View source for Bravais lattice

{{short description|Geometry and crystallography point array}}
{{Use dmy dates|date=February 2023}}
[[File:Lattice systems.png|thumb|The seven lattice systems and their Bravais lattices in three dimensions]]

In [[geometry]] and [[crystallography]], a '''Bravais lattice''', named after {{harvs|txt|first=Auguste |last=Bravais|year=1850|authorlink=Auguste Bravais}},<ref>{{cite journal|last1 = Aroyo|first1 = Mois I.|first2 = Ulrich|last2 = Müller|first3 = Hans|last3 = Wondratschek|title = Historical Introduction|journal = International Tables for Crystallography|volume = A1|issue = 1.1|pages = 2–5|year = 2006|url = http://it.iucr.org/A1a/ch1o1v0001/sec1o1o1/|doi = 10.1107/97809553602060000537|access-date = 2008-04-21|url-status = dead|archive-url = https://archive.today/20130704032928/http://it.iucr.org/A1a/ch1o1v0001/sec1o1o1/|archive-date = 2013-07-04|citeseerx = 10.1.1.471.4170}}</ref> is an infinite array of [[discrete point]]s generated by a set of [[Translation operator (quantum mechanics)#Discrete Translational Symmetry|discrete translation]] operations described in three dimensional space by

: <math>\mathbf{R} = n_1 \mathbf{a}_1 + n_2 \mathbf{a}_2 + n_3 \mathbf{a}_3,</math>

where the ''n<sub>i</sub>'' are any integers, and '''a'''<sub>''i''</sub> are ''primitive translation vectors'', or ''primitive vectors'', which lie in different directions (not necessarily mutually perpendicular) and span the lattice. The choice of primitive vectors for a given Bravais lattice is not unique. A fundamental aspect of any Bravais lattice is that, for any choice of direction, the lattice appears exactly the same from each of the discrete lattice points when looking in that chosen direction.

The Bravais lattice concept is used to formally define a ''crystalline arrangement'' and its (finite) frontiers. A [[crystal]] is made up of one or more atoms, called the ''basis'' or ''motif'', at each lattice point. The ''basis'' may consist of [[atom]]s, [[molecule]]s, or [[polymer]] strings of [[Solid|solid matter]], and the lattice provides the locations of the basis. 

Two Bravais lattices are often considered equivalent if they have isomorphic [[symmetry group]]s. In this sense, there are 5 possible Bravais lattices in 2-dimensional space and 14 possible Bravais lattices in 3-dimensional space. The 14 possible symmetry groups of Bravais lattices are 14 of the 230 [[space group]]s. In the context of the space group classification, the Bravais lattices are also called Bravais classes, Bravais arithmetic classes, or Bravais flocks.<ref>{{cite web |title=Bravais class |url=http://reference.iucr.org/dictionary/Bravais_class |website=Online Dictionary of Crystallography |publisher=IUCr |access-date=8 August 2019}}</ref>

==Unit cell==
{{Main|Unit cell}}
In crystallography, there is the concept of a unit cell which comprises the space between adjacent lattice points as well as any atoms in that space. A unit cell is defined as a space that, when translated through a subset of all vectors described by <math>\mathbf{R} = n_{1}\mathbf{a}_{1} + n_{2}\mathbf{a}_{2} + n_{3}\mathbf{a}_{3}</math>, fills the lattice space without overlapping or voids. (I.e., a lattice space is a multiple of a unit cell.)<ref name=":0">{{Cite book|last1=Ashcroft|first1=Neil|title=Solid State Physics|last2=Mermin|first2=Nathaniel|publisher=Saunders College Publishing|year=1976|isbn=0030839939|pages=71–72}}</ref> 

There are mainly two types of unit cells: primitive unit cells and conventional unit cells. A primitive cell is the very smallest component of a lattice (or crystal) which, when stacked together with lattice translation operations, reproduces the whole lattice (or crystal).<ref>{{Cite web|title=Materials & Solid State Chemistry (course notes)|author= Peidong Yang|url=http://nanowires.berkeley.edu/teaching/253a/2016/253A-2016-01.pdf|year=2016|department=UC Berkeley|series=Chem 253}}</ref> Note that the translations must be lattice translation operations that cause the lattice to appear unchanged after the translation. If arbitrary translations were allowed, one could make a primitive cell half the size of the true one, and translate twice as often, as an example. 

