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Chapter 1 Crystal Structure
• Definition of Crystal and Bravais lattice• Examples of Bravais lattice and crystal structures• Primitive unit cell• Wigner – Seitz unit cell• Miller Indices• Classification of Braivais lattices
Outline
2
• An ideal crystal is constructed by the infinite repetition in space of identical
structural unit.
• The structure of all crystals is described in terms of a lattice with a group of
atoms attached to each lattice point.
Bravais lattice basis
A Bravais lattice is an infinite array of discrete points and appear exactly the
same, from whichever of the points the array is viewed.
A (three dimensional) Bravais lattice consists of all points with
positions vectors of the formR→
→→→→
++= 332211 anananR
1ar
Where are any three vectors and are not all in the same
plane, and n1, n2, and n3 range through all integral values2
ar
3ar
3
A general 2-D Bravais lattice of no particular symmetry
1ar
2ar
'
212122 aaaaPrrrr
+−=+=
O
P
Q
'
2
'
121 2 aaaaQrrrr
+−=+−=
'
2ar
Primitive vectors are not unique
Primitive vectors: 1ar
2ar
or1
ar '
2ar
4
Vortices of a 2-D honeycomb do not form a Bravais lattice
P
Q
R
P and Q are equivalent
P and R are not
5
Simple cubic (sc) structure
xaa ˆ1
=r
yaa ˆ2
=r
zaa ˆ3
=r
1ar
3ar
2ar
Atoms per cubic cell: 1
Body centered cubic (bcc)
A
B
A and B are equivalent
It is a Bravais lattice
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x y
z
1ar
2ar
3ar
)ˆˆˆ(2
1
);ˆˆˆ(2
1
);ˆˆˆ(2
1
3
2
1
zyxaa
zyxaa
zyxaa
+−=
++−=
−+=
r
r
r
Primitive vectors for bcc structure
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An alternative set of primitive vectors for bcc structure
x
y
z
1ar
2ar3
ar
)ˆˆˆ(2
ˆ
ˆ
3
2
1
zyxa
a
yaa
xaa
++=
=
=
r
r
r
Less symmetric compared to previous set
8
Face centered cubic (fcc) structure
Each point can be either a corner point or a face-centering point
It is a Bravais lattice
9
Primitive vectors for fcc structure
)ˆˆ(2
1
)ˆˆ(2
1
)ˆˆ(2
1
3
2
1
xzaa
zyaa
yxaa
+=
+=
+=
r
r
r
1ar
2ar
3ar
x
y
z
10
Primitive unit cell
Primitive unit cell is a volume of space that, when translated through all
the vectors in a Bravais lattice, just fills all the space without either
overlapping itself or leaving voids.
Two ways of defining primitive cell
• Primitive cell is not unique
• A primitive cell must contain exactly one lattice point.
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The obvious primitive cell:
332211axaxaxrrrrr
++=
Is the set of all points of the above form for all xi ranging
continuously between 0 and 1.
It is the parallelipiped spanned by the primitive vectors
1ar
2ar
3ar
Disadvantage: the primitive cell defined as above does not
reflect full symmetry of the Bravais lattice
12
Primitive cell of a bcc Bravais lattice
1ar
2ar3
ar
Primitive cell is a rhombohedron with edge a2
3
Volume of primitive cell is half of the cube
13
x
y
z
1ar
2ar
3ar
Primitive cell of a fcc Bravais lattice
Volume of the primitive cell is ¼ of the cube
14
x
y
z
Simple hexagonal (sc) Bravais lattice and its primitive cell
1ar
2ar
3ar
zca
ya
xaa
ya
xaa
ˆ
ˆ)2
(ˆ)2
3(
ˆ)2
(ˆ)2
3(
3
2
1
=
+−=
+=
r
r
r
zca
yaa
ya
xaa
ˆ
ˆ
ˆ)2
(ˆ)2
3(
3
2
1
=
=
+=
r
r
r
An alternative set:
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Wigner – Seitz primitive cell
• a primitive cell with the full symmetry of the Bravais lattice
• a W-S cell about a lattice point is the region of space that is
closer to that point than to any other lattice point
Wigner – Seitz unit cell about a lattice point can be constructed
by drawing lines connecting the point to all others in the lattice,
bisecting each line with a plane, and taking the smallest
polyhedron containing the point bounded by these plane
hexagon
16
Wigner-Seitz cell of bcc
Wigner-Seitz cell of fcc
Note: the surrounding
cube is not the cubic cell
Truncated octahedron
14 faces (8 regular hexagons and 6 squares)
12 faces (parallelograms)
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Crystal structure: lattice with a basis
A crystal structure consists of identical copies of the same physical
unit, called the basis, located at all the points of a Bravias lattice (or,
equivalently, translated through all the vectors of a Bravais lattice)
Honeycomb net
Basis
Lattice: 2-D triangular lattice
18
Describe a Bravais lattice as a lattice with a basis by choosing a non-
primitive cell (a unit cell)
A unit cell is a region that just fills space without any over-lapping when
translated through some subset of the vectors of a Bravais lattice. It is
usually larger than the primitive cell (by an integer factor)
bcc: Simple cubic unit cell
Basis: 0 )ˆˆˆ(2
zyxa
++
)ˆˆ(2
yxa
+ )ˆˆ(2
zya
+
fcc: Simple cubic unit cell
Basis: 0 )ˆˆ(2
zxa
+
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Diamond structure
• Not a Bravais lattice
• Two interpenetrating fcc Bravais lattice
Bravais lattice : fcc
basis0 )ˆˆˆ(
4
1zyx ++
Coordination number : 4
Four nearest neighbors of each point form the vertices of a
regular tetrahedron
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0 1/2 0
1/2 0 1/2
0 1/2 0
3/4 1/4
1/4 3/4
Atomic positions in the cubic cell of diamond structure projected on (100)
surface
Fractions in circles denote height above the base in units of a cube edge.
