In a Body-Centered Cubic (BCC) crystal structure, the reflection conditions in X-ray diffraction are derived based on structure factor calculations.
The structure factor for BCC is non-zero (i.e., reflections are allowed) only when the sum of the Miller indices \( h + k + l \) is even.
This arises because the BCC unit cell has atoms at positions (0,0,0) and (1/2,1/2,1/2).
The phase difference introduced by the atom at (1/2,1/2,1/2) is:
\[
\exp\left[\pi i (h + k + l)\right] = (-1)^{h+k+l}
\]
So, the structure factor becomes zero (i.e., forbidden reflection) when \( h + k + l \) is odd, and is non-zero (i.e., allowed reflection) when \( h + k + l \) is even.