Coherent Backscattering from Multiple Scattering Systems - KOPS ...
Coherent Backscattering from Multiple Scattering Systems - KOPS ...
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 />
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