Another way of defining the size of a primitive cell that avoids invoking lattice translation operations, is to say that the primitive cell is the smallest possible component of a lattice (or crystal) that can be repeated to reproduce the whole lattice (or crystal), ''and'' that contains exactly one lattice point. In either definition, the primitive cell is characterized by its small size. 

There are clearly many choices of cell that can reproduce the whole lattice when stacked (two lattice halves, for instance), and the minimum size requirement distinguishes the primitive cell from all these other valid repeating units. If the lattice or crystal is 2-dimensional, the primitive cell has a minimum area; likewise in 3 dimensions the primitive cell has a minimum volume. 

Despite this rigid minimum-size requirement, there is not one unique choice of primitive unit cell. In fact, all cells whose borders are primitive translation vectors will be primitive unit cells. The fact that there is not a unique choice of primitive translation vectors for a given lattice leads to the multiplicity of possible primitive unit cells. Conventional unit cells, on the other hand, are not necessarily minimum-size cells. They are chosen purely for convenience and are often used for illustration purposes. They are loosely defined.

===Primitive unit cell===
Primitive unit cells are defined as unit cells with the smallest volume for a given crystal. (A crystal is a lattice and a basis at every lattice point.) To have the smallest cell volume, a primitive unit cell must contain (1) only one lattice point and (2) the minimum amount of basis constituents (e.g., the minimum number of atoms in a basis). For the former requirement, counting the number of lattice points in a unit cell is such that, if a lattice point is shared by ''m'' adjacent unit cells around that lattice point, then the point is counted as 1/''m''. The latter requirement is necessary since there are crystals that can be described by more than one combination of a lattice and a basis. For example, a crystal, viewed as a lattice with a single kind of atom located at every lattice point (the simplest basis form), may also be viewed as a lattice with a basis of two atoms. In this case, a primitive unit cell is a unit cell having only one lattice point in the first way of describing the crystal in order to ensure the smallest unit cell volume.

There can be more than one way to choose a primitive cell for a given crystal and each choice will have a different primitive cell shape, but the primitive cell volume is the same for every choice and each choice will have the property that a one-to-one correspondence can be established between primitive unit cells and discrete lattice points over the associated lattice. All primitive unit cells with different shapes for a given crystal have the same volume by definition; For a given crystal, if ''n'' is the density of lattice points in a lattice ensuring the minimum amount of basis constituents and ''v'' is the volume of a chosen primitive cell, then ''nv'' = 1 resulting in ''v'' = 1/''n'', so every primitive cell has the same volume of 1/''n''.<ref name=":0" />

Among all possible primitive cells for a given crystal, an obvious primitive cell may be the [[parallelepiped]] formed by a chosen set of primitive translation vectors. (Again, these vectors must make a lattice with the minimum amount of basis constituents.)<ref name=":0" /> That is, the set of all points <math>\mathbf{r} = x_{1}\mathbf{a}_{1} + x_{2}\mathbf{a}_{2} + x_{3}\mathbf{a}_{3}</math> where <math>0 \le x_{i} < 1</math> and <math>\mathbf{a}_{i}</math> is the chosen primitive vector. This primitive cell does not always show the clear symmetry of a given crystal. In this case, a conventional unit cell easily displaying the crystal symmetry is often used. The conventional unit cell volume will be an integer-multiple of the primitive unit cell volume.

