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The fit algorithm was tested using Monte Carlo simulations of single fiber reflectance intensities that investigated biologically relevant ranges of scattering properties (μ′ s ∈ [0.4 – 4]mm−1) and phase functions (γ ∈ [1.4 – 1.9]) and for multiple fiber diameters (d fiber ∈ [0.2 – 1.5] mm).
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The second set of windows separated by 50 μm is used to monitor the scattered light intensities over a wide range of scattering vector q (from 0.35 to 4 μm−1) which allows the assessment of the mechanism of phase separation.
CIPS provides panoramic ultraviolet images of the atmosphere over a wide range of scattering angles in order to determine the presence of polar mesospheric clouds, measure their spatial morphology, and constrain the parameters of cloud particle size distribution.
For some defined sets of points, the analytical expressions for diffraction intensities were found and tested numerically on a wide range of scattering vectors and for up to 232 atoms.
Whilst consistency has been observed between all three techniques, electron diffraction has been found to have advantages by allowing data to be collected over a large range of scattering angles as well as without interference from crystalline regions within the char.
DLS measures the scattered intensity over a range of scattering angles θdls for a given time t k in time steps ∆t.
On the intensity curve in a wide range of scattering angles, there is the linear section with the slope n2 = 3.3.
In case of PCM, modified at 500°С, the scattering intensity curves are characterized by the linear section in the wide range of scattering angles, the slope of which changes within the limits 3 < n2 < 4.
Strong orientation facilitated the use of a range of scattering techniques.
It is understood that reflectance devices sample photons that have experienced a range of scattering events [ 27].
The scattering intensities were collected over a very wide range of scattering angles and the data is suggestive of a hierarchy of structural architectures.
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