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The sheet resistance, R s, as a function of transmittance at 550 nm is summarized in Figure 7.
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Figure 7 Sheet resistance of different films as a function of optical transmittance at 550 nm.
Performance characteristics have been investigated as a function of output mirror transmittance.
Finally, we determined the apparent densities of the samples by weighing cylindrical samples of known dimensions. Figure 1 presents transmittance as a function of wavelength for samples prepared at pH values ranging from 1 to 10. Open image in new window Fig. 1 Transmittance spectra (percent transmitted) of aerogel samples at a low and b high pH values.
The optical transmittance and reflection spectra were measured as a function of incident photon wavelength at wavelengths between 200 and 800 nm from films deposited on the fused silica substrates using a Shimadzu UV-3101 spectrophotometer.
The optical properties of the films have been studied by optical spectrophotometry in the UV-Vis-NIR range, and the obtained results are shown in Figure 2. On the left is shown the optical transmittance as a function of wavelength, and on the right is shown the optical transmittance at λ = 2500 nm as a function of temperature.
The variation of transmittance T as a function of wavelength for samples 1 4 were recorded at room temperature and are shown in Fig. 5.
Figure 2 Optical transmittance spectra of VO 2 films: (a1-a3) optical transmittance as a function of wavelength, in semiconducting and metallic states; (b1-b3) optical transmittance as a function of temperature obtained at λ = 2500 nm.
The curve of light transmittance as a function of temperature can be obtained after testing the light transmittances of the polymer solution at different temperatures.
Absorption spectra at different potentials and change of transmittance at different wavelengths as a function of potential are furnished.
When the hydrogen flow rate was 30 sccm, the transmittance as a function of wavelength for single-layer graphene reached its maximum of 97.7% at λ =550 nm.
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