE Optoelectronics, Vol. 14 7, No. 1, pp. 49–55, Feb. 2000, Institu...
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Advances in Optical Amplifiers Part 4 potx
... Technol., vol. 7, pp. 11 18 11 24, July 19 89 J. Mark and J.Mork, “Sub-picosecond gain dynamics in InGaAsP optical amplifiers: Experiment and theory”, Appl. Phys. Lett., 61 , 22 81- 2283 (19 92) CIP white ... Mode Regenerator for Optical Burst Switching network transmission, IEEE Photon. Technol. Lett. , Vol. 19 , No. 22, 18 34 -18 36, 10 41- 113 5 Advances in Optical...
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Advances in Optical Amplifiers Part 5 pptx
... and lower sidebands around 1 ω with frequency span of 13 ω ω − and the optical field can be expressed as: {} 13 13 3 3 11 13 13 13 13 311 1 (2 ) (2 ) ( ) 13 13 1 E() ( )[( )exp ( ) ( )exp ... shown in Fig.5 as inset (ii). 15 40.0 15 42.5 15 45.0 15 47.5 15 50.0 15 52.5 -50 -40 -30 -20 -10 0 Optical power (dBm) Wavelength (nm) 1. 25nm/D Converted signal 17 d...
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Advances in Optical Amplifiers Part 6 pot
... -0.5 0.0 0.5 1. 0 0.0 01 0. 01 0 .1 1 10 Optimum Time Delay (ps) Detuning: 3 THz Input Pump Energy: 10 fJ 1. 7 pJ 5.8 pJ 11 pJ 15 pJ Input Probe Energy (pJ) Simulation -0.2 -0 .1 0.0 0 .1 0.2 0.3 0. 01 0 .1 1 10 Optimum ... -60 -50 -40 -30 -20 -10 0 0.0 01 0. 01 0 .1 1 10 FWM Conversion Effeciency (dB) Input Pump Energy: 15 pJ 11 pJ 5.8 pJ 1. 7 pJ 10 fJ Input Prob...
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Advances in Optical Amplifiers Part 7 pptx
... Amplifier Spectral Shift Effect in 40 Gb/s Optical Communication Systems 0, 01 0 ,1 1 10 -10 -5 0 5 10 15 20 25 : W s Gain (dB) (b) Optical filtering 0, 01 0 ,1 1 10 -200 -15 0 -10 0 -50 0 Phase (°) CPO ... Amplifiers Amplification (b) Total transfer functions 0 .1 1 10 -10 0 10 20 Sf W s Gain (dB) 0 .1 1 10 0 Phase (deg) M MS 0 .1 1 10 -10 0 10...
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Advances in Optical Amplifiers Part 8 docx
... Ω 2 −Ω 1 . −2Ω 2 −2Ω 1 −Ω 2 −Ω 1 0 Ω 1 Ω 2 2Ω 1 2Ω 2 Ω 1 +Ω 2 −Ω 1 −Ω 2 Ω 2 −Ω 1 Ω 1 −Ω 2 2Ω 2 −Ω 1 2Ω 1 −Ω 2 2(Ω 2 −Ω 1 ) 2(Ω 1 −Ω 2 ) −2Ω 1 +Ω 2 −2Ω 2 +Ω 1 k= 2n+2 2n +1 2n ( ) n+2 n +1 n n -1 ( ... 33, 12 , 10 83 -10 84, (19 97) Eskildsen, L. and P.B. Hansen, "Interferometric noise in lightwave systems with optical preamplifiers", Photonic...
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Advances in Optical Amplifiers Part 9 pptx
... random optical signals are transmitted. Wavelength G max G min PDG NF 15 30 nm 18 .3 dB 17 .7 dB 0.62 dB 8.3 dB 15 44 nm 16 .8 dB 16 .2 dB 0.63 dB 6 .1 dB 15 50 nm 17 .1 dB 16 .0 dB 0.68 dB 5 .1 dB 15 58 ... 7, 10 71- 10 81, (19 89) Onishchukov, G., V. Lokhnygin, A. Shipulin and P. Reidel, " ;10 Gbit/s transmission over 15 00km with semiconductor optical amplifie...
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