#include <asu.h>

Public Member Functions | |
| asym_index () | |
| Default constructor. Some data members are not initialized! | |
| asym_index (sgtbx::space_group const &space_group, sgtbx::reciprocal_space::asu const &asu, index<> const &h) | |
| Selection of an asymmetric Miller index. | |
| asym_index (sgtbx::space_group const &space_group, index<> const &h) | |
| Selection of a "pretty" index for human-readable listings, given symmetry operations and an input index. | |
| asym_index (sym_equiv_indices const &h_eq) | |
| Selection of a "pretty" index for human-readable listings, given a list of symmetrically equivalent Miller indices. | |
| index_table_layout_adaptor | one_column (bool anomalous_flag) const |
| Adaptor for one-column table of asymmetric Miller indices. | |
| index_table_layout_adaptor | two_column (bool anomalous_flag) const |
| Adaptor for two-column table of asymmetric Miller indices. | |
The selection of a particular asymmetric Miller index amongst symmetrically equivalent Miller indices is based on class sgtbx::reciprocal_space::asu, or alternatively on an ad hoc scheme for the determination of the "prettiest" index for human- readable listings.
Friedel's law is always considered in the determination of the asymmetric index. friedel_flag() indicates if Friedel's law was actually applied.
Support for one- and two-column data layouts is provided using the class index_table_layout_adaptor:
| asym_index | ( | sgtbx::space_group const & | space_group, | |
| sgtbx::reciprocal_space::asu const & | asu, | |||
| index<> const & | h | |||
| ) |
Selection of an asymmetric Miller index.
The asymmetric index is determined as the product of the index h and the symmetry operation of sgtbx::space_group which maps h into the reciprocal space asymmetric unit (sgtbx::reciprocal_space::asu).
| asym_index | ( | sgtbx::space_group const & | space_group, | |
| index<> const & | h | |||
| ) |
| asym_index | ( | sym_equiv_indices const & | h_eq | ) |
Selection of a "pretty" index for human-readable listings, given a list of symmetrically equivalent Miller indices.
The selection is based on miller::index<>::operator<(). The asymmetric unit from which the indices are selected is not necessarily contiguous.
| index_table_layout_adaptor one_column | ( | bool | anomalous_flag | ) | const [inline] |
Adaptor for one-column table of asymmetric Miller indices.
anomalous_flag == false and only one value is stored for a Friedel pair:
h k l F The values associated with h,k,l and -h,-k,-l are assumed to be equal, and the phases are related by the equation phi(h,k,l) = -phi(-h,-k,-l). anomalous_flag == true (i.e. in the presence of an anomalous signal):
h k l F
-h -k -l F There is a separate entry for each Friedel mate in a table.
| index_table_layout_adaptor two_column | ( | bool | anomalous_flag | ) | const [inline] |
Adaptor for two-column table of asymmetric Miller indices.
anomalous_flag == false: same as one_column(). Only one column is used. Provided for completeness.
anomalous_flag == true:
h k l F+ F- Both Friedel mates are associated with the same index in a table. The Miller index for F+ is (h, k, l) and the implied Miller index for F- is (-h, -k, -l).
1.5.6