PHYS01200804001 Sohrab Abbas - Homi Bhabha National Institute
PHYS01200804001 Sohrab Abbas - Homi Bhabha National Institute
PHYS01200804001 Sohrab Abbas - Homi Bhabha National Institute
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Due to the rapid strides made lately by the semiconductor electronics industry, most relevant<br />
properties of single crystal silicon have been determined to great precision over a wide temperature<br />
range. Single crystal silicon is therefore an ideal candidate for high precision b c determination (cf.<br />
Chapter 5). For Si, attn /(2 b c ) ~ 10 -5 for 2Å neutrons, implying negligible neutron absorption and<br />
incoherent scattering. Some important neutron scattering properties of silicon cited in literature<br />
[119] are summarised in the Table 1.<br />
2.2 Dynamical diffraction from a single crystal<br />
The dynamical theory [1,4,54-70] regards the incident and diffracted waves inside the crystal to be<br />
coherently coupled forming a composite wave function<br />
<br />
( r ) e e ,<br />
(9)<br />
i KO<br />
. r ' i KH<br />
. r<br />
O<br />
H<br />
H<br />
which behaves as a single entity. The sum extends over all reciprocal lattice vectors. The internal<br />
wave vectors K O and K H are related through the Bragg condition<br />
K H = K O + H. (10)<br />
The interactions between the waves and the crystal are represented by the potential<br />
<br />
<br />
V( r) V e V V e<br />
i H. r<br />
i H.<br />
r<br />
H O H<br />
H H≠0<br />
(11)<br />
with<br />
V<br />
H<br />
2 2 2<br />
2<br />
Nbc FH<br />
k0<br />
<br />
m F 2m<br />
O<br />
H<br />
. (12)<br />
Here m stands for the neutron mass, F O and F H , the structure factors for O and H reflections<br />
respectively, N, the atomic number density, H , the susceptibility for the H reflection and b c , the<br />
coherent scattering length.<br />
16