== Origin of concept ==
{{See also|Crystallographic point group}}
In two dimensions, any lattice can be specified by the length of its two primitive translation vectors and the angle between them. There are an infinite number of possible lattices one can describe in this way. Some way to categorize different types of lattices is desired. One way to do so is to recognize that some lattices have inherent symmetry. One can impose conditions on the length of the primitive translation vectors and on the angle between them to produce various symmetric lattices. These symmetries themselves are categorized into different types, such as point groups (which includes mirror symmetries, inversion symmetries and rotation symmetries) and translational symmetries. Thus, lattices can be categorized based on what point group or translational symmetry applies to them.

In two dimensions, the most basic point group corresponds to rotational invariance under 2π and π, or 1- and 2-fold rotational symmetry. This actually applies automatically to all 2D lattices, and is the most general point group. Lattices contained in this group (technically all lattices, but conventionally all lattices that don't fall into any of the other point groups) are called oblique lattices. From there, there are 4 further combinations of point groups with translational elements (or equivalently, 4 types of restriction on the lengths/angles of the primitive translation vectors) that correspond to the 4 remaining lattice categories: square, hexagonal, rectangular, and centered rectangular. Thus altogether there are 5 Bravais lattices in 2 dimensions.

Likewise, in 3 dimensions, there are 14 Bravais lattices: 1 general "wastebasket" category (triclinic) and 13 more categories. These 14 lattice types are classified by their point groups into 7 lattice systems (triclinic, monoclinic, orthorhombic, tetragonal, cubic, rhombohedral, and hexagonal).

==In 2 dimensions==
{{further|Lattice (group)}}
In two-dimensional space there are 5 Bravais lattices,<ref>{{cite book |last=Kittel |first=Charles |title=[[Introduction to Solid State Physics]] |orig-year=1953 |chapter-url= http://www.wiley.com/WileyCDA/WileyTitle/productCd-047141526X.html |access-date=2008-04-21 |edition=Seventh  |year=1996 |publisher=John Wiley & Sons |location=New York  |isbn=978-0-471-11181-8 |pages=10 |chapter=Chapter 1}}</ref> grouped into four [[lattice system]]s, shown in the table below. Below each diagram is the Pearson symbol for that Bravais lattice.

'''Note:''' In the unit cell diagrams in the following table the lattice points are depicted using black circles and the unit cells are depicted using parallelograms (which may be squares or rectangles) outlined in black. Although each of the four corners of each parallelogram connects to a lattice point, only one of the four lattice points technically belongs to a given unit cell and each of the other three lattice points belongs to one of the adjacent unit cells. This can be seen by imagining moving the unit cell parallelogram slightly left and slightly down while leaving all the black circles of the lattice points fixed.

{| class=wikitable
! rowspan=2| Lattice system
! rowspan=2| Point group <br />([[Schoenflies notation|Schönflies notation]])
! colspan=2| 5 Bravais lattices
|-
! Primitive (p)
! Centered (c)
|- align=center
! Monoclinic (m)
| C<sub>2</sub>
| [[File:2d mp.svg|90px|Oblique]]<br/>[[Oblique lattice|Oblique]]<br/>(mp)
|
|- align=center
! Orthorhombic (o)
| D<sub>2</sub>
| [[File:2d op rectangular.svg|110px|Oblique]]<br/>[[Rectangular lattice|Rectangular]]<br/>(op)
| [[File:2d oc rectangular.svg|110px|Oblique]]<br/>Centered rectangular <br/>(oc)
|- align=center
! Tetragonal (t)
| D<sub>4</sub>
| [[File:2d tp.svg|90px|Oblique]]<br/>[[Square lattice|Square]]<br/>(tp)
|
|- align=center
! Hexagonal (h)
| D<sub>6</sub>
| [[File:2d hp.svg|100px|Oblique]]<br/>[[Hexagonal lattice|Hexagonal]]<br/>(hp)
|
|}
{{Clear}}

