By Cox III C.H.
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1994 H. , 1992 T. , 1995 R. , 1992 L. , 1991 Y. , 1997 J. , 1994 S. 8 3 10 12 12 13 18 20 20 22 28 30 33 40 form of impedance matching between the modulation source and the laser to satisfy the definition of available power. A simple, but as we will see inefficient, way to implement the impedance match is to add a resistor, RMATCH , in series with the laser. The value of this resistor is chosen such that RS = RL + RMATCH . Putting all the foregoing together results in the circuit shown in Fig.
And Bender, K. 1994. Low-bias-current direct modulation up to 33 GHz in InGaAs/GaAs/AlGaAs pseudomorphic MQW ridge-waveguide devices, IEEE Photon. Technol. , 6, 1076–9. Seeds, A. J. 1996. Optical transmission of microwaves. In Review of Radio Science 1993–1996, ed. W. Ross Stone, Oxford: Oxford University Press, Chapter 14. Taylor, J. H. and Yates, H. W. 1957. Atmospheric transmission in the infrared, J. Opt. Soc. , 47, 223–6. Uitjens, A. G. W. and Kater, H. E. 1977. Receivers. In Electronics Designers’ Handbook, 2nd edition, ed.
There are any number of bias voltages we could choose, depending on the link parameter we are trying to maximize. In this discussion, let us assume that we are interested in the maximum incremental modulation efficiency. 12) with respect to VM and solving for the value of VM that maximizes the result. 13). e. 13) as well. These substitutions yield a relationship between the small-signal modulation voltage and the resulting intensity modulated optical power: π vm TFF PI pm,o ∼ . 14) This is half of what we need to express the incremental modulation efficiency.
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