lecture 6
Transcript of lecture 6
Miller Indices of directions and planes
William Hallowes Miller(1801 – 1880)
University of Cambridge
1. Choose a point on the direction as the origin.2. Choose a coordinate system with axes parallel to the unit cell edges.
x
y3. Find the coordinates of another point on the direction in terms of a, b and c
4. Reduce the coordinates to smallest integers.
5. Put in square brackets
Miller Indices of Directions
[100]
1a+0b+0c
z
1, 0, 0
1, 0, 0
Note that we use separator only when one of them in double digits
x
y
z
O
A 1/2, 1/2, 1
[1 1 2]
OA=1/2 a + 1/2 b + 1 c
P
Q
x
y
z
PQ = -1 a -1 b + 1 c
-1, -1, 1
Miller Indices of Directions (contd.)
[ 1 1 1 ]__
-ve steps are shown as bar over the number
Family of Directions
Direction which looks physically identical but not parallelto some other direction comes under family of directions
A set of directions related by symmetry operationsof the lattice or the crystal is called a family of directions
For instance properties measured along these directions would be same owing to the symmetry of the crystal
Take an example of Cubic-F, face diagonals
All the equivalent directions can be represented by <u v w>
Miller indices of a family of symmetry related directions
[100]
[001]
[010]
uvw = [uvw] and all other directions related to [uvw] by the symmetry of the crystal
cubic100 = [100], [010], [001]
tetragonal100 = [100], [010]
Cubic Tetragonal
[010]
[100]
Family of directions
IndexNumber in the family for cubic
lattice
<100> → 3 x 2 = 6
<110> → 6 x 2 = 12
<111> → 4 x 2 = 8
These directions are very important for cubic latticewhen we will talk about properties
Negatives (opposite directions)
5. Enclose in parenthesis
Miller Indices for planes
3. Take reciprocal
2. Find intercepts along axes in
terms of respective lattice
parameters
1. Select a crystallographic
coordinate system with origin not
on the plane
4. Convert to smallest integers in
the same ratio
1 1 1
1 1 1
1 1 1
(111)
x
y
z
O
Octahedral plane
Again note that there is no separator
Miller Indices for planes (contd.)
origin
intercepts
reciprocals
Miller Indices
AB
CD
O
ABCD
O
1 ∞ ∞
1 0 0
(1 0 0)
OCBE
O*
1 -1 ∞
1 -1 0
(1 1 0)_
Plane
x
z
y
O*
x
z
E
Zero represents
that the plane is parallel to
the corresponding
axis
Bar represents a negative intercept
Crystallographically equivalent planes:Family of planes
All members physically identical butnot parallel to one and other.
Planes related with symmetry operation
Miller indices of a family of symmetry related planes
= (hkl ) and all other planes related to (hkl ) by the symmetry of the crystal
{hkl }
All the faces of the cube are equivalent to each other by symmetry
Front & back faces: (100)
Left and right faces: (010)
Top and bottom faces: (001)
{100} = (100), (010), (001)
{100}cubic = (100), (010), (001)
{100}tetragonal = (100), (010)
(001)
Cubic
Tetragonal
Miller indices of a family of symmetry related planes
x
z
y
z
x
y
CUBIC CRYSTALS
[hkl] (hkl)
Angle between two directions [h1k1l1] and [h2k2l2]:
C
[111]
(111)
22
22
22
21
21
21
212121coslkhlkh
llkkhh
Weiss zone law
True for ALL crystal systems
Not in the textbook
• If a direction [uvw] lies in a plane (hkl) then
• uh+vk+wl = 0
(hkl)
dhklInterplanar spacing between ‘successive’ (hkl) planes passing through the corners of the unit cell
222 lkh
acubichkld
O
x(100)
ad 100
B
O
x
z
E
2011
ad
INTERPLANAR SPACING
[uvw] Miller indices of a direction (i.e. a set of parallel directions)
(hkl) Miller Indices of a plane (i.e. a set of parallel planes)
<uvw> Miller indices of a family of symmetry related directions
{hkl} Miller indices of a family of symmetry related planes
No separators are allowed in MI of directions and planes
Unless the magnitude is in double digit
Summary of Notation convention for Indices
How do we determine the structure of a piece of crystalline solid?
We often say something is Cubic-F….
You can probe the atomic arrangements by X-ray diffraction (XRD)
How Characteristic X-rays are generated??
25
Characteristic X-rays are produced by electron transitionsbetween the electron shells.