Polycrystalline Cu_(2)O photovoltaic devices incorporating Zn(O,S) window layers

The tunability of the Zn(O,S) conduction band edge makes it an ideal, earth-abundant heterojunction partner for Cu_(2)O, whose low electron affinity has limited photovoltaic performance with most other heterojunction candidates. However, to date Cu_(2)O/Zn(O,S) solar cells have exhibited photocurrents well below the entitled short-circuit current in the detailed balance limit. In this work, we examine the sources of photocurrent loss in Cu_(2)O/Zn(O,S) solar cells fabricated by sputter deposition of Zn(O,S) on polycrystalline Cu_(2)O substrates grown by thermal oxidation of Cu foils. X-ray photoelectron spectra reveal that Zn(O,S) deposited at room temperature leads to a thin layer of ZnSO_4 at the Zn(O,S)/Cu_(2)O interface that impedes current collection and limits the short circuit current density to 2 mA/cm^2. Deposition of Zn(O,S) at elevated temperatures decreases the presence of interfacial ZnSO_4 and therefore the barrier to photocurrent collection. Optimal photovoltaic performance is achieved at a Zn(O,S) deposition temperature of 100°C, which enables an increase in the short circuit current density to 5 mA/cm^2, although a small ZnSO_4 layer is still present. Deposition at temperatures above 100°C leads to a reduction in photovoltaic performance. Spectral response measurements indicate the presence of a barrier to photocurrent and exhibit a strong dependence on voltage and light bias, likely due to the photodoping of Zn(O,S) layer