Derivation of braggs law using laue equation
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Let
{\displaystyle \mathbf {a} \,,\mathbf {b} \,,\mathbf {c} }
be the primitive vectors of the crystal lattice
{\displaystyle L}
, whose atoms are located at the points
{\displaystyle \mathbf {x} =p\,\mathbf {a} +q\,\mathbf {b} +r\,\mathbf {c} }
that are integer linear combinations of the primitive vectors.
Let
{\displaystyle \mathbf {k} _{\mathrm {in} }}
be the wavevector of the incoming (incident) beam, and let
{\displaystyle \mathbf {k} _{\mathrm {out} }}
be the wavevector of the outgoing (diffracted) beam. Then the vector
{\displaystyle \mathbf {k} _{\mathrm {out} }-\mathbf {k} _{\mathrm {in} }=\mathbf {\Delta k} }
is called the scattering vector (also called transferred wavevector) and measures the change between the two wavevectors.
The three conditions that the scattering vector
{\displaystyle \mathbf {\Delta k} }
must satisfy, called the Laue equations, are the following: the numbers
{\displaystyle h,k,l}
determined by the equations
{\displaystyle \mathbf {a} \cdot \mathbf {\Delta k} =2\pi h}
{\displaystyle \mathbf {b} \cdot \mathbf {\Delta k} =2\pi k}
{\displaystyle \mathbf {c} \cdot \mathbf {\Delta k} =2\pi l}
must be integer numbers. Each choice of the integers
{\displaystyle (h,k,l)}
, called Miller indices, determines a scattering vector
{\displaystyle \mathbf {\Delta k} }
. Hence there are infinitely many scattering vectors that satisfy the Laue equations. They form a lattice
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