The unit cells are specified according to the relative lengths of the cell edges (''a'' and ''b'') and the angle between them (''θ''). The area of the unit cell can be calculated by evaluating the [[Vector norm|norm]] {{nowrap|{{norm|'''a''' × '''b'''}}}}, where '''a''' and '''b''' are the lattice vectors. The properties of the lattice systems are given below:

{| class=wikitable
! Lattice system
! Area
! Axial distances (edge lengths)
! Axial angle
|-
! Monoclinic
| <math>ab \, \sin\theta</math>
| 
| 
|-
! Orthorhombic
| <math> ab </math>
| 
| ''θ'' = 90°
|-
! Tetragonal
| <math>a^2</math>
| ''a'' = ''b''
| ''θ'' = 90° 
|-
! Hexagonal
|<math>\frac{\sqrt{3}}{2}\, a^2</math>
| ''a'' = ''b''
| ''θ'' = 120°
|}
{{Clear}}

==In 3 dimensions==
[[File:diamond_lattice.stl|thumb|2&times;2&times;2 unit cells of a [[diamond cubic]] lattice]]
In three-dimensional space there are 14 Bravais lattices. These are obtained by combining one of the seven [[lattice system]]s with one of the centering types. The centering types identify the locations of the lattice points in the unit cell as follows:

*Primitive (P): lattice points on the cell corners only (sometimes called simple)
*Base-centered (S: A, B, or C): lattice points on the cell corners with one additional point at the center of each face of one pair of parallel faces of the cell (sometimes called end-centered)
*Body-centered (I): lattice points on the cell corners, with one additional point at the center of the cell
*Face-centered (F): lattice points on the cell corners, with one additional point at the center of each of the faces of the cell

Not all combinations of lattice systems and centering types are needed to describe all of the possible lattices, as it can be shown that several of these are in fact equivalent to each other. For example, the monoclinic I lattice can be described by a monoclinic C lattice by different choice of crystal axes. Similarly, all A- or B-centred lattices can be described either by a C- or P-centering. This reduces the number of combinations to 14 conventional Bravais lattices, shown in the table below.<ref name=Hahn>{{Cite book|editor1-last=Hahn|editor1-first=Theo|title=International Tables for Crystallography, Volume A: Space Group Symmetry|url=http://it.iucr.org/A/|publisher=[[Springer-Verlag]]|location=Berlin, New York|edition=5th|isbn=978-0-7923-6590-7|doi=10.1107/97809553602060000100|year=2002|volume=A}}</ref>{{rp|744}} Below each diagram is the [[Pearson symbol]] for that Bravais lattice.

'''Note:''' In the unit cell diagrams in the following table all the lattice points on the cell boundary (corners and faces) are shown; however, not all of these lattice points technically belong to the given unit cell.  This can be seen by imagining moving the unit cell slightly in the negative direction of each axis while keeping the lattice points fixed. Roughly speaking, this can be thought of as moving the unit cell slightly left, slightly down, and slightly out of the screen. This shows that only one of the eight corner lattice points (specifically the front, left, bottom one) belongs to the given unit cell (the other seven lattice points belong to adjacent unit cells). In addition, only one of the two lattice points shown on the top and bottom face in the ''Base-centered'' column belongs to the given unit cell. Finally, only three of the six lattice points on the faces in the ''Face-centered'' column belong to the given unit cell.

