Effects of laser diode parameters on power penalty in 10 Gb/s optical fiber transmission systems

A composite tradeoff study based on the influence of key laser diode parameters on frequency chirp induced power penalty, extinction induced power penalty, the turn-on delay, and the dispersion transmission limit is presented for 10 Gb/s optical fiber transmission systems. The simulated results reveal that an optimum range of differential gain and nonlinear gain coefficient exists, and it is advantageous to set an extinction ratio that minimizes both the total power penalty and the turn-on delay. In addition, it is shown that a reduction of chirp and maximization of the dispersion transmission limit can be realized by designing the laser diode with a linewidth enhancement factor near -0.8.

[1]  K. Hinton,et al.  Laser turn-on delay and chirp noise effects in Gb/s intensity-modulated direct-detection systems , 1995 .

[2]  T. J. Whitley,et al.  A review of recent system demonstrations incorporating 1.3-/spl mu/m praseodymium-doped fluoride fiber amplifiers , 1995 .

[3]  Richard E. Wagner,et al.  Chromatic dispersion limitations in coherent lightwave transmission systems , 1988 .

[4]  P. J. Corvini,et al.  Computer simulation of high-bit-rate optical fiber transmission using single-frequency lasers , 1987 .

[5]  Shu Yamamoto,et al.  Analysis of chirp power penalty in 1.55-µm DFB-LD high-speed optical fiber transmission systems , 1987 .

[6]  G P Agrawal,et al.  Effect of frequency chirping on the performance of optical communication systems. , 1986, Optics letters.

[7]  F. Koyama,et al.  Analysis of dynamic spectral width of dynamic-single-mode (DSM) lasers and related transmission bandwidth of single-mode fibers , 1985, IEEE Journal of Quantum Electronics.

[8]  Ivan P. Kaminow,et al.  High-frequency characteristics of directly modulated InGaAsP ridge waveguide and buried heterostructure lasers , 1984 .

[9]  J. J. O'Reilly Chirp-induced penalty in optical fibre systems , 1987 .

[10]  R. Olshansky,et al.  Frequency response of 1.3µm InGaAsP high speed semiconductor lasers , 1987 .

[11]  G. Agrawal Fiber‐Optic Communication Systems , 2021 .

[12]  Ian Francis Lealman,et al.  Effect of Zn doping on differential gain and damping of 1.55 mu m InGaAs/InGaAsP MWQ lasers , 1992 .

[13]  H. Hillmer,et al.  A tractable large-signal dynamic model-application to strongly coupled distributed feedback lasers , 1994 .

[14]  S. Murata,et al.  Strain effect on K factor, differential gain and nonlinear gain coefficient for InGaAs/InGaAsP strained multiquantum well lasers , 1993 .

[15]  K. Petermann,et al.  Turn-on jitter in zero-biased single-mode semiconductor lasers , 1996, IEEE Photonics Technology Letters.

[16]  Y. Terunuma,et al.  Low-noise Pr3+-doped fluoride fibre amplifier , 1995 .

[17]  T. Koch,et al.  Effect of nonlinear gain reduction on semiconductor laser wavelength chirping , 1986 .

[18]  Yutaka Miyamoto,et al.  10-Gb/s strained MQW DFB-LD transmitter module and superlattice APD receiver module using GaAs MESFET IC's , 1994 .