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Coherent Backscattering from Multiple Scattering Systems - KOPS ...

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4.2 The samples<br />

sample particle size [nm] polydispersity [%] TiO 2 content [%] n eff D [m 2 /s] τ [ns]<br />

a-1 1.38 25 1.05<br />

a-2 1.46 13 1.31<br />

NIX-2 1.38 27 0.43<br />

NIX-3 1.31 41 0.67<br />

R700 (DuPont) 245 22 1.58(6) 15(1) 2.0(1)<br />

R700 + gypsum ≈ 17 1.29 250 0.1<br />

R900 (DuPont) 359 29 1.44 17 1.05<br />

R902 (DuPont) 279 38 1.63 15 0.88<br />

S-25 1.35 21 0.65<br />

Ti-pure (Aldrich) 540 37 1.38 19(1) 6.2(3)<br />

Table 4.1: Colloidal samples. Particle size and polydispersity of the particles were<br />

determined <strong>from</strong> electron microscope images [47]. The effective refractive indices n eff<br />

were calculated using eqn. 4.1, diffusion coefficient D and absorption time τ were measured<br />

in time of flight experiments at laser wavelength λ = 590 nm. Note that the data<br />

are of strongly varied quality. Errors are given only when it was possible to quantify<br />

them.<br />

4.2.1 Titanium dioxide<br />

Titanium dioxide (TiO 2 ), or titania, is widely used as white pigment for paint, plastics or<br />

papers, in cosmetics, medicines and food, and in many other applications. The reason are its<br />

extreme ‘whiteness’ and opacity, which are due to its high refractive index (n = 2.7 in rutile<br />

phase) and its low absorption. In this work we use it to examine the structure of the coherent<br />

backscattering cone. This requires samples with kl ∗ close to unity, as in this regime the cones<br />

become very wide and their features are easier to observe in the experiment.<br />

We use both custom-made TiO 2 particles that were produced in cooperation with the chemistry<br />

department of the University of Konstanz and commercially available titania powders<br />

which were kindly provided for free by Sigma-Aldrich and DuPont. These contain more or<br />

less spherical particles of rutile titania with diameters between 200 and 600 nm (tab. 4.1). As<br />

conglomerates are rare, the powders can quite easily be compressed to volume fractions of the<br />

order of 40%.<br />

The pure titania samples have diffusion coefficients in the low two-digit range. As we also<br />

intended to do measurements on samples with higher diffusion coefficients, we mixed titania<br />

and ground blackboard chalk (gypsum) in a weight ratio of 1 to 5.<br />

4.2.2 Teflon<br />

Polytetrafluoroethylene (PTFE), best known under its DuPont brand name Teflon, is our reference<br />

sample for backscattering experiments. It is a solid (thus avoiding the problem of<br />

re-creating the sample with exactly the same properties for later measurements, which one<br />

would have with a colloidal reference), but without any particular order (crystalline or otherwise),<br />

has low absorption (though not as low as the TiO 2 samples), and a very large transport<br />

mean free path and therefore an extremely narrow backscattering cone.<br />

39

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