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Taking advantage of these technical improvements, photovoltaic cells are added behind slats for a stand-alone function and a possible connection to the grid (Figure 1).
On the reference grid (Figure 5a), the targets cannot be resolved at any range.
The information-based grid (Figure 3) leads to higher coherence for close ranges because of the smaller cells (Figure 4b).
Using electron diffraction spectroscopy we obtained electron diffraction patterns of cadmium sulfide nanocrystals deposited on carbon coated copper grid (Figure 6).
Ramified objects are expected to have frequent crossings with the grid (Figure 6B, top panel), while round-shaped ones have few crossings (Figure 6B, bottom panel).
The reference grid (Figure 3) causes the coherence to be low and its maximum is constant for all ranges (Figure 4a).
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After having run our simulation, we will obtain 60 × 60 × 125 values of the thermal conductivity distributed on a Cartesian grid (Figures 4 and 5).
The disadvantages of the B/ZM-grid (Figure 4b) and C-grid (Figure 4c) arrangements, which were pointed out by Ničkovic et al. ([2002]), on the hexagonal grid were partially solved by Ringler and Randall ([2002]) and Thuburn et al. ([2009]), respectively.
The methodology to assess the C sequestration potential in carbon plantations, as presented here, is a rule-based approach that is implemented on a geographical explicit -0.5° longitude × 0.5° latitude-grid (Figure 4).
SSP on both irregular grids (Figure 5b,c) enables resolving the two targets at closer ranges but on the coherence-adjusted grid with less cells.
Labeling did not impede oligomer formation on the EM grids (Figure S2).
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