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An Introduction to Neutron Scattering - Spallation Neutron Source

An Introduction to Neutron Scattering - Spallation Neutron Source

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<strong>Neutron</strong> Polarization at the Echo Point is a<br />

Measure of the Intermediate <strong>Scattering</strong> Function<br />

r<br />

∫∫ I(<br />

λ)<br />

S(<br />

Q,<br />

ω)<br />

cos( φ1<br />

−φ<br />

2 ) dλdω<br />

r<br />

r<br />

P = r<br />

≈ ∫ S(<br />

Q,<br />

ω)<br />

cos( ωτ ) dω<br />

= I( Q,τ)<br />

∫∫ I(<br />

λ)<br />

S(<br />

Q,<br />

ω)<br />

dλdω<br />

Bd λ τ<br />

2<br />

m 3<br />

where the " spin echo time" τ = γBd<br />

λ<br />

(T.m)<br />

(nm) (ns)<br />

2<br />

2πh<br />

1 0.4 12<br />

• I(Q,t) is called the intermediate scattering function<br />

– Time Fourier transform of S(Q,ω) or the Q Fourier transform of G(r,t), the two<br />

particle correlation function<br />

• NSE probes the sample dynamics as a function of time rather than<br />

as a function of ω<br />

• The spin echo time, τ, is the “correlation time”<br />

1<br />

1<br />

0.6<br />

1.0<br />

40<br />

186

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