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An Introduction to Neutron Scattering - Spallation Neutron Source

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SANS Measures Particle Shapes and Inter-particle Correlations<br />

dσ<br />

dΩ<br />

=<br />

=<br />

b<br />

3<br />

∫ d R ∫<br />

space space<br />

2 3<br />

∫ d r ∫<br />

space space<br />

d<br />

3<br />

R'<br />

n<br />

P<br />

d<br />

3<br />

r'<br />

n<br />

r<br />

( R)<br />

n<br />

N<br />

P<br />

r<br />

( r ) n<br />

r<br />

( R')<br />

dσ<br />

= ( ρ − ρ<br />

dΩ<br />

0<br />

)<br />

2<br />

N<br />

e<br />

v<br />

F(<br />

Q)<br />

r<br />

( r ').<br />

e<br />

r r r<br />

iQ.(<br />

R−<br />

R')<br />

r<br />

F(<br />

Q)<br />

2<br />

r r r<br />

iQ.(<br />

r −r<br />

')<br />

2<br />

where G P is the particle - particle correlation<br />

function (the probability<br />

that the re<br />

r<br />

v 2<br />

is a particle at R if there's<br />

one at the origin) and F( Q)<br />

is the particle form fac<strong>to</strong>r<br />

=<br />

∫<br />

( ρ − ρ<br />

N<br />

d<br />

particle<br />

3<br />

∫<br />

P<br />

space<br />

x.<br />

e<br />

d<br />

0<br />

3<br />

)<br />

r v<br />

iQ.<br />

x<br />

R.<br />

G<br />

2<br />

∫<br />

d<br />

particle<br />

P<br />

3<br />

x.<br />

e<br />

r v<br />

iQ.<br />

x<br />

r<br />

( R).<br />

e<br />

These expressions are the same as those for nuclear scattering except for the addition<br />

of a form fac<strong>to</strong>r that arises because the scattering is no longer from point-like particles<br />

2<br />

r r<br />

iQ.<br />

R<br />

:

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