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An Introduction to Neutron Scattering - Spallation Neutron Source

An Introduction to Neutron Scattering - Spallation Neutron Source

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Inelastic neutron scattering measures a<strong>to</strong>mic motions<br />

The concept of a pair correlation function can be generalized:<br />

G(r,t) = probability of finding a nucleus at (r,t) given that there is one at r=0 at t=0<br />

G s (r,t) = probability of finding a nucleus at (r,t) if the same nucleus was at r=0 at t=0<br />

Then one finds:<br />

2 ⎛ d σ ⎞<br />

⎜<br />

d dE ⎟<br />

⎝ Ω.<br />

⎠<br />

2 ⎛ d σ ⎞<br />

⎜<br />

d dE<br />

⎟<br />

⎝ Ω.<br />

⎠<br />

coh<br />

inc<br />

= b<br />

= b<br />

where<br />

r 1<br />

S(<br />

Q,<br />

ω)<br />

=<br />

2πh<br />

2<br />

coh<br />

2<br />

inc<br />

∫∫<br />

k'<br />

r<br />

NS(<br />

Q,<br />

ω)<br />

k<br />

k'<br />

r<br />

NSi<br />

( Q,<br />

ω)<br />

k<br />

r<br />

G(<br />

r,<br />

t)<br />

e<br />

r r<br />

i(<br />

Q.<br />

r −ωt)<br />

r<br />

drdt<br />

and<br />

(h/2π)Q & (h/2π)ω are the momentum &<br />

energy transferred <strong>to</strong> the neutron during the<br />

scattering process<br />

r 1<br />

Si<br />

( Q,<br />

ω)<br />

=<br />

2πh<br />

∫∫<br />

G<br />

s<br />

r<br />

( r,<br />

t)<br />

e<br />

r r<br />

i(<br />

Q.<br />

r −ωt<br />

)<br />

r<br />

drdt<br />

Inelastic coherent scattering measures correlated motions of a<strong>to</strong>ms<br />

Inelastic incoherent scattering measures self-correlations e.g. diffusion

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