Trihexagonal tiling

Trihexagonal tiling

TypeSemiregular tiling
Vertex configuration
(3.6)2
Schläfli symbolr{6,3}
h2{6,3}
Wythoff symbol2 | 6 3
3 3 | 3
Coxeter diagram
=
Symmetryp6m, [6,3], (*632)
Rotation symmetryp6, [6,3]+, (632)
p3, [3[3]]+, (333)
Bowers acronymThat
DualRhombille tiling
PropertiesVertex-transitive Edge-transitive

In geometry, the trihexagonal tiling is one of 11 uniform tilings of the Euclidean plane by regular polygons.[1] It consists of equilateral triangles and regular hexagons, arranged so that each hexagon is surrounded by triangles and vice versa. The name derives from the fact that it combines a regular hexagonal tiling and a regular triangular tiling. Two hexagons and two triangles alternate around each vertex, and its edges form an infinite arrangement of lines. Its dual is the rhombille tiling.[2]

This pattern, and its place in the classification of uniform tilings, was already known to Johannes Kepler in his 1619 book Harmonices Mundi.[3] The pattern has long been used in Japanese basketry, where it is called kagome. The Japanese term for this pattern has been taken up in physics, where it is called a Kagome lattice. It occurs also in the crystal structures of certain minerals. Conway calls it a hexadeltille, combining alternate elements from a hexagonal tiling (hextille) and triangular tiling (deltille).[4]

Kagome

Japanese basket showing the kagome pattern

Kagome (籠目) is a traditional Japanese woven bamboo pattern; its name is composed from the words kago, meaning "basket", and me, meaning "eye(s)", referring to the pattern of holes in a woven basket.

It is a weaved arrangement of laths composed of interlaced triangles such that each point where two laths cross has four neighboring points, forming the pattern of a trihexagonal tiling. The weaved process gives the Kagome a chiral wallpaper group symmetry, p6, (632).

Kagome lattice

The term kagome lattice was coined by Japanese physicist Kôdi Husimi, and first appeared in a 1951 paper by his assistant Ichirō Shōji.[5] The kagome lattice in this sense consists of the vertices and edges of the trihexagonal tiling. Despite the name, these crossing points do not form a mathematical lattice.

A related three dimensional structure formed by the vertices and edges of the quarter cubic honeycomb, filling space by regular tetrahedra and truncated tetrahedra, has been called a hyper-kagome lattice.[6] It is represented by the vertices and edges of the quarter cubic honeycomb, filling space by regular tetrahedra and truncated tetrahedra. It contains four sets of parallel planes of points and lines, each plane being a two dimensional kagome lattice. A second expression in three dimensions has parallel layers of two dimensional lattices and is called an orthorhombic-kagome lattice.[6] The trihexagonal prismatic honeycomb represents its edges and vertices.

Some minerals, namely jarosites and herbertsmithite, contain two dimensional layers or three dimensional kagome lattice arrangement of atoms in their crystal structure. These minerals display novel physical properties connected with geometrically frustrated magnetism. For instance, the spin arrangement of the magnetic ions in Co3V2O8 rests in a kagome lattice which exhibits fascinating magnetic behavior at low temperatures.[7] The term is much in use nowadays in the scientific literature, especially by theorists studying the magnetic properties of a theoretical kagome lattice.

Symmetry

30-60-90 triangle fundamental domains of p6m (*632) symmetry

The trihexagonal tiling has Schläfli symbol of r{6,3}, or Coxeter diagram, , symbolizing the fact that it is a rectified hexagonal tiling, {6,3}. Its symmetries can be described by the wallpaper group p6mm, (*632),[8] and the tiling can be derived as a Wythoff construction within the reflectional fundamental domains of this group. The trihexagonal tiling is a quasiregular tiling, alternating two types of polygons, with vertex configuration (3.6)2. It is also a uniform tiling, one of eight derived from the regular hexagonal tiling.

Uniform colorings

There are two distinct uniform colorings of a trihexagonal tiling. Naming the colors by indices on the 4 faces around a vertex (3.6.3.6): 1212, 1232.[1] The second is called a cantic hexagonal tiling, h2{6,3}, with two colors of triangles, existing in p3m1 (*333) symmetry.

