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Coherent Backscattering from Multiple Scattering Systems - KOPS ...

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5 Experiments<br />

1<br />

0.8<br />

α c<br />

(A)<br />

α c<br />

(A) + αc<br />

(B+C)<br />

R700 with ℵ=1<br />

R700 with ℵ=0.92<br />

cooperon<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 10 20 30 40 50 60 70 80 90<br />

scattering angle [deg]<br />

1<br />

0.8<br />

α c<br />

(A)<br />

α c<br />

(A) + αc<br />

(B+C)<br />

NIX−2 with ℵ=1<br />

NIX−2 with ℵ=0.93<br />

cooperon<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 10 20 30 40 50 60 70 80 90<br />

scattering angle [deg]<br />

Figure 5.7: Example wide angle backscattering data. Top: R700, bottom: NIX-2. If the<br />

different albedos of sample and reference are neglected (red), the data clearly violate<br />

conservation of energy and do not fit with any theory. The correctly evaluated data<br />

(orange) deviate significantly <strong>from</strong> α (A)<br />

c , but fit very well with α c = α (A)<br />

c + α (B+C)<br />

c within<br />

the region of confidence (which is only marginally larger than the data points and is<br />

therefore not drawn explicitly). For R700 one obtains kl ∗ = 2.7(3) and l ∗ = 250(30) nm,<br />

and kl ∗ = 6.4(3) and l ∗ = 600(30) nm for NIX-2. The integration over the cooperon<br />

yields E = −0.024(5) sterad for R700 and E = −0.013(7) sterad for NIX-2 if the error of<br />

the albedo is set to zero. E is zero within the margins of error if the error of the albedo<br />

is 1%.<br />

54

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