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Cyclic symmetry in three dimensions


In three dimensional geometry, there are four infinite series of point groups in three dimensions (n ≥ 1) with n-fold rotational or reflectional symmetry about one axis (by an angle of 360°/n) that does not change the object.

They are the finite symmetry groups on a cone. For n = ∞ they correspond to four frieze groups. Schönflies notation is used. The terms horizontal (h) and vertical (v) imply the existence and direction of reflections with respect to a vertical axis of symmetry. Also shown are Coxeter notation in brackets, and, in parentheses, orbifold notation.

Types

;Chiral:

  • Cn, [n]+, (nn) of order n - n-fold rotational symmetry - acro-n-gonal group (abstract group Zn); for n = 1: no symmetry (trivial group) ;Achiral:
  • Cnh, [n+,2], (n)* of order 2n - prismatic symmetry or ortho-n-gonal group (abstract group Zn × Dih1); for n = 1 this is denoted by Cs (1)* and called reflection symmetry, also bilateral symmetry. It has reflection symmetry with respect to a plane perpendicular to the n-fold rotation axis.
  • Cnv, [n], (nn) of order 2n* - pyramidal symmetry or full acro-n-gonal group (abstract group Dihn); in biology C2v is called biradial symmetry. For n = 1 we have again Cs (1*). It has vertical mirror planes. This is the symmetry group for a regular n-sided pyramid.
  • S2n, [2+,2n+], (n×) of order 2n - gyro-n-gonal group (not to be confused with symmetric groups, for which the same notation is used; abstract group Z2n); It has a 2n-fold rotoreflection axis, also called 2n-fold improper rotation axis, i.e., the symmetry group contains a combination of a reflection in the horizontal plane and a rotation by an angle 180°/n. Thus, like Dnd, it contains a number of improper rotations without containing the corresponding rotations.
    • for n = 1 we have S2 (), also denoted by Ci; this is inversion symmetry.

C2h, [2,2+] (2)* and *C2v, [2], (22) of order 4 are two of the three 3D symmetry group types with the Klein four-group as abstract group. C2v applies e.g. for a rectangular tile with its top side different from its bottom side.

Frieze groups

In the limit these four groups represent Euclidean plane frieze groups as C∞, C∞h, C∞v, and S∞. Rotations become translations in the limit. Portions of the infinite plane can also be cut and connected into an infinite cylinder.

NotationsExamplesIUCOrbifoldCoxeterSchönflies*Euclidean planeCylindrical (n=6)p1∞∞[∞]+C∞p1m1*∞∞[∞]C∞vp11m∞*[∞+,2]C∞hp11g∞×[∞+,2+]S∞
[[File:Frieze example p1.png150px]][[File:Uniaxial c6.png150px]]
[[File:Frieze example p1m1.png150px]][[File:Uniaxial c6v.png150px]]
[[File:Frieze example p11m.png150px]][[File:Uniaxial c6h.png150px]]
[[File:Frieze example p11g.png150px]][[File:Uniaxial s6.png150px]]

Examples

S2/Ci (1x):C4v (*44):C5v (*55):
Parallelepiped[[Image:Square pyramid.png100px]]Square pyramid[[Image:Elongated square pyramid.png100px]]Elongated square pyramid

References

  • On Quaternions and Octonions, 2003, John Horton Conway and Derek A. Smith
  • The Symmetries of Things 2008, John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss,
  • Kaleidoscopes: Selected Writings of H.S.M. Coxeter, edited by F. Arthur Sherk, Peter McMullen, Anthony C. Thompson, Asia Ivic Weiss, Wiley-Interscience Publication, 1995, wiley.com,
  • N.W. Johnson: Geometries and Transformations, (2018) , Chapter 11: Finite symmetry groups, 11.5 Spherical Coxeter groups
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