Abstract

The theory of pulse distortion in single-mode fibers is extended to include laser sources that suffer a linear wavelength sweep (chirp) during the duration of the pulse. The transmitted pulse is expressed as a Fourier integral whose spectral function is given by an analytical expression in closed form. The rms width of the transmitted pulse is also expressed in closed form. Numerical examples illustrate the influence of the chirp on the shape and rms width of the pulse. A somewhat paradoxical situation exists. A given input pulse can be made arbitrarily short by a sufficiently large amount of chirping, and, after a given fiber length, this chirped pulse returns to its original width. But at this particular distance an unchirped pulse would be only $\sqrt{2}$ times longer. Thus chirping can improve the rate of data transmission by only 40%.

© 1981 Optical Society of America

Pulse distortion in single-mode fibers. Part 2

D. Marcuse
Appl. Opt. 20(17) 2969-2974 (1981)

Pulse distortion in single-mode fibers

D. Marcuse
Appl. Opt. 19(10) 1653-1660 (1980)

Equalization of dispersion in single-mode fibers

D. Marcuse
Appl. Opt. 20(4) 696-700 (1981)

Pulse distortion in optical fibers with transverse offset splices

L. Bjerkan and H. Nordby
Appl. Opt. 20(3) 435-439 (1981)

Propagation of pulse fluctuations in single-mode fibers

D. Marcuse
Appl. Opt. 19(11) 1856-1861 (1980)