Point group

From Online Dictionary of Crystallography

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<font color="blue">Groupe ponctuel</font> (''Fr''). <font color="red">Punktgruppe</font> (''Ge''). <font color="green">Grupo puntual</font> (''Sp''). <font color="black">Gruppo punto</font> (''It''). <font color="brown">Точечная группа симметрии</font> (''Ru''). <font color="purple">点群</font> (''Ja'').
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<font color="orange">زمرة نقطية</font> (''Ar''); <font color="blue">Groupe ponctuel</font> (''Fr''); <font color="red">Punktgruppe</font> (''Ge''); <font color="black">Gruppo punto</font> (''It''); <font color="purple">点群</font> (''Ja''); <font color="brown">Точечная группа симметрии</font> (''Ru''); <font color="green">Grupo puntual</font> (''Sp'').
==Definition==
==Definition==

Revision as of 09:26, 12 October 2017

زمرة نقطية (Ar); Groupe ponctuel (Fr); Punktgruppe (Ge); Gruppo punto (It); 点群 (Ja); Точечная группа симметрии (Ru); Grupo puntual (Sp).

Contents

Definition

A point group is a group of symmetry operations all of which leave at least one point unmoved. A crystallographic point group is a point group that maps a point lattice onto itself: in three dimensions rotations and rotoinversions are restricted to 1, 2, 3, 4, 6 and \bar 1, \bar 2 (= m), \bar 3, \bar 4, \bar 6 respectively.

Occurrence

Crystallographic point groups occur:

  • in vector space, as symmetries of the external shapes of crystals (morphological symmetry), as well as symmetry of the physical properties of the crystal ('vector point group');
  • in point space, as site-symmetry groups of points in lattices or in crystal structures, and as symmetries of atomic groups and coordination polyhedra ('point point group').

Controversy on the nomenclature

The matrix representation of a symmetry operation consists of a linear part, which represents the rotation or rotoinversion component of the operation, and a vector part, which gives the shift to be added once the linear part of the operation has been applied. The vector part is divided into two components: the intrinsic component, which represents the screw and glide component of the operation, and the localization component, which is non-zero when the symmetry element does not pass through the origin. The set of the linear parts of the matrices representing the symmetry operations of a space group is a representation of the point group of the crystal. On the other hand, the set of matrix-vector pairs representing the symmetry operations of a site symmetry group form a group which is isomorphic to a crystallographic point group. The vector part being in general non-zero, some authors reject the term point group for the site-symmetry groups. On the other hand, all the symmetry elements of a site symmetry group do leave invariant at least one point, albeit not necessarily the origin, satisfying the above definition of point group.

See also

  • Chapter 3.2.1 of International Tables for Crystallography, Volume A, 6th edition