Dichromatic symmetry explained

Dichromatic symmetry,[1] also referred to as antisymmetry,[2] black-and-white symmetry,[3] magnetic symmetry,[4] counterchange symmetry[5] or dichroic symmetry,[6] is a symmetry operation which reverses an object to its opposite.[7] A more precise definition is "operations of antisymmetry transform objects possessing two possible values of a given property from one value to the other."[8] Dichromatic symmetry refers specifically to two-coloured symmetry; this can be extended to three or more colours in which case it is termed polychromatic symmetry.[9] A general term for dichromatic and polychromatic symmetry is simply colour symmetry. Dichromatic symmetry is used to describe magnetic crystals and in other areas of physics,[10] such as time reversal,[11] which require two-valued symmetry operations.

Examples

A simple example is to take a white object, such as a triangle, and apply a colour change resulting in a black triangle. Applying the colour change once more yields the original white triangle.

The colour change, here termed an anti-identity operation (1'), yields the identity operation (1) if performed twice.

Another example is to construct an anti-mirror reflection (m') from a mirror reflection (m) and an anti-identity operation (1') executed in either order.

The m' operation can then be used to construct the antisymmetry point group 3m' of a dichromatic triangle.

There are no mirror reflection (m) operations for the dichromatic triangle, as there would be if all the smaller component triangles were coloured white. However, by introducing the anti-mirror reflection (m') operation the full dihedral D3 symmetry is restored. The six operations making up the dichromatic D3 (3m') point group are:

Note that the vertex numbers do not form part of the triangle being operated on - they are shown to keep track of where the vertices end up after each operation.

History

In 1930 Heinrich Heesch was the first person to formally postulate an antisymmetry operation in the context of examining the 3D space groups in 4D.[12] Heesch's work was influenced by Weber's 1929 paper on black-and-white colouring of 2D bands.[13]

In 1935-1936 H.J. Woods published a series of four papers with the title The geometrical basis of pattern design. The last of these[14] was devoted to counterchange symmetry and in which was derived for the first time the 46 dichromatic 2D point groups.

The work of Heesch and Woods were not influential at the time, and the subject of dichromatic symmetry did not start to become important until the publication of A.V. Shubnikov's book Symmetry and antisymmetry of finite figures in 1951. Thereafter the subject developed rapidly, initially in Russia but subsequently in many other countries, because of its importance in magnetic structures and other physical fields.

Dimensional counts

The table below gives the number of ordinary and dichromatic groups by dimension. The Bohm[37] symbol

a
G
ol
is used to denote the number of groups where

o

= overall dimension,

l

= lattice dimension and

a

= number of antisymmetry operation types.

a=1

for dichromatic groups with a single antisymmetry operation .
Overall
dimension
Lattice
dimension
Ordinary groupsDichromatic groups
NameSymbolCountRefsSymbolCountRefs
00Zero-dimensional symmetry group

G0

1
1
G
0
2
1 0One-dimensional point groups

G10

2
1
G
10
5
1One-dimensional discrete symmetry groups

G1

2
1
G
1
7
20Two-dimensional point groups (rosettes)

