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After cultivation at 37 °C for 24 h, all the colonies grown were enumerated, and the mean values and maximal scatter in CFUs were determined.
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The scattering curve for Cu@Chit-2 showed the maximal scattering intensity in very small angles (<2 nm−1).
Red numbers in the scattering patterns indicate the angles with maximal scattering power.
Interestingly, similar shapes to the cross-sectional geometry of these lens-like structures have been reported elsewhere by Macías et al. recently when they attempted to search for the 2-D shapes with maximal scattering geometry[22].
Each scattering curve was normalized to 1.0 by dividing the observed data by the maximal scattering.
Friebel et al. [ 3] found a maximal scattering cross-section for shrunken RBCs.
The mean inhibition-zone diameter and the maximal data scatter also were determined.
In this article, the optimal core radii and shell thicknesses of silica gold and hollow gold nanoshells, possessing maximal light scattering and absorption at wavelengths between 700 and 1100 nm, are obtained using the Mie theory of a coated sphere.
In the case of β = 2, the maximal energy absorbed (scattered) by the ensemble is achieved for the same dimensions that maximize the absorption (scattering) efficiency of a single nanoshell.
For this goal, it may be useful to analyze maximal intensities in scattering images as a function of deformation.
When β = 1 and ρ ∝ 1/ R2 [see Figs. 1(a) and 1(b)], the strongest absorption and scattering occur for the nanoshells of diameters 400 nm, i.e., at the edge of the parametric domain of interest (absorption peaks for R1 ≈ 180 nm, while scattering becomes maximal for pure gold nanoshells).
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