Difference between revisions of "OD structure"
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| − | <font color="blue">Structure OD</font> (''Fr'') | + | <font color="blue">Structure OD</font> (''Fr''). <font color="red">OD Struktur</font> (''Ge''). <font color="black">Struttura OD</font> (''It''). <font color="purple">OD構造</font> (''Ja''). |
| − | OD structures consist of slabs with their own symmetry, containing coincidence operations constituting a [[subperiodic group|diperiodic group]] (layer group) only within individual slabs. For the entire structure these coincidence operations are only local (partial), i.e. they are valid only in a subspace of the crystal space. The ambiguity (= existence of more than one equivalent possibilities) in the stacking of slabs arises from the existence of this local symmetry, which does not appear in the [[space group]] of the structure. The resulting structure can be | + | OD structures consist of slabs with their own symmetry, containing coincidence operations constituting a [[subperiodic group|diperiodic group]] (layer group) only within individual slabs. For the entire structure these coincidence operations are only local (partial), ''i.e.'' they are valid only in a subspace of the crystal space. The ambiguity (= existence of more than one equivalent possibilities) in the stacking of slabs arises from the existence of this local symmetry, which does not appear in the [[space group]] of the structure. The resulting structure can be 'ordered' (''periodic'') or 'disordered' (''non-periodic''), depending on the sequence of local symmetry operations relating pairs of slabs. The set of all the operations valid in the whole crystal space constitutes a [[space group]]; by adding the set of all the operations valid in a subspace of it, one obtains a space [[groupoid]]. |
In the OD theory, a central role is played by the '''vicinity condition''' ('''VC'''), which states the geometrical equivalence of layer pairs. The vicinity condition consists of three parts: | In the OD theory, a central role is played by the '''vicinity condition''' ('''VC'''), which states the geometrical equivalence of layer pairs. The vicinity condition consists of three parts: | ||
| − | *'''VC α | + | *'''VC''' α: VC layers are either geometrically equivalent or, if not, they are relatively few in kind. |
| − | *'''VC β | + | *'''VC''' β: translation groups of all VC layers are either identical or they have a common subgroup. |
| − | *'''VC γ | + | *'''VC''' γ: equivalent sides of equivalent layers are faced by equivalent sides of adjacent layers so that the resulting pairs are equivalent. |
If the position of a layer is uniquely defined by the position of the adjacent layers and by the VC, the resulting structure is fully ordered. If, on the other hand, more than one position is possible that obeys the VC, the resulting structure is an '''OD structure''' and the layers are '''OD layers'''. VC structures may thus be either fully ordered structures or OD structures. All OD structures are [[polytypism|polytypic]]; the reverse may or may not be true. Equivalency depends on the choice of OD layers and also on the definition of [[polytypism]]. | If the position of a layer is uniquely defined by the position of the adjacent layers and by the VC, the resulting structure is fully ordered. If, on the other hand, more than one position is possible that obeys the VC, the resulting structure is an '''OD structure''' and the layers are '''OD layers'''. VC structures may thus be either fully ordered structures or OD structures. All OD structures are [[polytypism|polytypic]]; the reverse may or may not be true. Equivalency depends on the choice of OD layers and also on the definition of [[polytypism]]. | ||
==The notion of family== | ==The notion of family== | ||
| − | All OD structures, even of different substances, built according to the same symmetry principle, belong to an '''OD groupoid family'''. The notion OD groupoid family may be compared with the notion space-group type: the infinite space groups are classified in a finite number of space-group types. Similarly, the infinite OD groupoids are classified in a finite number of OD groupoid families. For OD structures of one kind of layers, there are 400 OD groupoid families | + | All OD structures, even of different substances, built according to the same symmetry principle, belong to an '''OD groupoid family'''. The notion OD groupoid family may be compared with the notion space-group type: the infinite space groups are classified in a finite number of space-group types. Similarly, the infinite OD groupoids are classified in a finite number of OD groupoid families. For OD structures of one kind of layers, there are 400 OD groupoid families. |
| − | The OD groupoid family is an abstract family, whose members are the groupoids describing the symmetry of the substances sharing the same symmetry principle. Moving from the abstract to the concrete level, the OD structures of the same substance built on the same structural principle - differing thus | + | The OD groupoid family is an abstract family, whose members are the groupoids describing the symmetry of the substances sharing the same symmetry principle. Moving from the abstract to the concrete level, the OD structures of the same substance built on the same structural principle - differing thus in their stacking mode - belong to one and the same family: the members of a family are individual, real structures. |
==See also== | ==See also== | ||
| − | * Chapter 9.2 of ''[http://it.iucr.org/C/ International Tables for Crystallography, Volume C]'' | + | *Chapter 9.2 of ''[http://it.iucr.org/C/ International Tables for Crystallography, Volume C]'' |
[[Category:Fundamental crystallography]] | [[Category:Fundamental crystallography]] | ||
Latest revision as of 13:15, 16 November 2017
Structure OD (Fr). OD Struktur (Ge). Struttura OD (It). OD構造 (Ja).
OD structures consist of slabs with their own symmetry, containing coincidence operations constituting a diperiodic group (layer group) only within individual slabs. For the entire structure these coincidence operations are only local (partial), i.e. they are valid only in a subspace of the crystal space. The ambiguity (= existence of more than one equivalent possibilities) in the stacking of slabs arises from the existence of this local symmetry, which does not appear in the space group of the structure. The resulting structure can be 'ordered' (periodic) or 'disordered' (non-periodic), depending on the sequence of local symmetry operations relating pairs of slabs. The set of all the operations valid in the whole crystal space constitutes a space group; by adding the set of all the operations valid in a subspace of it, one obtains a space groupoid.
In the OD theory, a central role is played by the vicinity condition (VC), which states the geometrical equivalence of layer pairs. The vicinity condition consists of three parts:
- VC α: VC layers are either geometrically equivalent or, if not, they are relatively few in kind.
- VC β: translation groups of all VC layers are either identical or they have a common subgroup.
- VC γ: equivalent sides of equivalent layers are faced by equivalent sides of adjacent layers so that the resulting pairs are equivalent.
If the position of a layer is uniquely defined by the position of the adjacent layers and by the VC, the resulting structure is fully ordered. If, on the other hand, more than one position is possible that obeys the VC, the resulting structure is an OD structure and the layers are OD layers. VC structures may thus be either fully ordered structures or OD structures. All OD structures are polytypic; the reverse may or may not be true. Equivalency depends on the choice of OD layers and also on the definition of polytypism.
The notion of family
All OD structures, even of different substances, built according to the same symmetry principle, belong to an OD groupoid family. The notion OD groupoid family may be compared with the notion space-group type: the infinite space groups are classified in a finite number of space-group types. Similarly, the infinite OD groupoids are classified in a finite number of OD groupoid families. For OD structures of one kind of layers, there are 400 OD groupoid families.
The OD groupoid family is an abstract family, whose members are the groupoids describing the symmetry of the substances sharing the same symmetry principle. Moving from the abstract to the concrete level, the OD structures of the same substance built on the same structural principle - differing thus in their stacking mode - belong to one and the same family: the members of a family are individual, real structures.
See also
- Chapter 9.2 of International Tables for Crystallography, Volume C