We obtain a maximum photocurrent of 7.29 matcm2 athehe optimum CdS deposition of 39.33 ms%.
The maximum photocurrent density of 500 µatcm2 (at 0.5 V vs. SCE) was obtained for α-Fe2O30.5 α-Fe2O30.5electrode.
We also show that the photocurrent strongly depends on the position of the laser spot with maximum photocurrent occurring at the metal film interface.
The photocurrent contrast at hotspots is found to be due to local variations in the maximum photocurrent response in the absence of recombination process.
The maximum photocurrent density and incident photon conversion efficiencies (IPCE) were obtained for 16 at.% Cr-doped films.
In this paper, we simulate front surface inverted pyramidal grating texture on 2 400-μm 2 400-μmlicon and opthicke it to derive maximum photocurrent densiliconom the cell.
Thus, multi-parameter optimizations employing exact numerical models, as performed in this work, are essential to determine the maximum photocurrent enhancement that can be produced in solar cells.
A maximum photocurrent density of composite photoanode is achieved with a deposition time of 3 min, which is higher than that of pristine WO3 photoanode around 40%.
A maximum photocurrent density of 2 mA cm−2 is achieved for the ZnIn2S4 nanowiret/TiO2 nanowire composite film for a 6 h reaction time under white illumination.
CoTiOx and NiOx water oxidation cocatalysts were deposited onto the Si-Ta3N5 to yield active photoanodes that with NiOx retained 50-60% of their maximum photocurrent after 24 h chronoamperometry experiments and are thus among the most stable Ta3N5 photoanodes reported to date.
