TY - GEN
T1 - Earth-abundant iron oxysulfide (FeSxOy) for bandgap optimization
AU - Han, X.
AU - Zhou, B.
AU - Tao, Meng
PY - 2012/11/26
Y1 - 2012/11/26
N2 - Transition metal sulfides with small bandgap are attractive for solar cell applications since most transition metals are abundant and many can be deposited in solution. Pyrite FeS2, with a bandgap of 0.95 eV, is one of the most desirable for solar cell applications. The problem with FeS2 is that its bandgap is ∼0.45 eV smaller than the optimum bandgap for maximum efficiency, which should be ∼1.4 eV. In this paper, we propose the concept of metal oxysulfide as the approach to a low-cost Earth-abundant semiconductor with a direct bandgap of ∼1.4 eV for terawatt-scale solar cells. This is because the bandgap of Fe2O3 is 2.2 eV. By introducing O into FeS2, the bandgap should increase. In our experiments, we use oxidation of electrodeposited FeSx for this purpose. FeSx films were electrodeposited on FTO-coated glass. Post-deposition annealing was carried out in vacuum to make FeSx films denser and more stable in air. SEM and EDX confirm that the as-grown FeSx film is amorphous and the S/Fe ratio in the film is slightly above 1. Oxidation of the FeS x films was performed either in a tube furnace under air or electrochemically in an electrolyte. After oxidation, the bandgap in the resultant FeSxOy is ∼1.3 eV by electrochemical oxidation and ∼1.1 eV by thermal oxidation. Further optimization is expected to produce a FeSxOy with a ∼1.4 eV bandgap.
AB - Transition metal sulfides with small bandgap are attractive for solar cell applications since most transition metals are abundant and many can be deposited in solution. Pyrite FeS2, with a bandgap of 0.95 eV, is one of the most desirable for solar cell applications. The problem with FeS2 is that its bandgap is ∼0.45 eV smaller than the optimum bandgap for maximum efficiency, which should be ∼1.4 eV. In this paper, we propose the concept of metal oxysulfide as the approach to a low-cost Earth-abundant semiconductor with a direct bandgap of ∼1.4 eV for terawatt-scale solar cells. This is because the bandgap of Fe2O3 is 2.2 eV. By introducing O into FeS2, the bandgap should increase. In our experiments, we use oxidation of electrodeposited FeSx for this purpose. FeSx films were electrodeposited on FTO-coated glass. Post-deposition annealing was carried out in vacuum to make FeSx films denser and more stable in air. SEM and EDX confirm that the as-grown FeSx film is amorphous and the S/Fe ratio in the film is slightly above 1. Oxidation of the FeS x films was performed either in a tube furnace under air or electrochemically in an electrolyte. After oxidation, the bandgap in the resultant FeSxOy is ∼1.3 eV by electrochemical oxidation and ∼1.1 eV by thermal oxidation. Further optimization is expected to produce a FeSxOy with a ∼1.4 eV bandgap.
KW - bandgap
KW - iron sulfide
KW - light absorber
KW - oxysulfide
UR - http://www.scopus.com/inward/record.url?scp=84869390218&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84869390218&partnerID=8YFLogxK
U2 - 10.1109/PVSC.2012.6318109
DO - 10.1109/PVSC.2012.6318109
M3 - Conference contribution
AN - SCOPUS:84869390218
SN - 9781467300643
T3 - Conference Record of the IEEE Photovoltaic Specialists Conference
SP - 2528
EP - 2532
BT - Program - 38th IEEE Photovoltaic Specialists Conference, PVSC 2012
T2 - 38th IEEE Photovoltaic Specialists Conference, PVSC 2012
Y2 - 3 June 2012 through 8 June 2012
ER -