In physics, a Bragg plane is a plane in reciprocal space which bisects a reciprocal lattice vector,
\scriptstyleK
Considering the adjacent diagram, the arriving x-ray plane wave is defined by:
eik=\cos{(k ⋅ r)}+i\sin{(k ⋅ r)}
Where
\scriptstylek
k=
2\pi | |
λ |
\hat{n}
where
\scriptstyleλ
k\prime |
=
2\pi | |
λ |
\hat{n}\prime
The condition for constructive interference in the
\scriptstyle\hat{n}\prime
|d|\cos{\theta}+|d|\cos{\theta\prime}=d ⋅ \left(\hat{n}-\hat{n}\prime\right)=mλ
where
\scriptstylem~\in~Z
\scriptstyle
2\pi | |
λ |
\scriptstylek
\scriptstyle
k\prime |
d ⋅ \left(k-
k\prime\right) |
=2\pim
Now consider that a crystal is an array of scattering centres, each at a point in the Bravais lattice. We can set one of the scattering centres as the origin of an array. Since the lattice points are displaced by the Bravais lattice vectors,
\scriptstyleR
\scriptstyleR
R ⋅ \left(k-
k\prime\right) |
=2\pim
An equivalent statement (see mathematical description of the reciprocal lattice) is to say that:
| ||||
e |
=1
By comparing this equation with the definition of a reciprocal lattice vector, we see that constructive interference occurs if
\scriptstyleK~=~k-
k\prime |
\scriptstylek
\scriptstyle
k\prime |
\scriptstylek
\scriptstyleK