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Compton Scattering *****

**Compton scattered high energy photons from (essentially) free electrons** in 1923.
He measured the wavelength of the scattered photons as a function of the scattering angle.
The figure below shows both the initial state (a) and the final state, with the photon
scattered by an angle
and the electron recoiling at an angle
.
The photons were from nuclear decay and so they were of high enough energy that it
didn't matter that the electrons were actually bound in atoms.
We wish to derive the formula for the **wavelength of the scattered photon as a function of angle**.

We solve the problem using only conservation of energy and momentum.
Lets work in **units in which**
for now. We'll put the
back in at the end.
Assume the photon is initially moving in the
direction with energy E
and that it scatters in the
plane so that
.
**Conservation of momentum** gives

**and**

**Conservation of energy** gives

Our goal is to solve for
in terms of
so lets make sure we eliminate the
.
Continuing from the energy equation

squaring and calculating
from the components

and writing out the squares on the right side

and removing things that appear on both sides

and grouping

Since
in our fine units,

We now apply the speed of light to make the units come out to be a length.

These calculations can be fairly frustrating if you don't decide which variables you want to keep and which
you need to eliminate from your equations.
In this case we eliminated
by using the energy equation and computing
.

Jim Branson
2013-04-22