{| class=wikitable
! rowspan=2| Crystal family
! rowspan=2| Lattice system
! rowspan=2| Point group <br />([[Schoenflies notation|Schönflies notation]])
! colspan=4| 14 Bravais lattices
|-
! Primitive (P)
! Base-centered (S)
! Body-centered (I)
! Face-centered (F)
|- align=center
! colspan=2| [[Triclinic]] (a)
| C<sub>i</sub>
| [[File:Triclinic.svg|80px|Triclinic]]
aP
|
|
|
|- align=center
! colspan=2| [[Monoclinic]] (m)
| C<sub>2h</sub>
| [[File:Monoclinic.svg|80px|Monoclinic, simple]]
mP
| [[File:Base-centered monoclinic.svg|80px|Monoclinic, centered]]
mS
|
|
|- align=center
! colspan=2| [[Orthorhombic]] (o)
| D<sub>2h</sub>
| [[File:Orthorhombic.svg|80px|Orthorhombic, simple]]
oP
| [[File:Orthorhombic-base-centered.svg|80px|Orthorhombic, base-centered]]
oS
| [[File:Orthorhombic-body-centered.svg|80px|Orthorhombic, body-centered]]
oI
| [[File:Orthorhombic-face-centered.svg|80px|Orthorhombic, face-centered]]
oF
|- align=center
! colspan=2| [[Tetragonal]] (t)
| D<sub>4h</sub>
| [[File:Tetragonal.svg|80px|Tetragonal, simple]]
tP
|
| [[File:Tetragonal-body-centered.svg|80px|Tetragonal, body-centered]]
tI
|
|- align=center
! rowspan=2| [[Hexagonal crystal family|Hexagonal]] (h)
! Rhombohedral
| D<sub>3d</sub>
| [[File:Rhombohedral.svg|80px|Rhombohedral]]
hR
|
|
|
|- align=center
! Hexagonal
| D<sub>6h</sub>
| [[File:Hexagonal latticeFRONT.svg|80px|Hexagonal]]
hP
|
|
|
|- align=center
! colspan=2| [[Cubic crystal system|Cubic]] (c)
| O<sub>h</sub>
| [[File:Cubic.svg|80px|Cubic, simple]]
cP
|
| [[File:Cubic-body-centered.svg|80px|Cubic, body-centered]]
cI
| [[File:Cubic-face-centered.svg|80px|Cubic, face-centered]]
cF
|}
{{Clear}}

The unit cells are specified according to six [[unit cell|lattice parameters]] which are the relative lengths of the cell edges (''a'', ''b'', ''c'') and the angles between them (''α'', ''β'', ''γ''), where ''α'' is the angle between ''b'' and ''c'', ''β'' is the angle between ''a'' and ''c'', and ''γ'' is the angle between ''a'' and ''b''. The volume of the unit cell can be calculated by evaluating the [[triple product]] {{nowrap|'''a''' · ('''b''' × '''c''')}}, where '''a''', '''b''', and '''c''' are the lattice vectors. The properties of the lattice systems are given below:

