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How to define a crystallographic direction with Miller indices
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Find two points lying on the given crystallographic
direction.
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Determine the coordinates of the two points
using a right hand coordinate system which is defined by crystallographic
axes a, b and c.
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Subtract the coordinates of the "tail"
point form the coordinates of the "head" point to
obtain the number of lattice parameters traveled in the direction
of each axis of the coordinate system.
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Clear fraction and/or reduce the results
obtained from the subtraction to lowest integers
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Enclose the number in square bracket [uvw].
If a negative sign is produced, represent the negative sign
with a bar over the number
Example: Find the Miller indices of direction
d shown in the figure
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Fine two arbitrary points on direction d:
P1 and P2
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The coordinates of the two points are: P1
(1/2, 1, 0) and P2 (0, 0, 1)
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Subtraction: P2 (0, 0, 1) - P1 (1/2, 1, 0)
= (-1/2, -1, 1)
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Fractions to clear: 2(-1/2, -1, 1) = (-1,
-2, 2)
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Result: [-1-22]
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| How to
define a crystallographic plane with Miller indices? |
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Find the intercepts between the crystallographic
plane and the three crystallographic axes in terms of number
of lattice constants. If the plane passes through the origin,
the origin of coordinate system should be moved.
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Take reciprocals of these intercepts.
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Clear the fractions
- Enclose the resulting numbers in parentheses (hkl). The negative
number should be written with a bar over the number.
Example: Determine the Miller indices for the
indicated plane
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Lattice constants (axial lengths): 4A,
8A, 3A
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Lengths of the intercepts: 1A, 4A, 3A
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Intercepts in terms of number of lattice
constants: ¼, ½, 1
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Clear the fractions: 4, 2, 1
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| Four indices
representation |
In hexagonal system, a crystallographic plane
is usually expressed in form of four basic vectors a1,
a2, a3 and c and
is written as (hkil). The index i is the reciprocal of the fractional
intercept on the a3 axis. The value of i depends on the values of
h and k. The relation is h
+ k = -i
The advantage of (hkil) representation
is that it can give the similar indices to similar planes. For example,
the six side planes of the hexagonal prism in the following figure
are similar and symmetrically located. Their indices can be expressed
as, in (hkil) representation, (10-10), (01-10), (-1100), (-1010),
(0-110) and (1-100) which clearly demonstrate the symmetrical relationship
of the six planes. On the other hand, the (hkl) representation:
(100), (010), (-110), (-100), (0-10) and (1-10) do not immediately
suggest the symmetrical relationship.
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Directions in a hexagonal system are best expressed as [UVW] in
the form of three basic vectors a1, a2,
and c. The four indices representation [uvtw] does
not provide any advantage over [UVW]. The relation between these
two representations is as follows:
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| U = u - t |
u = (2U - V) / 3 |
| V = v - t |
v = (2V - U) / 3 |
| W = w |
t = -(u + v) = -(U + V) / 3 |
| -- |
w = W |
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For
example, [210] and [10-10] represent the same directions as illustrated
in the above figure.
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