Definition:
The displacive distortion of a given atom or rigid group (see
also _atom_site_rot_Fourier_param_modulus) is usually
parameterized by Fourier series. Each term of the series commonly
adopts two different representations: the sine-cosine form,
Ac cos(2\p k r)+As sin(2\p k r),
and the modulus-argument form,
|A| cos(2\p k r+\f),
where k is the wave vector of the term and r is the atomic
average position. _atom_site_displace_Fourier_param_modulus is
the modulus (|A|) of the complex amplitude corresponding to the
Fourier term defined by
_atom_site_displace_Fourier_atom_site_label,
_atom_site_displace_Fourier_axis and
_atom_site_displace_Fourier_wave_vector_seq_id. Atomic or rigid-
group displacements must be expressed as fractions of the unit
cell or in angstroms if the modulations are referred to some
special axes defined by
_atom_sites_displace_Fourier_axes_description.
Appears in list containing _atom_site_displace_Fourier_param_id
The permitted range is 0.0 -> infinity
Enumeration default: 0.0
Type: numb
Category: atom_site_displace_Fourier_param
Copyright © 2005 International Union of Crystallography