The Structure FactorThe Structure Factor - University of Babylon
The Structure Factor
Suggested Reading
Pages 303-312 in DeGraef & McHenry Pages 59-61 in Engler and Randle
1
Structure Factor (Fhkl)
N
F f e2i(hui kv j lwi )
hkl
i
i1
? Describes how atomic arrangement (uvw) influences the intensity of the scattered beam.
? It tells us which reflections (i.e., peaks, hkl) to expect in a diffraction pattern.
2
Structure Factor (Fhkl)
? The amplitude of the resultant wave is given by a ratio of amplitudes:
Fhkl
amplitude of amplitude
the wave scattered by of the wave scattered
all by
atoms of a UC one electron
? The intensity of the diffracted wave is proportional to |Fhkl|2.
3
Some Useful Relations
ei = e3i = e5i = ... = -1 e2i = e4i = e6i = ... = +1 eni = (-1)n, where n is any integer eni = e-ni, where n is any integer
eix + e-ix =2 cos x
Needed for structure factor calculations
4
Fhkl for Simple Cubic
? Atom coordinate(s) u,v,w:
? 0,0,0
N
F f e2i(hui kvj lwi )
hkl
i
i1
Fhkl fe2i(0h0k0l ) f
No matter what atom coordinates or plane indices you substitute into the structure factor equation for simple cubic crystals, the solution is always
non-zero.
Thus, all reflections are allowed for simple cubic (primitive) structures.
5
Fhkl for Body Centered Cubic
? Atom coordinate(s) u,v,w:
? 0,0,0; ? ?, ?, ?.
N
F f e2i(hui kvj lwi )
hkl
i
i1
Fhkl
fe2i(0)
fe2
i
h 2
k 2
l 2
Fhkl f 1 eihkl
When h+k+l is even Fhkl = non-zero reflection.
When h+k+l is odd Fhkl = 0 no reflection.
6
Fhkl for Face Centered Cubic
? Atom coordinate(s) u,v,w:
? 0,0,0; ? ?,?,0; ? ?,0,?; ? 0,?,?.
N
F f e2i(hui kvj lwi )
hkl
i
i1
Fhkl
fe2i0
fe 2
i
h 2
k 2
fe 2
i
h 2
l 2
fe2
i
k 2
l 2
Fhkl f 1 eihk eihl eikl
7
Fhkl for Face Centered Cubic
Fhkl f 1 eihk eihl eikl
? Substitute in a few values of hkl and you will find the following:
? When h,k,l are unmixed (i.e. all even or all odd), then Fhkl = 4f. [NOTE: zero is considered even]
? Fhkl = 0 for mixed indices (i.e., a combination of odd and even).
8
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