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Updated: Aug 7, 2026

Harvesting Solar Energy by Means of Charge-Separating Nanocrystals and Their Solids
Published on: August 23, 2012
Power conversion in SnS photocathodes made by electrochemical growth is limited by recombination at (002) buried
Zainab Najaf1, Mahya Salmanion1, Rajesh Kandel1
1Department of Chemistry, University of California, Davis, One Shields Avenue, Davis, CA 95616, USA. fosterloh@ucdavis.edu.
Abstract:
Herzenbergite α-SnS is a promising p-type semiconductor for photovoltaic and solar fuel applications, but current devices are plagued by substantial photovoltage losses. Here we use vibrating Kelvin probe surface photovoltage for the first time to study the recombination losses in microcrystalline SnS photoelectrodes. α-SnS films of varied crystal orientation, size, and shape are obtained by electrochemical growth from aqueous tin(II) chloride and sodium thiosulfate solutions near room temperature. After application of a CdS passivation layer, the films function as photocathodes for the methylviologen reduction reaction. Photoelectrochemical and surface photovoltage measurements reveal that the performance of these devices is sensitively controlled by mainly the SnS crystal orientation and to a lesser extent by the grain size. For example, the highest charge recombination rates of 8.97 × 1014 s-1 cm-2 and lowest photocurrent (0.73 mA cm-2) and lowest photovoltage (0.12 V) occur for SnS films containing 500 nm crystals with irregular shapes and SnS lattices tilted away from the (001) orientation. On the other hand, the best performance (1.62 mA cm-2, 0.16 V, 3.32 × 1012 s-1 cm-2) is seen for 1100 nm fully (001) oriented SnS nanoplates. These findings agree with improved charge carrier mobility in the 001 direction and they also show that charge recombination in SnS films occurs mainly at dangling Sn-S bonds at buried (002) facets. Such buried interfaces need to be suppressed for optimized solar energy conversion with SnS.
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