Fixed points of isometry groups in Euclidean space
For an object, any unique centre and, more generally, any point with unique properties with respect to the object is a fixed point of its symmetry group.
In particular this applies for the centroid of a figure, if it exists. In the case of a physical body, if for the symmetry not only the shape but also the density is taken into account, it applies to the centre of mass.
If the set of fixed points of the symmetry group of an object is a singleton then the object has a specific centre of symmetry. The centroid and centre of mass, if defined, are this point. Another meaning of "centre of symmetry" is a point with respect to which inversion symmetry applies. Such a point needs not be unique; if it is not, there is translational symmetry, hence there are infinitely many of such points. On the other hand, in the cases of e.g. C3h and D2 symmetry there is a centre of symmetry in the first sense, but no inversion.
If the symmetry group of an object has no fixed points then the object is infinite and its centroid and centre of mass are undefined.
If the set of fixed points of the symmetry group of an object is a line or plane then the centroid and centre of mass of the object, if defined, and any other point that has unique properties with respect to the object, are on this line or plane.
1D
- Line
- Only the trivial isometry group leaves the whole line fixed.
- Point
- The groups generated by a reflection leave a point fixed.
2D
- Plane
- Only the trivial isometry group C1 leaves the whole plane fixed.
- Line
- Cs with respect to any line leaves that line fixed.
- Point
- The point groups in two dimensions with respect to any point leave that point fixed.
3D
- Space
- Only the trivial isometry group C1 leaves the whole space fixed.
- Plane
- Cs with respect to a plane leaves that plane fixed.
- Line
- Isometry groups leaving a line fixed are isometries which in every plane perpendicular to that line have common 2D point groups in two dimensions with respect to the point of intersection of the line and the planes.
- Cn ( n > 1 ) and Cnv ( n > 1 )
- cylindrical symmetry without reflection symmetry in a plane perpendicular to the axis
- cases in which the symmetry group is an infinite subset of that of cylindrical symmetry
- Point
- All other point groups in three dimensions
- No fixed points
- The isometry group contains translations or a screw operation.
Arbitrary dimension
- Point
- One example of an isometry group, applying in every dimension, is that generated by inversion in a point. An n-dimensional parallelepiped is an example of an object invariant under such an inversion.
References
Slavik V. Jablan, Symmetry, Ornament and Modularity, Volume 30 of K & E Series on Knots and Everything, World Scientific, 2002. ISBN 9812380809
 |