G20

10
1
G
20
31
1Frieze (strip) groups

G21

7[38]
1
G
21
31
2Wallpaper (plane) groups

G2

17[39] [40]
1
G
2
80[41]
30Three-dimensional point groups

G30

32[42]
1
G
30
122
1Rod (cylinder) groups

G31

75
1
G
31
394[43]
2Layer (sheet) groups

G32

80
1
G
32
528[44]
3Three-dimensional space groups

G3

230[45]
1
G
3
1651
40Four-dimensional point groups

G40

271[46]
1
G
40
1202[47]
1

G41

343[48]
2

G42

1091[49]
3

G43

1594[50]
4Four-dimensional discrete symmetry groups

G4

4894
1
G
4
62227

External links

Notes and References

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  2. Shubnikov, A.V. (1951). Symmetry and antisymmetry of finite figures, Izv. Akad. Nauk SSSR, Moscow
  3. Gévay, G. (2000). Black-and-white symmetry, magnetic symmetry, self-duality and antiprismatic symmetry: the common mathematical background, Forma, 15, 57–60
  4. Tavger, B.A. (1958). The symmetry of ferromagnetics and antiferromagnetics, Sov. Phys. Cryst., 3, 341-343
  5. Woods, H.J. (1935). The geometric basis of pattern design part I: point and line symmetry in simple figures and borders, Journal of the Textile Institute, Transactions, 26, T197-T210
  6. Makovicky, E. (2016). Symmetry through the eyes of old masters, de Gruyter, Berlin,
  7. Atoji, A. (1965). Graphical representations of magnetic space groups, American Journal of Physics, 33(3), 212–219
  8. Mackay, A.L. (1957). Extensions of space-group theory, Acta Crystallogr. 10, 543-548,
  9. Lockwood, E.H. and Macmillan, R.H. (1978). Geometric symmetry , Cambridge University Press, Cambridge, 67-70 & 206-208
  10. Padmanabhan, H., Munro, J.M., Dabo, I and Gopalan, V. (2020). Antisymmetry: fundamentals and applications, Annual Review of Materials Research, 50, 255-281,
  11. Shubnikov, A.V. (1960). Time reversal as an operation of antisymmetry, Sov. Phys. Cryst., 5, 309-314
  12. Heesch, H. (1930). Über die vierdimensionalen Gruppen des dreidimensionalen Raumes, Z. Krist., 73, 325-345
  13. Weber, L. (1929). Die Symmetrie homogener ebener Punktsysteme, Z. Krist., 70, 309-327,
  14. Woods, H.J. (1936). The geometric basis of pattern design part IV: counterchange symmetry in plane patterns, Journal of the Textile Institute, Transactions, 27, T305-320
  15. Landau, L.D. and Lifshitz E.M. (1951). Course of theoretical physics, vol. 5. Statistical physics, 1st edition, Nauka, Moscow
  16. Zamorzaev, A.M. (1953). Generalization of the space groups, Dissertation, Leningrad University
  17. Zamorzaev, A.M. (1957). Generalization of Fedorov groups, Sov. Phys. Cryst., 2, 10-15
  18. Tavger, B.A. and Zaitsev, V.M. (1956). Magnetic symmetry of crystals, Soviet Physics JETP, 3(3), 430-436
  19. Belov, N.V., Neronova, N.N. and Smirnova, T.S. (1957). Shubnikov groups, Sov. Phys. Cryst., 2, 311-322
  20. Zamorzaev, A.M. and Sokolov, E.I. (1957). Symmetry and various kinds of antisymmetry of finite bodies, Sov. Phys. Cryst., 2, 5-9
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  24. Koptsik, V.A. (1968). A general sketch of the development of the theory of symmetry and its applications in physical crystallography over the last 50 years, Sov. Phys. Cryst., 12(5), 667-683
  25. Schwarzenberger, R.L.E. (1984). Colour symmetry, Bull. London Math. Soc., 16, 209-240,
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  27. Brückler, F.M. and Stilinović, V. (2024) From friezes to quasicrystals: a history of symmetry groups, 1-42,, in Sriraman, B. (ed.) Handbook of the history and philosophy of mathematical practice, Springer, pp 3200,
  28. MacGillavry, C.H. (1976). Symmetry aspects of M. C. Escher's periodic drawings, International Union of Crystallography, Utrecht,
  29. Schnattschneider, D. (2004). , Harry. N. Abrams, New York,
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  32. Opechowski, W. and Guccione, R. (1965). Magnetic symmetry in Magnetism, vol. IIA ed. Rado, G.T. and Suhl, H., Academic Press, New York, pp 105-165
  33. Koptsik, V.A. (1966). Shubnikov groups: Handbook on the symmetry and physical properties of crystal structures, Moscow University, Moscow
  34. Shubnikov, A.V. and Koptsik, V.A. (1974). Symmetry in science and art, Plenum Press, New York, (original in Russian published by Nauka, Moscow, 1972.)
  35. Washburn, D.K. and Crowe, D.W. (1988). , Washington University Press, Seattle,
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  39. Fedorov . E.S. . Симметрія на плоскости . Записки Императорского С.-Петербургского Минералогического Общества (Zapiski Imperatorskova Sankt-Petersburgskova Mineralogicheskova Obshchestva, Proceedings of the Imperial St. Petersburg Mineralogical Society) . 1891 . 28 . 345–390 . 2nd series . Simmetriya na ploskosti, Symmetry in the plane . ru.
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  45. Burckhardt, J.J. (1967). Zur Geschichte der Entdeckung der 230 Raumgruppen [On the history of the discovery of the 230 space groups], Archive for History of Exact Sciences, 4(3), 235-246,
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