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An Introduction to Neutron Scattering - Spallation Neutron Source

An Introduction to Neutron Scattering - Spallation Neutron Source

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Coherent and Incoherent <strong>Scattering</strong><br />

The scattering length, b i , depends on the nuclear iso<strong>to</strong>pe, spin relative <strong>to</strong> the<br />

neutron & nuclear eigenstate. For a single nucleus:<br />

b<br />

i<br />

b b<br />

i<br />

=<br />

but<br />

j<br />

δb<br />

2<br />

i<br />

=<br />

dσ<br />

∴<br />

dΩ<br />

b<br />

δb<br />

=<br />

=<br />

+ δb<br />

b<br />

2<br />

=<br />

b<br />

i<br />

b<br />

0<br />

i<br />

+<br />

−<br />

2<br />

b<br />

where δb<br />

averages <strong>to</strong> zero<br />

and<br />

b<br />

∑<br />

i,<br />

j<br />

( δb<br />

e<br />

2<br />

i<br />

+ δb<br />

δb<br />

δb<br />

=<br />

i<br />

b<br />

2<br />

r r r<br />

−iQ.(<br />

R −R<br />

Coherent <strong>Scattering</strong><br />

(scattering depends on the<br />

direction of Q)<br />

i<br />

j<br />

j<br />

j<br />

)<br />

) + δbδb<br />

vanishes<br />

−<br />

+ (<br />

b<br />

b<br />

2<br />

i<br />

2<br />

j<br />

−<br />

unless<br />

b<br />

2<br />

) N<br />

Note: N = number of a<strong>to</strong>ms in scattering system<br />

i<br />

=<br />

Incoherent <strong>Scattering</strong><br />

(scattering is uniform in all directions)<br />

j

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