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GPC coupled with light scattering allowed molar masses to be determined.
Moreover, the low-frequency Raman scattering allowed to determine an average particle size diameter of 4 nm.
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Dynamic light scattering allows detecting these aggregates, giving a size distribution from 10too 100 nm in diameter.
Individual subwavelength Si nanostructures (e.g., NWs and nanoparticles) exhibit strong morphology-dependent resonant scattering, allowing their arrays to be used for controllable structural coloration [5, 18].
The cavity-induced enhancement of the Raman scattering allows the observation of Raman spectra from only a monolayer of CdTe quantum dots.
In dark-field radiography, the simultaneous image information of the attenuation and the small angle scattering allows for an improved assessment of foreign bodies.
Our B-modeling of diffuse scattering allows a closer connection between haze and both physical and physiological quantities, while yielding the same quantification of haze as the standard method.
In addition to calculating the spectrum and the efficiency for Raman active modes, it is shown that the negligible wave-vector of the phonons involved in this type of scattering allows for the use of the bandgap "pinching" effect to arrive at specific layer thicknesses for Si and Ge that optimize the scattering efficiency.
However, we found that if you can control every individual light wave with which you illuminate these lenses, it is possible to prepare for the scattering, allowing you to focus the light through opaque materials.
Thus difference between the fluorescence intensities at resonance (SPRF + scattering) and just off-resonance (scattering) allows the determination of the fraction of the fluorescence signal due to scattering (∼35%); this was subtracted from our fluorescence measurements.
However, their physical properties of forward scattering and side scattering allow safe discrimination of these two populations; and b) the lack of measurement of the precise lymphocyte count at every time of sampling.
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