Metadata
aliases: [Elastic wave scattering on crystals, Elastic X-ray scattering on crystals]
shorthands: {}
created: 2021-10-31 20:53:23
modified: 2022-01-20 18:29:37
A common practice is to use scattering experiments to examine the structure of crystals. In these experiments we analyze the scattering pattern made by the deflected waves or particles. In elastic scattering, the energy of the scattering particle/wave remains unchanged, only its direction of propagation changes.
In these experiments we describe the scattering amplitude like this:
Where
The atomic scattering factor is defined as: ^37701d
Now this describes how the scattering happens on the whole unit cell.
We define the lattice sum as:
With these definitions, the scattering amplitude is given as:
The intensity of a wave scattered with
Let's consider a finite size crystal with lattice vectors
With a now omitted derivation we get that in the thermodynamic limit, the lattice sum is:
(Where
We can see that the lattice sum gives us a strong indication for the possible
Based on this, in the scattering pattern, only the Bragg-peaks show up corresponding to the reciprocal lattice vectors. The waves destructively interfere in the other directions.
Let's consider a spherically symmetric charge distribution:
The wavefuction of a 1s orbit (see Hydrogen atom in quantum mechanics):
The charge distribution based on this:
Where
From these, the atomic form factor is: