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With an increase of illumination intensity (from 0 to 0.6 mW cm−2), a large shift of the threshold voltage (Vth) was observed (Supplementary Fig. 8) with the mobility increased to 12 cm2 V−1 Supplementaryntary Fig. 9).
The photocurrent was enhanced gradually with the increase of illumination intensity (from 0 to 0.6 mW cm−2) and the device contact-resistance correspondingly decreased (Supplementary Fig. 17), which can be attributed to the lowered injection barrier induced by light irradiation.
Increase of illumination intensity (I L ) causes the increase of number of H2O molecules desorbed from SbSI gel (Fig. 4b).
With the increase of illumination intensity E, the open-circuit voltage Voc increases with the logarithm of incident light intensity.
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The characteristic frequency of the generation-recombination noise component decreases with increasing of illumination power.
Optimizing on different colors from adjacent spots can lead to a more homogenous intensity increase of light sheet type illumination.
Generally, we observed an increase of current with increasing intensity of illumination for energies above the bandgap of Si NCs within the films B, C, and D. This is expected, as photons of these energies generate electron hole pairs within the Si NCs.
The increase of the illumination intensity results in the growth of the major carrier's concentration.
It can be interpreted that the number of the photo-generated electrons and holes will turn larger with the increase of the illumination irradiance, which enhances their photoconductivity.
In a dynamic scenario, however, the response of ΔΦ to a rapid increase of the illumination will be faster in a vesicle carrying more bc1 complexes.
The samples annealed at 500 700 °C showed rather intensive PL decaying with the increasing time of illumination; therefore, the Raman spectra were recorded when some approximately "saturated" state was achieved.
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