Hexagonal crystal family

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Crystal system
Trigonal
Hexagonal
Lattice system

Rhombohedral.svg
Rhombohedral

Hexagonal latticeFRONT.svg
Hexagonal
Example

Dolomite Morocco.jpg
Dolomite

Cinnabar on Dolomite.jpg
Cinnabar

Berillo.jpg
Beryl

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.





Contents





  • 1 Lattice systems


  • 2 Crystal systems


  • 3 Crystal classes

    • 3.1 Trigonal crystal system


    • 3.2 Hexagonal crystal system



  • 4 Hexagonal close packed


  • 5 Example: Quartz


  • 6 Rhombohedral lattice angle


  • 7 See also


  • 8 References


  • 9 Further reading


  • 10 External links




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

Hexagonal, primitive

Hexagonal, R-centered

Rhombohedral
unit cell

Rhombohedral, D-centered

Rhombohedral, primitive

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 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 rhombohedral unit cell for the hexagonal Bravais lattice is the D-centered[5] 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

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 classes



Trigonal crystal system


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
Type
Examples
Space groups
Name[9]
Intl

Schoen.

Orb.

Cox.
Hexagonal
Rhombohedral
143–146
Trigonal pyramidal
3C333[3]+
enantiomorphic polar

carlinite, jarosite
P3, P31, P32R3
147–148
Rhombohedral
3C3i (S6)[2+,6+]

centrosymmetric

dolomite, ilmenite
P3
R3
149–155
Trigonal trapezohedral
32D3223[2,3]+
enantiomorphic

abhurite, alpha-quartz (152, 154), cinnabar
P312, P321, P3112, P3121, P3212, P3221R32
156–161

Ditrigonal pyramidal
3mC3v*33[3]

polar

schorl, cerite, tourmaline, alunite, lithium tantalate
P3m1, P31m, P3c1, P31cR3m, R3c
162–167
Ditrigonal scalenohedral

3m
D3d2*3[2+,6]

centrosymmetric

antimony, hematite, corundum, calcite, bismuth
P31m, P31c, P3m1, P3c1R3m, R3c


Hexagonal crystal system


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][10]











































































Space group no.
Point group
Type
Examples
Space groups
Name[9]
Intl

Schoen.

Orb.

Cox.
168–173
Hexagonal pyramidal
6C666[6]+
enantiomorphic polar

nepheline, cancrinite
P6, P61, P65, P62, P64, P63
174
Trigonal dipyramidal
6C3h3*[2,3+]


laurelite and boric acid
P6
175–176
Hexagonal dipyramidal
6/mC6h6*[2,6+]

centrosymmetric

apatite, vanadinite
P6/m, P63/m
177–182
Hexagonal trapezohedral
622D6226[2,6]+
enantiomorphic

kalsilite and high quartz
P622, P6122, P6522, P6222, P6422, P6322
183–186
Dihexagonal pyramidal
6mmC6v*66[6]

polar

greenockite, wurtzite [11]
P6mm, P6cc, P63cm, P63mc
187–190
Ditrigonal dipyramidal

6m2
D3h*223[2,3]


benitoite
P6m2, P6c2, P62m, P62c
191–194
Dihexagonal dipyramidal
6/mmmD6h*226[2,6]

centrosymmetric

beryl
P6/mmm, P6/mcc, P63/mcm, P63/mmc


Hexagonal close packed





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.[12]




Example: Quartz




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 angle


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.[13] A rhombohedral lattice will result from lattice angles other than these.



See also


  • Crystal structure


  • Close-packing (hcp)

  • Wurtzite (crystal structure)


References




  1. ^ ab 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". quantumwise.com. 


  3. ^ "Medium-Resolution Space Group Diagrams and Tables". img.chem.ucl.ac.uk. 


  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. ^ ab Hahn (2002), p. 794


  10. ^ "Crystallography". Webmineral.com. Retrieved 2014-08-03. 


  11. ^ "Minerals in the Hexagonal crystal system, Dihexagonal Pyramidal class (6mm)". Mindat.org. Retrieved 2014-08-03. 


  12. ^ Jaswon, Maurice Aaron (1965-01-01). An introduction to mathematical crystallography. American Elsevier Pub. Co. 


  13. ^ Hahn (2002), p. 747




Further reading



  • Hahn, Theo, ed. (2002). International Tables for Crystallography, Volume A: Space Group Symmetry. A (5th ed.). Berlin, New York: Springer-Verlag. doi:10.1107/97809553602060000100. ISBN 978-0-7923-6590-7. 


External links


  • Mineralogy database




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