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Figure 7 Planar average of donor-electron density as a function of z -position for 1/4 ML-doped 80-layer cell.
In order to quantify the extent of the donor-electron distribution, we have integrated the local density of states between the VBM and Fermi level and have taken the planar average with respect to the z-position.
Figure7 shows the planar average of the donor electrons (a sum of both spin-up and spin-down channels) for the 80-layer cell calculated using the DZP basis set.
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Fig. 4 a Profile of the planar averaged self-consistent electrostatic potential for the ZrS2/B20 as a function of position in the z-direction.
c Profile of the planar averaged charge density difference for the ZrS2/B20 as a function of position in the z-direction.
To display the quantitative analysis, the profile of the planar averaged self-consistent electrostatic potential for the ZrS2/B20 hybrid as a function of position in the z-direction is displayed in Fig. 4a.
To offer quantitative results of charge redistribution, Fig. 4c plots the planar averaged charge density difference along the direction perpendicular to the monolayer ZrS2, where the positive value indicates the charge accumulation, and negative value represents the charge depletion.
In the crystal, the NNN molecules are always planar on average.
The average planar sizes of CuO microdisks are in range of 1.0 ~ 1.8 μm.
This material is produced from microwave expansion of acid intercalated graphite which yields a planar structure with average thickness of 1 to 10 nm and varying diameter of 15 to 50 microns [55-57] [55-57]
Compared with the planar one, the average absorption of the optimum structure with an a-Si layer of 280-nm thickness and a Ag layer of 200-nm thickness is boosted by 71.6 %, from 45.1 to 77.4 % over the whole wavelength due to the presence of the periodic configuration.
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