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Neutron Scattering

Neutron Scattering - JuSER - Forschungszentrum Jülich

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E<br />

ô<br />

ô<br />

x<br />

z<br />

w<br />

0<br />

z<br />

_w<br />

U<br />

N<br />

Figure 2 .7 : <strong>Scattering</strong> length of nuclei for thermal neutrons as a function of atomic weight .<br />

2 .6 .2 Coherent and incoherent scattering<br />

The scattering of neutrons depends on the isotope as well as on the relative spin orientations .<br />

We now will look into the consequences in regarding the elastic scattering from an ensemble<br />

of isotopes with the coordinates and scattering lengths {R, , b, } . The pseudo potential of this<br />

ensemble has the form<br />

V (L) - 2z b z Y, b, 8(r - R ) (2 .23)<br />

ni,<br />

l<br />

with Eq . [2 .l8] we may calculate the matrix element of Vbetween k and k' as<br />

~k' IVI k) = 2z b z b f e>k'r ä (r _ R, ) e>~ d3 r (2 .24)<br />

m<br />

2zb 2<br />

m<br />

b, eiQnr Q - k_ k'<br />

The matrix element is just a Fourier surr over the atomic positions decorated with the<br />

appropriate scattering length bi. The scattering cross section is obtained following Eq .[2.19] .<br />

2- 15

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