Download PDF by Cox III C.H.: Analog optical links

By Cox III C.H.

ISBN-10: 0521621631

ISBN-13: 9780521621632

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In this case a second wavelength dependence comes into play, in addition to the one just discussed. The shorter wavelength permits a smaller single mode optical waveguide, thereby permitting a narrower gap between the modulation electrodes and consequently increasing the electrical field across the optical waveguide. This effect scales approximately inversely as wavelength. Consequently for two modulators, each of which was optimized for a different wavelength, smz scales as approximately λ−2 .

1990. Lightwave subcarrier CATV transmission systems, IEEE Trans. , 38, 524–33. Desurvire, E. 1994. Erbium-Doped Fiber Amplifiers, New York: Wiley. Gowar, J. 1983. 1. , Miyazawa, H. and Mitomi, O. 1994. 75 GHz broadband Ti:LiNbO3 optical modulator with ridge structure, Electron. , 30, 949–51. , Lanzisera, V. A. and Hill, P. M. 1989. Subcarrier multiplexed lightwave systems for broad band distribution, J. , 7, 1329–42. O’Mahony, M. 1988. Semiconductor laser optical amplifiers for use in future fiber systems, J.

0001 to 1 W/V. The values of smz corresponding to these ratios of PI /Vπ are plotted in Fig. 10, along with some experimentally reported values. 2 Modulation devices 41 The corresponding bandwidths for each of the devices in Fig. 10 are presented in Chapter 4. In addition to data on Mach–Zehnder modulators, Fig. 3, respectively. In comparing Figs. 10, we see that both in theory and in practice it is presently possible to achieve higher slope efficiencies with a MZM fed by a high power laser than it is with direct modulation of a diode laser.

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Analog optical links by Cox III C.H.

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