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For the turbid medium, we assumed the Rayleigh scattering function and ω = 0.1, and we considered the same geometry as the experiment.
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To model the carrier transport properties of the effective medium, we assume that the optical generated carriers in GaAs barriers are captured by the lower bandgap 2D WL and, subsequently, relax to the QD ground state on time scales of 1 50 ps [28, 29].
Since the lipid bodies are suspended in an aqueous medium, we assume that the lipid is saturated with water and used water-saturated octanol, referred to herein as wet octanol, as a model.
Since our culture was rescued by transfer to richly supplemented U-medium, we assume one of the supplements as a necessary factor.
As a baseline for the medium prevalence setting, we assumed a steady-state prevalence of 5% over the time frame, although without interventions the prevalence would continue to rise to the high prevalence level.
In this paper we consider 2.5D problems in which 3D delta-type sources are used to illuminate the medium but we assume the chromophore concentrations vary only in two dimensions, x and y, and are constant in the third, z.
Prioritizing the bandwidth of cluster members with high, medium, or low, we assume that there are only one node with high priority, two with medium priority, and the rest with low priority in one cluster, of which bandwidth are defined as B high, B medium, and B low, respectively.
The setting of the computation of Fig. 3 is very simple: we assumed a homogeneous infinite medium.
Here we assumed a weakly scattering medium initially and, therefore, the first approximation to the transport coefficient was estimated without solving the Helmholz equation.
We assume a medium voltage (MV) radial distribution network with high RES penetration level.
Thus we assume a medium degree of complexity compared to other settings [ 49- 52].
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