TY - JOUR
T1 - Polycrystalline Cu2O photovoltaic devices incorporating Zn(O,S) window layers
AU - Tolstova, Yulia
AU - Omelchenko, Stefan T.
AU - Blackwell, Raymond E.
AU - Shing, Amanda M.
AU - Atwater, Harry A.
N1 - Publisher Copyright: © 2016 Elsevier B.V.
PY - 2017/2/1
Y1 - 2017/2/1
N2 - The tunability of the Zn(O,S) conduction band edge makes it an ideal, earth-abundant heterojunction partner for Cu2O, whose low electron affinity has limited photovoltaic performance with most other heterojunction candidates. However, to date Cu2O/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 Cu2O/Zn(O,S) solar cells fabricated by sputter deposition of Zn(O,S) on polycrystalline Cu2O 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 ZnSO4 at the Zn(O,S)/Cu2O interface that impedes current collection and limits the short circuit current density to 2 mA/cm2. Deposition of Zn(O,S) at elevated temperatures decreases the presence of interfacial ZnSO4 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/cm2, although a small ZnSO4 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.
AB - The tunability of the Zn(O,S) conduction band edge makes it an ideal, earth-abundant heterojunction partner for Cu2O, whose low electron affinity has limited photovoltaic performance with most other heterojunction candidates. However, to date Cu2O/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 Cu2O/Zn(O,S) solar cells fabricated by sputter deposition of Zn(O,S) on polycrystalline Cu2O 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 ZnSO4 at the Zn(O,S)/Cu2O interface that impedes current collection and limits the short circuit current density to 2 mA/cm2. Deposition of Zn(O,S) at elevated temperatures decreases the presence of interfacial ZnSO4 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/cm2, although a small ZnSO4 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.
KW - Cuprous oxide
KW - Earth-abundant semiconductors
KW - Heterojunction solar cell
KW - Photovoltaics
KW - Sputtering
UR - https://www.scopus.com/pages/publications/84994700898
U2 - 10.1016/j.solmat.2016.10.049
DO - 10.1016/j.solmat.2016.10.049
M3 - Article
SN - 0927-0248
VL - 160
SP - 340
EP - 345
JO - Solar Energy Materials and Solar Cells
JF - Solar Energy Materials and Solar Cells
ER -