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Hexagonal crystal family

  (Redirected from Hexagonal crystal system)
Crystal system Trigonal Hexagonal
Lattice system Rhombohedral.svg
Hexagonal latticeFRONT.svg
Example Dolomite Morocco.jpg
Cinnabar on Dolomite.jpg

In crystallography, the hexagonal crystal family is one of the 6 crystal families, which includes 2 crystal systems (hexagonal and trigonal) and 2 lattice systems (hexagonal and rhombohedral).

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.[1] There are 52 space groups associated with it, which are exactly those whose Bravais lattice is either hexagonal or rhombohedral.


Lattice systemsEdit

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
Conventional hexagonal
unit cell
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 conventional cell for the rhombohedral Bravais lattice is the rhombohedrally-centered (R-centered) hexagonal cell, consisting of two additional lattice points which occupy one body diagonal of the unit cell with coordinates (​23, ​13, ​13) and (​13, ​23, ​23). Hence, 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.[2][3] The unit cell is a rhombohedron (which gives the name for the rhombohedral lattice system). This is a unit cell with parameters a = b = c; α = β = γ ≠ 90°.[4] 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 unit cell for the hexagonal Bravais lattice in rhombohedral axes, consisting of two additional lattice points which occupy one body diagonal of the unit cell with coordinates (​13, ​13, ​13) and (​23, ​23, ​23), is called the hexagonally-centered (D-centered)[5] rhombohedral cell. However, such a description is rarely used.

Crystal systemsEdit

Crystal system Required symmetries of point group Point groups Space groups Lattice system
Trigonal 1 threefold axis of rotation 5 7 Rhombohedral
18 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#Crystal classes).

The trigonal crystal system consists of the 5 point groups that have a single three-fold rotation axis. These 5 point groups (space groups 143 to 167) 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.

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. Graphite is an example of a crystal that crystallizes in the hexagonal crystal system.

Crystal classesEdit

Trigonal crystal systemEdit

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 and rhombohedral lattices both appear.

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. (All these point groups are also associated with some space groups not in the rhombohedral lattice system.)[6][7][8]

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

Hexagonal crystal systemEdit

The 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.[1][9]

Space group no. Point group Examples Space groups
Class Intl Schoen. Orb. Cox.
168–173 Hexagonal pyramidal 6 C6 66 [6]+ 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+] apatite, vanadinite P6/m, P63/m
177–182 Hexagonal trapezohedral 622 D6 226 [2,6]+ kalsilite and high quartz P622, P6122, P6522, P6222, P6422, P6322
183–186 Dihexagonal pyramidal 6mm C6v *66 [6] greenockite, wurtzite [10] 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] beryl P6/mmm, P6/mcc, P63/mcm, P63/mmc

Example: QuartzEdit

Quartz mineral embedded in limestone (top right of the sample), easily identifiable by its hexagonal form.

Quartz is a crystal that belongs to the hexagonal lattice system but exists in two polymorphs that are in two different crystal systems. The crystal structures of α-quartz are described by two of the 18 space groups (152 and 154) associated with the trigonal crystal system, while the crystal structures of β-quartz are described by two of the 27 space groups (180 and 181) associated with the hexagonal crystal system.

Rhombohedral lattice angleEdit

The lattice angles and the lengths of the lattice vectors are all the same for both the cubic and rhombohedral lattice systems. The lattice angles for simple cubic, face-centered cubic, and body-centered cubic lattices are π/2 radians, π/3 radians, and arccos(-1/3) radians, respectively.[11] A rhombohedral lattice will result from lattice angles other than these.

Hexagonal close packedEdit

Note that the atom in the body center of the hexagonal close packed (hcp) unit cell in the hexagonal lattice system does not appear in the unit cell of the hexagonal lattice. It is part of the two atom motif (the additional atom at about (​23,​13,​12)) associated with each lattice point in the underlying lattice.[12]

See alsoEdit


  1. ^ a b Dana, James Dwight; Hurlbut, Cornelius Searle (1959). Dana's Manual of Mineralogy (17th ed.). New York: Chapman Hall. pp. 78–89. 
  2. ^ "Page not found - QuantumWise". 
  3. ^ "Medium-Resolution Space Group Diagrams and Tables". 
  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. ^ "Crystallography and Minerals Arranged by Crystal Form". Webmineral. 
  9. ^ "Crystallography". Retrieved 2014-08-03. 
  10. ^ "Minerals in the Hexagonal crystal system, Dihexagonal Pyramidal class (6mm)". Retrieved 2014-08-03. 
  11. ^ Hahn (2002), p. 747
  12. ^ Jaswon, Maurice Aaron (1965-01-01). An introduction to mathematical crystallography. American Elsevier Pub. Co. 

Further readingEdit

External linksEdit