Abstract
The special orthogonal group SO 3 may be identified with the group of rotations of β3 which fix the origin (Chapter 9). If an object is positioned in β3 with its centre of gravity at the origin, then its rotational symmetry group βisβ a subgroup of SO 3 . We are familiar with several possibilities. From a right regular pyramid with an n-sided base we obtain a cyclic group of order n, while a regular plate with n sides exhibits dihedral symmetry and gives D n . (Regular with two sides means the lens shape described in Exercise 9.12.) In addition, we have the symmetry groups of the regular solids. As we shall see, these are the only possibilities, provided our object has only a finite amount of symmetry. In other words a finite subgroup of SO 3 is either cyclic, dihedral, or isomorphic to the rotational symmetry group of one of the regular solids. We begin with a less ambitious result which deals with finite subgroups of O 2.
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Β© 1988 Springer Science+Business Media New York
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Armstrong, M.A. (1988). Finite Rotation Groups. In: Groups and Symmetry. Undergraduate Texts in Mathematics. Springer, New York, NY. https://doi.org/10.1007/978-1-4757-4034-9_19
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DOI: https://doi.org/10.1007/978-1-4757-4034-9_19
Publisher Name: Springer, New York, NY
Print ISBN: 978-1-4419-3085-9
Online ISBN: 978-1-4757-4034-9
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