XI. Single-Mode Fibers

While discussing step-index fibers, we considered light propagation inside the fiber as a set of many rays bouncing back and forth at the core-cladding interface (see Figure 7-7). There the angle q could take a continuum of values lying between 0 and cos–1(n2/n1), i.e.,

0 < q < cos–1 (n2/n1)

For n2 = 1.5 and D » = 0.01, we would get n2/n 1 ~ and cos –1  = 8.1°, so

0 < q < 8.1°

Now, when the core radius (or the quantity D) becomes very small, ray optics does not remain valid and one has to use the more accurate wave theory based on Maxwell's equations. This wave theory is fairly involved [see, e.g., Chapters 7 and 8 of Ghatak and Thyagarajan]. Here we just give some of the important results for a step-index fiber.

In wave theory, one introduces the parameter

 

(7-28)

where D has been defined earlier (see Equation 7-5) and n1  ~  n2 . The quantity V is often referred to as the "V-number" or the "waveguide parameter" of the fiber. It can be shown that, if

V < 2.4045

only one guided mode (as if there is only one discrete value of q) is possible and the fiber is known as a single-mode fiber. Further, for a step-index single-mode fiber, the corresponding (discrete) value of q is approximately given by the following empirical formula

 

(7-29)

We may mention here that because of practical considerations the value D of ranges from about 0.002 to about 0.008.