Fiber Optic Essentials

Chapter 11 - Fiber Bragg Gratings

11.1   INTRODUCTION

In a normal optical fiber, the refractive indices of the core and of the cladding do not
change along the length of the fiber. In fact, any deviation from this leads to scattering
of the propagating light and to additional loss in the optical fiber. On the other hand,
if we induce a periodic modulation of refractive index along the length in the core of
the optical fiber, such a device, referred to as an optical fiber grating, exhibits very
interesting spectral properties and such fiber gratings are finding many applications
in fiber optic communications and sensing.

There are two main types of fiber gratings: short-period gratings or fiber Bragg
gratings
(FBGs) and long-period gratings (LPGs). In the case of FBGs, the spatial
period of the modulation is about half a micrometer (i.e., the refractive index of
the fiber core varies periodically along the fiber length and has the same value after
every half a micrometer or so). Such a grating couples light at a specific wavelength
propagating in the forward direction in the optical fiber to light propagating in the
reverse direction in the fiber, thus acting like a mirror (Fig. 11.1). LPGs, which have
spatial periods of refractive index modulation of a few hundreds of micrometers,
couple light at specific wavelengths propagating in the core in the forward direction
into the cladding, causing it to be lost from guidance (Fig. 11.2). Due to the periodic
nature of the coupling process, FBGs and LPGs both have very interesting
wavelength characteristics and thus find many uses in telecommunications and
sensing.

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