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To see how the transition energy shifts with the excitation, we calculated the energy shifts of the electron and heavy hole as a function of the sheet charge density Figure 2b.
Binding energy of 3.7 meV is obtained for the exciton by comparing with the energies of the single-particle calculation Equation 1. Figure 3b shows the exciton energy shift in the GaAsSb/GaAs QW as a function of the sheet charge density.
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(d) Approximate color scale for mica sheets as a function of the thickness with thickness in the 10- to 50-nm range.
The microstructural evolution of the sheets was investigated as a function of the processing time and the mass of the ball.
The data in Figure 7 (I) show the sheet resistance and carrier concentration as a function of the rGO loading in the rGO-PEDOT PTS hybrGO-PEDOT PTS
Further structural analysis is shown in Fig. 8, where we plot the number of amino acids associated with alpha-helical and beta-sheet secondary structures as a function of the applied tensile strain in a geometry-strain map.
Figure 3 shows the sheet resistance values of the IAAM and AAM films as a function of the AAM film thickness and Ag content.
It is shown that the sheet resistance and transmittance are inversely proportional to each other as a function of the process parameters.
The sheet conductance of a-LAO/STO and c-LAO/STO heterostructures were measured as a function of the thickness of LAO overlayer at room temperature.
Fig. 2 Electrical resistivity and sheet resistance of the BAB multilayer thin films as a function of the annealing temperature.
Figure 2 shows the variation in electrical resistivity and sheet resistance of the BAB multilayer thin films as a function of the annealing temperature.
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