In: Physics
Consider pulse propagation in a dispersive, isotropic medium with a refractive index given as a function of vacuum wavelength lmda0 by: n(lmda0) = nc + a (lmda0/lmdac )^2
Here nc, a, and lmdac are fixed parameters describing the medium.
a) Derive an expression for the phase velocity of radiation in this medium, and evaluate your answer for vacuum wavelength lmda0 = lmdac .
b) Derive an expression for the velocity of a pulse propagating in this medium, and evaluate your answer when the pulse’s central vacuum wavelength is lmda0 = lmdac. For a transform‐limited optical pulse of initial duration t0, and a central vacuum wavelength of lmda0 = lmdac, write an expression for the pulse broadening after propagation over a distance d.
Let us assume the speed in the vacuum is c.
And so, the phase velocity in the medium is

Now given
And so, the phase velocity in terms of the vacuum wavelength
is

And so, the phase velocity at
is
b)
Group velocity is defined as



Now as we have already got

So,

Ans so,

And so, at

Let the initial duration is
.
And the pulse has propagated a distance d. Let us
assume that as the pulse propagates it broadens to a width
.
This amount of spreading occurs because the different
frequency components move at a different group velocity. And so, if
we assume the two ferquency components

Now as the initial duration is

So, we have





Now we have


And so,

Now at

And so, at

