| The solution of the wave equation comprises of the general form |
|
(34.21) |
| Thus in the absence of dispersion, pulses of arbitrary shape travel without distortion through the fiber. |
| Proof: |
| Let us consider the optical pulse at the input end of medium |
|
(34.22) |
| f(t) is related to its counterpart, F(w) in the frequency domain as |
|
(34.23) |
| After traveling a distance z |
|
(34.24) |
Where |
|
(34.25) |
