In the plane S2 and E2 there are seven discrete,
one-dimensional, line groups of isometries, the symmetry groups
of friezes G21: p11 (11), p1g (1g),
p12 (12), pm1 (m1), p1m (1m),
pmg (mg), pmm (mm) and two visually
presentable continuous symmetry groups of friezes:
p0m1=pm01 (m01) and p0mm=
pm0m (m0m).
To denote them, we have used the simplified version of
International Two-dimensional Symbols (M. Senechal, 1975;
H.S.M. Coxeter, 1985). Here, the first symbol represents an
element of symmetry perpendicular to the direction of the
translation, while the second denotes an element of symmetry
parallel or perpendicular (exclusively for 2-rotations) to
the direction of the translation.
Presentations and structures:
Form of the fundamental region: unbounded, allows variation of the
boundaries that do not belong to reflection lines.
Enantiomorphism: 11, 12 possess enantiomorphic
modifications, while in other cases the
enantiomorphism does not occur.
Polarity of rotations: polar rotations - 12, mg;
Polarity of translations: polar translations -
11, 1g, 1m;
The table of minimal indexes of subgroups in groups:
All the discrete symmetry groups of friezes are subgroups
of the group mm generated by reflections and given by the
presentation:
The survey of the characteristics of the symmetry groups
of friezes relies on the work of A.V. Shubnikov, V.A. Koptsik,
1974; H.S.M. Coxeter, W.O.J. Moser, 1980.
The first derivation of the symmetry groups of friezes as
the line subgroups of the symmetry groups of ornaments G2 and
their complete list, was given by G. Pòlya (1924), P. Niggli
(1926) and A. Speiser (1927).
Cayley diagrams (Figure 2.28):
11 {X} C¥
1g {P} C¥
12 {X,T} T2 = (TX)2 = E D¥
{T,T1} T2 = T12 = E (T1 = TX)
m1 {X,R1} R12 = (R1X)2 = E D¥
{R1,R2} R12 = R22 = E (R2 = R1X)
1m {X,R} R2 = E RX = XR C¥ ×D1
mg {P,R1} R12 = (R1P)2 = E D¥
{R1,T} R12 = T2 = E (T = R1P)
mm {X,R,R1} R2 = R12 = (R1X)2 = E RX = XR RR1 = R1R D¥ ×D1
{R,R1,R2} R2 = R12 = R22 = E RR1 = R1R RR2 = R2R (R2 = R1X)
non-polar rotations - mm, m0m.
bipolar translations - 12;
non-polar translations - m1, mg, mm,
m01, m0m.
11 1g 12 m1 1m mg mm
11 2
1g 2 3
12 2 2
m1 2 2
1m 2 2 2
mg 4 2 2 2 3
mm 4 4 2 2 2 2 2
{R,R1,R2} R2 = R12 = R22 = E RR1 = R1R RR2 = R2R D¥ ×D1
R1, T = RR2 generate mg D¥
R, X = R1R2 generate 1m C¥ ×D1
R1, X generate m1 D¥
X, T = RR1 generate 12 D¥
P = RR1R2 generates 1g C¥
X generates 11 C¥
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