Crystallography¶
Cell metric and spacing¶
Cell lengths \(a,b,c\) and angles \(\alpha,\beta,\gamma\) define the direct metric
For reflection indices \(\mathbf h=(h,k,l)^{\mathsf T}\),
Lengths are in Å, angles are entered in degrees, and the trigonometric functions use the corresponding angles. The reciprocal metric above excludes a \(2\pi\) factor. The scattering-vector magnitude is \(Q=2\pi/d\).
Bragg condition¶
For an indexed reflection the order can be incorporated in its Miller indices. The measured powder angle is \(2\theta\), not \(\theta\). A CW reflection is reachable only when \(\lambda/(2d)<1\) in the implemented open-angle domain. See calibration for how this becomes an experimental coordinate.
Symmetry and atom positions¶
Space-group operations map fractional positions as \(\mathbf r'=R\mathbf r+\mathbf t\) modulo lattice translations. The selected setting fixes the coordinate convention. Symmetry may relate cell parameters or fix atom coordinates; such values are not additional independent fitting directions.
The asymmetric unit and its symmetry-generated images define the unit cell. Wyckoff positions describe site symmetry and multiplicity. Do not count identical special-position images twice or confuse a site's multiplicity with the multiplicity of a reflection.
Reflection multiplicity and absences¶
Equivalent reciprocal-lattice vectors contribute a reflection multiplicity to a powder intensity. Centering, glide and screw translations can cause systematic absences through phase cancellation in the structure factor. A reflection's symmetry equivalence is a property of its space-group setting and radiation model; a count of atom sites is not its multiplicity.
For practical input, see Structure. Scattering connects the positions to intensities.
References¶
- International Union of Crystallography. Bragg's law.