# Physics:Hexagonal crystal family

(Redirected from Chemistry:Trigonal)
Short description: Union of crystal groups with related structures and lattices
Crystal system Lattice system Example Trigonal Hexagonal Rhombohedral Hexagonal Dolomite α-Quartz Beryl

In crystallography, the hexagonal crystal family is one of the six crystal families, which includes two crystal systems (hexagonal and trigonal) and two lattice systems (hexagonal and rhombohedral). While commonly confused, the trigonal crystal system and the rhombohedral lattice system are not equivalent (see section crystal systems below).[1] In particular, there are crystals with trigonal symmetry but belong to the hexagonal lattice (such as α-Quartz).

The hexagonal crystal family consists of the 12 point groups such that at least one of their space groups has the hexagonal lattice as underlying lattice, and is the union of the hexagonal crystal system and the trigonal crystal system.[2] There are 52 space groups associated with it, which are exactly those whose Bravais lattice is either hexagonal or rhombohedral.

## Lattice systems

The hexagonal crystal family consists of two lattice systems: hexagonal and rhombohedral. Each lattice system consists of one Bravais lattice.

Relation between the two settings for the rhombohedral lattice
Hexagonal crystal family
Bravais lattice Hexagonal Rhombohedral
Pearson symbol hP hR
Hexagonal
unit cell
Rhombohedral
unit cell

In the hexagonal family, the crystal is conventionally described by a right rhombic prism unit cell with two equal axes (a by a), an included angle of 120° (γ) and a height (c, which can be different from a) perpendicular to the two base axes.

The hexagonal unit cell for the rhombohedral Bravais lattice is the R-centered cell, consisting of two additional lattice points which occupy one body diagonal of the unit cell. There are two ways to do this, which can be thought of as two notations which represent the same structure. In the usual so-called obverse setting, the additional lattice points are at coordinates (​23, ​13, ​13) and (​13, ​23, ​23), whereas in the alternative reverse setting they are at the coordinates (​13,​23,​13) and (​23,​13,​23).[3] In either case, there are 3 lattice points per unit cell in total and the lattice is non-primitive.

The Bravais lattices in the hexagonal crystal family can also be described by rhombohedral axes.[4][5] The unit cell is a rhombohedron (which gives the name for the rhombohedral lattice). This is a unit cell with parameters a = b = c; α = β = γ ≠ 90°.[6] In practice, the hexagonal description is more commonly used because it is easier to deal with a coordinate system with two 90° angles. However, the rhombohedral axes are often shown (for the rhombohedral lattice) in textbooks because this cell reveals 3m symmetry of crystal lattice.

The rhombohedral unit cell for the hexagonal Bravais lattice is the D-centered[7] cell, consisting of two additional lattice points which occupy one body diagonal of the unit cell with coordinates (​13, ​13, ​13) and (​23, ​23, ​23). However, such a description is rarely used.

## Crystal systems

Crystal system Required symmetries of point group Point groups Space groups Bravais lattices Lattice system
Trigonal 1 threefold axis of rotation 5 7 1 Rhombohedral
18 1 Hexagonal
Hexagonal 1 sixfold axis of rotation 7 27

The hexagonal crystal family consists of two crystal systems: trigonal and hexagonal. A crystal system is a set of point groups in which the point groups themselves and their corresponding space groups are assigned to a lattice system (see table in Crystal system).

The trigonal crystal system consists of the 5 point groups that have a single three-fold rotation axis, which includes space groups 143 to 167. These 5 point groups have 7 corresponding space groups (denoted by R) assigned to the rhombohedral lattice system and 18 corresponding space groups (denoted by P) assigned to the hexagonal lattice system. Hence, the trigonal crystal system is the only crystal system whose point groups have more than one lattice system associated with their space groups.

The hexagonal crystal system consists of the 7 point groups that have a single six-fold rotation axis. These 7 point groups have 27 space groups (168 to 194), all of which are assigned to the hexagonal lattice system.