Symmetry p6m, (*632) p3m, (*333)
Coloring
fundamental
domain
Wythoff 2 | 6 3 3 3 | 3
Coxeter =
Schläfli r{6,3} r{3[3]} = h2{6,3}

Topologically equivalent tilings

The trihexagonal tiling can be geometrically distorted into topologically equivalent tilings of lower symmetry.[1] In these variants of the tiling, the edges do not necessarily line up to form straight lines.

p3m1, (*333) p3, (333) p31m, (3*3)

Related quasiregular tilings

The trihexagonal tiling exists in a sequence of symmetries of quasiregular tilings with vertex configurations (3.n)2, progressing from tilings of the sphere to the Euclidean plane and into the hyperbolic plane. With orbifold notation symmetry of *n32 all of these tilings are wythoff construction within a fundamental domain of symmetry, with generator points at the right angle corner of the domain.[9][10]

*n32 orbifold symmetries of quasiregular tilings: (3.n)2

Construction		 Spherical Euclidean Hyperbolic
*332 *432 *532 *632 *732 *832... *∞32
Quasiregular
figures
Vertex (3.3)2 (3.4)2 (3.5)2 (3.6)2 (3.7)2 (3.8)2 (3.∞)2

See also

Wikimedia Commons has media related to Uniform tiling 3-6-3-6.

References

  1. 1 2 3 Grünbaum, Branko; Shephard, G. C. (1987). Tilings and Patterns. New York: W. H. Freeman. ISBN 0-7167-1193-1. See in particular Theorem 2.1.3, p. 59 (classification of uniform tilings); Figure 2.1.5, p.63 (illustration of this tiling), Theorem 2.9.1, p. 103 (classification of colored tilings), Figure 2.9.2, p. 105 (illustration of colored tilings), Figure 2.5.3(d), p. 83 (topologically equivalent star tiling), and Exercise 4.1.3, p. 171 (topological equivalence of trihexagonal and two-triangle tilings).
  2. ↑ Williams, Robert (1979). The Geometrical Foundation of Natural Structure: A Source Book of Design. Dover Publications, Inc. p. 38. ISBN 0-486-23729-X.
  3. ↑ Aiton, E. J.; Duncan, Alistair Matheson; Field, Judith Veronica, eds. (1997), The Harmony of the World by Johannes Kepler, Memoirs of the American Philosophical Society 209, American Philosophical Society, pp. 104–105, ISBN 9780871692092.
  4. ↑ Conway, John H.; Burgiel, Heidi; Goodman-Strauss, Chaim (2008). "Chapter 21: Naming Archimedean and Catalan polyhedra and tilings; Euclidean plane tessellations". The Symmetries of Things. Wellesley, MA: A K Peters, Ltd. p. 288. ISBN 978-1-56881-220-5. MR 2410150.
  5. ↑ Mekata, Mamoru (February 2003). "Kagome: The story of the basketweave lattice". Physics Today (AIP Publishing) 56 (2): 12–13. doi:10.1063/1.1564329.
  6. 1 2 Lawler, Michael J.; Kee, Hae-Young; Kim, Yong Baek; Vishwanath, Ashvin (June 2008). "Topological spin liquid on the hyperkagome lattice of Na4Ir3O8". Physical Review Letters 100 (22). arXiv:0705.0990. doi:10.1103/physrevlett.100.227201.
  7. ↑ Yen, F., Chaudhury, R. P., Galstyan, E., Lorenz, B., Wang, Y. Q., Sun, Y. Y., Chu, C. W. (2008). "Magnetic phase diagrams of the Kagome staircase compound Co3V2O8". Physica B: Condensed Matter 403: 1487–1489. doi:10.1016/j.physb.2007.10.334.
  8. ↑ Steurer, Walter; Deloudi, Sofia (2009). Crystallography of Quasicrystals: Concepts, Methods and Structures. Springer Series in Materials Science 126. Springer. p. 20. ISBN 9783642018992.
  9. ↑ Coxeter Regular Polytopes, Third edition, (1973), Dover edition, ISBN 0-486-61480-8 (Chapter V: The Kaleidoscope, Section: 5.7 Wythoff's construction)
  10. ↑ Two Dimensional symmetry Mutations by Daniel Huson
Wikimedia Commons has media related to Kagome structures.
This article is issued from Wikipedia - version of the Saturday, September 26, 2015. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.