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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

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