Fiber Optic Essentials

Chapter 7 - Pulse Dispersion in Single-Mode Optical Fibers

7.1   INTRODUCTION

As discussed in Chapter 6, pulse dispersion arises due primarily to:

  • Ray dispersion, which is caused by the fact that different rays take different
    times to propagate (along different paths) from the input end to the output end
    of the fiber; this is also known as intermodal dispersion.
  • Material dispersion, which is caused by the fact that the refractive index of the
    material of the fiber depends on the wavelength and that the source always has
    a finite spectral width.

To decrease pulse dispersion further, it is necessary to use single-mode fibers. As
mentioned in Chapter 4, we can imagine a single-mode fiber allowing propagation of
only one light ray path, corresponding to a single mode, and therefore we would not
have any ray (or intermodal) dispersion. However, in single-mode fibers, in addition to
material dispersion, another dispersion mechanism, referred to as waveguide dispersion,
becomes important; waveguide dispersion depends on the transverse refractive
index profile. In the next section we discuss how by changing the transverse refractive
index profile, we can change the wavelength dependence of the total dispersion.
Later, we discuss dispersion-compensating fibers, which are now used extensively in
optical fiber communication systems. Further, when we refer to high bit rates, it is
also important to consider the phenomenon of polarization mode dispersion, which
can limit the capacity of single-mode fiber optic systems; this is discussed briefly at
the end of the chapter.

 

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