### Trigonal crystal system

The 5 point groups in this crystal system are listed below, with their international number and notation, their space groups in name and example crystals.[8][9][10]

Space group no. Point group Type Examples Space groups
Name[11] Intl Schoen. Orb. Cox. Hexagonal Rhombohedral
143–146 Trigonal pyramidal 3 C3 33 [3]+ enantiomorphic polar carlinite, jarosite P3, P31, P32 R3
147–148 Rhombohedral 3 C3i (S6) [2+,6+] centrosymmetric dolomite, ilmenite P3 R3
149–155 Trigonal trapezohedral 32 D3 223 [2,3]+ enantiomorphic abhurite, alpha-quartz (152, 154), cinnabar P312, P321, P3112, P3121, P3212, P3221 R32
156–161 Ditrigonal pyramidal 3m C3v *33 [3] polar schorl, cerite, tourmaline, alunite, lithium tantalate P3m1, P31m, P3c1, P31c R3m, R3c
162–167 Ditrigonal scalenohedral 3m D3d 2*3 [2+,6] centrosymmetric antimony, hematite, corundum, calcite, bismuth P31m, P31c, P3m1, P3c1 R3m, R3c

### Hexagonal crystal system

The 7 point groups (crystal classes) in this crystal system are listed below, followed by their representations in Hermann–Mauguin or international notation and Schoenflies notation, and mineral examples, if they exist.[2][12]

Space group no. Point group Type Examples Space groups
Name[11] Intl Schoen. Orb. Cox.
168–173 Hexagonal pyramidal 6 C6 66 [6]+ enantiomorphic polar nepheline, cancrinite P6, P61, P65, P62, P64, P63
174 Trigonal dipyramidal 6 C3h 3* [2,3+] laurelite and boric acid P6
175–176 Hexagonal dipyramidal 6/m C6h 6* [2,6+] centrosymmetric apatite, vanadinite P6/m, P63/m
177–182 Hexagonal trapezohedral 622 D6 226 [2,6]+ enantiomorphic kalsilite and high quartz P622, P6122, P6522, P6222, P6422, P6322
183–186 Dihexagonal pyramidal 6mm C6v *66 [6] polar greenockite, wurtzite[13] P6mm, P6cc, P63cm, P63mc
187–190 Ditrigonal dipyramidal 6m2 D3h *223 [2,3] benitoite P6m2, P6c2, P62m, P62c
191–194 Dihexagonal dipyramidal 6/mmm D6h *226 [2,6] centrosymmetric beryl P6/mmm, P6/mcc, P63/mcm, P63/mmc

## Hexagonal close packed

Main page: Close-packing of equal spheres
Hexagonal close packed (hcp) unit cell

Hexagonal close packed (hcp) is one of the two simple types of atomic packing with the highest density, the other being the face-centered cubic (fcc). However, unlike the fcc, it is not a Bravais lattice, as there are two nonequivalent sets of lattice points. Instead, it can be constructed from the hexagonal Bravais lattice by using a two-atom motif (the additional atom at about (​23, ​13, ​12)) associated with each lattice point.[14]

## In two dimensions

Main page: Hexagonal lattice

There is only one hexagonal Bravais lattice in two dimensions: the hexagonal lattice.

Bravais lattice Hexagonal
Pearson symbol hp
Unit cell

## References

1. Hahn (2002)
2. Dana, James Dwight; Hurlbut, Cornelius Searle (1959). Dana's Manual of Mineralogy (17th ed.). New York: Chapman Hall. pp. 78–89.
3. Edward Prince (2004). Mathematical Techniques in Crystallography and Materials Science. Springer Science & Business Media. p. 41.
4. Ashcroft, Neil W.; Mermin, N. David (1976). Solid State Physics (1st ed.). p. 119. ISBN 0-03-083993-9.
5. Hahn (2002), p. 73
6. Pough, Frederick H.; Peterson, Roger Tory (1998). A Field Guide to Rocks and Minerals. Houghton Mifflin Harcourt. p. 62. ISBN 0-395-91096-X.
7. Hurlbut, Cornelius S.; Klein, Cornelis (1985). Manual of Mineralogy (20th ed.). pp. 78–89. ISBN 0-471-80580-7.
8. Hahn (2002), p. 794
9. "Crystallography". Webmineral.com.
10. Jaswon, Maurice Aaron (1965-01-01) (in en). An introduction to mathematical crystallography. American Elsevier Pub. Co..