{| class=wikitable
! Crystal family
! Lattice system
! Volume
! Axial distances (edge lengths){{r|"Hahn"|p=758}}
! Axial angles<ref name="Hahn"/>
! Corresponding examples
|-
! colspan=2| [[Triclinic]]
| <math>abc \sqrt{1-\cos^2\alpha-\cos^2\beta-\cos^2\gamma+2\cos\alpha \cos\beta \cos\gamma}</math>
|
|
| [[Potassium dichromate|K<sub>2</sub>Cr<sub>2</sub>O<sub>7</sub>]], [[Copper(II) sulfate|CuSO<sub>4</sub>·5H<sub>2</sub>O]], [[Boric acid|H<sub>3</sub>BO<sub>3</sub>]]
|-
! colspan=2| [[Monoclinic]]
| <math>abc \, \sin\beta</math>
| 
| ''α'' = ''γ'' = 90°
| [[Allotropes of sulphur|Monoclinic sulphur]], [[Sodium sulfate|Na<sub>2</sub>SO<sub>4</sub>·10H<sub>2</sub>O]], [[Lead(II) chromate|PbCrO<sub>3</sub>]]
|-
! colspan=2| [[Orthorhombic]]
| <math> abc </math>
| 
| ''α'' = ''β'' = ''γ'' = 90°
| [[Allotropes of sulfur|Rhombic sulphur]], [[Potassium nitrate|KNO<sub>3</sub>]], [[Barium sulfate|BaSO<sub>4</sub>]]
|-
! colspan=2| [[Tetragonal]]
| <math> a^2c </math>
| ''a'' = ''b''
| ''α'' = ''β'' = ''γ'' = 90°
| [[White tin]], [[Tin dioxide|SnO<sub>2</sub>]], [[Titanium dioxide|TiO<sub>2</sub>]], [[Calcium sulfate|CaSO<sub>4</sub>]]
|-
! rowspan=2| [[Hexagonal crystal family|Hexagonal]]
! Rhombohedral
| <math> a^3 \sqrt{1 - 3\cos^2\alpha + 2\cos^3\alpha} </math>
| ''a'' = ''b'' = ''c''
| ''α'' = ''β'' = ''γ'' 
| [[Calcite]] (CaCO<sub>3</sub>), [[cinnabar]] (HgS)
|-
! Hexagonal
| <math>\frac{\sqrt{3}}{2}\, a^2c</math>
| ''a'' = ''b''
| ''α'' = ''β'' = 90°, ''γ'' = 120°
| [[Graphite]], [[Zinc oxide|ZnO]], [[Cadmium sulphide|CdS]]
|-
! colspan=2| [[Cubic crystal system|Cubic]]
| <math> a^3</math>
| ''a'' = ''b'' = ''c''
| ''α'' = ''β'' = ''γ'' = 90°
| [[Sodium chloride|NaCl]], [[zinc blende]], [[copper|copper metal]], [[Potassium chloride|KCl]], [[Diamond]], [[Silver]]
|}
{{Clear}}

Some basic information for the lattice systems and Bravais lattices in three dimensions is summarized in the diagram at the beginning of this page. The seven sided polygon (heptagon) and the number 7 at the centre indicate the seven lattice systems. The inner heptagons indicate the lattice angles, lattice parameters, Bravais lattices and Schöenflies notations for the respective lattice systems.

==In 4 dimensions==

In four dimensions, there are 64 Bravais lattices. Of these, 23 are primitive and 41 are centered. Ten Bravais lattices split into [[enantiomorphic]] pairs.<ref>{{Citation | last1=Brown | first1=Harold | last2=Bülow | first2=Rolf | last3=Neubüser | first3=Joachim | last4=Wondratschek | first4=Hans | last5=Zassenhaus | first5=Hans | author5-link=Hans Zassenhaus | title=Crystallographic groups of four-dimensional space | publisher=Wiley-Interscience [John Wiley & Sons] | location=New York | isbn=978-0-471-03095-9 | mr=0484179  | year=1978}}</ref>

==See also==
{{div col|colwidth=30em}}
*[[Crystal habit]]
*[[Crystal system]]
*[[einstein problem]]
*[[Miller index]]
*[[Reciprocal lattice]]
*[[Translation operator (quantum mechanics)]]
*[[Translational symmetry]]
*[[Zone axis]]
{{div col end}}

==References==
{{Reflist}}

==Further reading==
*{{Cite journal|last=Bravais|first= A. |year=1850|title= Mémoire sur les systèmes formés par les points distribués régulièrement sur un plan ou dans l'espace|language=fr|trans-title=Memoir on the systems formed by points regularly distributed on a plane or in space|journal= J. École Polytech.|volume= 19|pages= 1–128}} (English: Memoir 1, Crystallographic Society of America, 1949).

==External links==
*[http://www.math.rwth-aachen.de/~Gabriele.Nebe/LATTICES/ Catalogue of Lattices (by Nebe and Sloane)]
*{{Cite web|url=http://www.haverford.edu/physics-astro/songs/bravais.htm |first=Walter Fox |last=Smith
|title=The Bravais Lattices Song|year=2002}}

{{Crystal systems}}
{{Crystallography}}

[[Category:Crystallography]]
[[Category:Tessellation]]
[[Category:Lattice points]]

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