Difference between revisions of "Wigner-Seitz cell"
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| − | + | Synonym: Voronoi domain | |
| − | = | + | <font color="blue">Maille de Wigner-Seitz</font> (''Fr''). <font color="red">Wigner-Seitz-Zelle, Wirkungsbereich</font> (''Ge''). <font color="black">Cella di Wigner-Seitz</font> (''It''). <font color="green">Celda de Wigner-Seitz</font> (''Sp''). |
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| − | Maille de Wigner-Seitz (''Fr''). Wigner-Seitz | ||
== Definition == | == Definition == | ||
| − | [[Image: | + | [[Image:W-S-1.gif|right]] |
| − | The Wigner-Seitz is | + | The Wigner-Seitz cell is a polyhedron obtained by connecting a lattice point ''P'' to all other lattice points and drawing the planes perpendicular to these connecting lines and passing through their midpoints (Fig. 1). The polyhedron enclosed by these planes is the Wigner-Seitz cell. This construction is called the Dirichlet construction. The cell thus obtained is a primitive cell and it is possible to fill up the whole space by translation of that cell. |
| − | + | The Wigner-Seitz cell of a body-centred cubic lattice ''I'' is a cuboctahedron (Fig. 2) and the Wigner-Seitz cell of a face-centred cubic lattice ''F'' is a rhomb-dodecahedron (Fig. 3). In reciprocal space this cell is the first Brillouin zone. Since the reciprocal lattice of a body-centred lattice is a face-centred lattice and reciprocally, the first [[Brillouin_zones|Brillouin zone]] of a body-centred cubic lattice is a rhomb-dodecahedron and that of a face-centred cubic lattice is a cuboctahedron. | |
| − | The Wigner-Seitz cell of a body-centred cubic lattice ''I'' | ||
| + | <center> | ||
| + | [[Image:W-S-2.gif]][[Image:W-S-3.gif]] | ||
| + | </center> | ||
| − | The inside of the Wigner-Seitz cell has been called [[domain of influence]] by Delaunay (1933). It is also called Dirichlet domain or Voronoi domain. The domain of influence of lattice point ''P'' thus consists of all points ''Q'' in space that are closer to this lattice point than to any other lattice point or at most equidistant to it (such that '''OP''' ≤ |'''t''' - '''OP'''| for | + | The inside of the Wigner-Seitz cell has been called the [[domain of influence]] by Delaunay (1933). It is also called the Dirichlet domain or [[Voronoi domain]]. The domain of influence of lattice point ''P'' thus consists of all points ''Q'' in space that are closer to this lattice point than to any other lattice point or at most equidistant to it (such that '''OP''' ≤ |'''t''' - '''OP'''| for any vector '''t''' ∈ ''L''). |
== See also == | == See also == | ||
| + | *Chapter 3.1.1.4 of ''International Tables for Crystallography, Volume A'', 6th edition | ||
| + | *Chapter 1.5 of ''International Tables for Crystallography, Volume B'' | ||
| + | *Chapters 1.2 and 2.2 of ''International Tables for Crystallography, Volume D'' | ||
| − | + | [[Category:Fundamental crystallography]] | |
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| − | [[Category:Fundamental crystallography]] | ||
Latest revision as of 14:50, 20 November 2017
Synonym: Voronoi domain
Maille de Wigner-Seitz (Fr). Wigner-Seitz-Zelle, Wirkungsbereich (Ge). Cella di Wigner-Seitz (It). Celda de Wigner-Seitz (Sp).
Definition
The Wigner-Seitz cell is a polyhedron obtained by connecting a lattice point P to all other lattice points and drawing the planes perpendicular to these connecting lines and passing through their midpoints (Fig. 1). The polyhedron enclosed by these planes is the Wigner-Seitz cell. This construction is called the Dirichlet construction. The cell thus obtained is a primitive cell and it is possible to fill up the whole space by translation of that cell.
The Wigner-Seitz cell of a body-centred cubic lattice I is a cuboctahedron (Fig. 2) and the Wigner-Seitz cell of a face-centred cubic lattice F is a rhomb-dodecahedron (Fig. 3). In reciprocal space this cell is the first Brillouin zone. Since the reciprocal lattice of a body-centred lattice is a face-centred lattice and reciprocally, the first Brillouin zone of a body-centred cubic lattice is a rhomb-dodecahedron and that of a face-centred cubic lattice is a cuboctahedron.
The inside of the Wigner-Seitz cell has been called the domain of influence by Delaunay (1933). It is also called the Dirichlet domain or Voronoi domain. The domain of influence of lattice point P thus consists of all points Q in space that are closer to this lattice point than to any other lattice point or at most equidistant to it (such that OP ≤ |t - OP| for any vector t ∈ L).
See also
- Chapter 3.1.1.4 of International Tables for Crystallography, Volume A, 6th edition
- Chapter 1.5 of International Tables for Crystallography, Volume B
- Chapters 1.2 and 2.2 of International Tables for Crystallography, Volume D