21
Hexagonal close-packed (hcp) structure
Bravais lattice: simple hexagonal
Basis: 0321
2
1
3
1
3
2aaarrr
++
Two interpenetrating simple hexagonal Bravais lattice
Four neighboring atoms form the vortices of a tetrahedron
1ar
2ar
3ar
22
Both hcp and fcc can be viewed as close-packed hard spheres
hcp
fcc
Coordination number: 12 for both fcc and hcp
23
Fcc is close packed structure
The (111) plane equivalent to the triangular close packed hard sphere
layer
Try calculating packing density
24
Basis consisting of different atoms
NaCl
CsCl
Bravais lattice: fcc
Basis: Cl- at (0,0,0) and Na+ at (1/2,1/2,1/2)
Bravais lattice: sc
Basis: Cs+ at (0,0,0) and Cl- at (1/2,1/2,1/2)
25
Miller indices to index crystal planes
1ar
2ar
3ar
x1
x2
x3
• find the intercepts x1, x2, and x3
• h: k: l = 1/x1 : 1/ x2: 1/x3
Find the intercepts on the axes in terms of lattice constants1
ar
2ar
3ar
Take the reciprocals of these numbers and then reduce to the smallest three integers h, k, and l.
The results, enclosed in parentheses (hkl), are known as Miller indices
26
Classification of Bravais lattices and crystal structures
Symmetry operations: all rigid operations that take the lattice into itself
All symmetry operations of a Bravais lattice contains only operations of
the following form:
1. Translations TR through lattice vectors
2. operations that leave a particular point of lattice fixed (point operation)
3. successive operations of 1 and 2
The set of symmetry operation is known as space group
The set of point operation is known as point group, a subset of space group
Rigid operation: operations that preserve the distance between all lattice points.
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(a) A rotation operation through an axis that contains no lattice points
(b) An equivalent compound operation involving a translation and a point
operation
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Seven crystal systems (point groups) and fourteen Bravais lattices (space groups)
cubic
tetragonal
orthorhombic
monoclinic
triclinic
trigonal
hexagonal
There are only seven distinct point groups that a Bravais lattice can have
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Cubic system: 3 Bravais lattices
Simple cubicBody centered cubic Face centered cubic
Tetragonal system: 2 Bravais lattices
Obtained by pulling on two opposite faces of a cube
Simple tetragonalCentered tetragonal
No distinction between face centered and body centered tetragonal
One lattice plane
Next lattice
plane c/2 above
Two ways of viewing the same lattice along c axis
Viewed as if it’s “body centered” Viewed as if it’s “face centered”
30
Orthorhombic system: 4 Bravais lattice
By stretching tetragonal along one of the a axis
Two ways of stretching the same simple tetragonal lattice viewed along c axis
stretchstretch
Simple orthorhombicBase centered orthorhombic
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Two ways of stretching the same centered tetragonal lattice viewed along c axis
stretch stretch
Body-centered orthorhombicface-centered orthorhombic
Symmetry reduced, two structures distinguishable
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not a right angle
Monoclinic system: 2 Bravais lattices
Base centered orthorhombic
Reduce orthorhombic symmetry by Distorting the rectangular faces perpendicular to c axis
Simple orthorhombic
Simple monoclinic
Distort rectangular shape into parallelogram
33
Distort rectangular shape into parallelogram
Body-centered orthorhombicface-centered orthorhombic
Centered monoclinic
No distinction between “face-centered” and “body-centered”
34
Triclinic system: 1 Bravais lattice
Tilt the c axis of a monoclinic lattice
• no restrictions except that pairs of opposite faces are parallel
• a Bravais lattice generated by three primitive vectors without special relationship to one another
• the Bravais lattice with the minimum symmetry
Think: why there are no face-centered or body-centered triclinic?
Trigonal system: 1 Bravais lattice
Stretch a cube along a body diagonal
Hexagonal system: 1 Bravais latticecubic
tetragonal
orthorhombic
monoclinic
triclinic
hexagonal
trigonal
Arrow: direction of symmetry reduction