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Published February 7, 1991 | public
Journal Article

Trends in the open circuit voltage of semiconductor/liquid interfaces: studies of n-AlₓGa₁₋ₓAs/CH₃CN-Ferrocene^(+/0) and n-AlₓGa₁₋ₓAs/KOH-Se^(~/2~)(aq) Junctions

Abstract

Trends in open-circuit voltage (V_(oc)), short-circuit current density (J_(sc)), and energy conversion efficiency have been determined for the n-type AlₓGa₁₋ₓAs series of photoelectrodes (x = 0.0, 0.09, 0.16, 0.24, 0.31) in contact with CH₃CN-Ferrocene^(+/0) and KOH-Se^(~/2~)(aq) electrolytes. V_(oc) increased linearly with increases in bandgap energy (E_g) of the n-AlₓGa₁₋ₓAs alloy electrodes, with ΔV_(oc)/ΔE_g = 0.45 ± 0.04 V eV⁻¹ in CH₃CN and 0.41 ± 0.09 V eV⁻¹ in KOH-Se^(~/2~)(aq) at a light intensity sufficient to provide J_(sc) = 1.0 mA cm². J_(sc) values under solar-simulated illumination decreased monotonically with increasing bandgap energy. The relatively low value of ΔV_(oc)/ΔE_g implies decreases in optimal energy conversion efficiency as the mole fraction of A1 in the AlₓGa₁₋ₓAs alloy is increased. This is in contrast to the behavior of the GaAsₓP₁₋ₓ alloy series in the same electrolytes. The lower value of ΔV_(oc)/ΔE_g for n-AlₓGa₁₋ₓAs also indicates that predictions of the "common anion rule" in solid-state barriers do not apply to this family of III—V semiconductor/liquid junctions.

Additional Information

© 1991 American Chemical Society. We thank the Department of Energy, Office of Basic Energy Sciences, for support of this work. We are indebted to Dr. C. R. Lewis of Varian Associates for generously providing the n-AlₓGa₁₋ₓAs alloy samples utilized in this study. We also thank Dr. B. Anspaugh of the Jet Propulsion Laboratory for performing some of the spectral irradiance measurements. N.S.L. acknowledges support as a Dreyfus Teacher-Scholar (1985-1990).

Additional details

Created:
August 22, 2023
Modified:
October 18, 2023