TY - JOUR
T1 - Cu
T2 - NiO as a hole-selective back contact to improve the photoelectrochemical performance of CuBi2O4 thin film photocathodes
AU - Song, Angang
AU - Plate, Paul
AU - Chemseddine, Abdelkrim
AU - Wang, Fuxian
AU - Abdi, Fatwa F.
AU - Wollgarten, Markus
AU - Van De Krol, Roel
AU - Berglund, Sean P.
N1 - Publication details (e.g. title, author(s), publication statuses and dates) are captured on an “AS IS” and “AS AVAILABLE” basis at the time of record harvesting from the data source. Suggestions for further amendments or supplementary information can be sent to [email protected].
PY - 2019/4
Y1 - 2019/4
N2 - P-type CuBi2O4 has recently been reported as a promising photocathode material for photoelectrochemical water reduction due to its optimal optical band gap and positive photocurrent onset potential. However, despite these favourable attributes, CuBi2O4 photocathodes have shown limitations in charge carrier transport within CuBi2O4 and across the interface with n-type fluorine doped tin oxide (FTO). To overcome the later limitation, a very thin and transparent p-type Cu doped NiO (Cu:NiO) back contact layer is inserted between the FTO substrate and CuBi2O4. The Cu:NiO layer is prepared by electron beam evaporation of Ni and Cu followed by post annealing in air. CuBi2O4 photocathodes with a 7 nm thick Cu:NiO back contact layer produce photocurrent densities up to 2.83 mA cm-2 at 0.6 V versus RHE under back illumination with H2O2 as an electron scavenger, which is 25% higher than photocathodes without the back contact layer. This is also the highest reported photocurrent density for CuBi2O4 to date. The observed improvement in photocurrent density with the Cu:NiO back contact layer is attributed to hole selective transport across the CuBi2O4-Cu:NiO interface with a decrease in barrier height compared to the CuBi2O4-FTO interface. © 2019 The Royal Society of Chemistry.
AB - P-type CuBi2O4 has recently been reported as a promising photocathode material for photoelectrochemical water reduction due to its optimal optical band gap and positive photocurrent onset potential. However, despite these favourable attributes, CuBi2O4 photocathodes have shown limitations in charge carrier transport within CuBi2O4 and across the interface with n-type fluorine doped tin oxide (FTO). To overcome the later limitation, a very thin and transparent p-type Cu doped NiO (Cu:NiO) back contact layer is inserted between the FTO substrate and CuBi2O4. The Cu:NiO layer is prepared by electron beam evaporation of Ni and Cu followed by post annealing in air. CuBi2O4 photocathodes with a 7 nm thick Cu:NiO back contact layer produce photocurrent densities up to 2.83 mA cm-2 at 0.6 V versus RHE under back illumination with H2O2 as an electron scavenger, which is 25% higher than photocathodes without the back contact layer. This is also the highest reported photocurrent density for CuBi2O4 to date. The observed improvement in photocurrent density with the Cu:NiO back contact layer is attributed to hole selective transport across the CuBi2O4-Cu:NiO interface with a decrease in barrier height compared to the CuBi2O4-FTO interface. © 2019 The Royal Society of Chemistry.
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U2 - 10.1039/c9ta01489f
DO - 10.1039/c9ta01489f
M3 - RGC 21 - Publication in refereed journal
SN - 2050-7488
VL - 7
SP - 9183
EP - 9194
JO - Journal of Materials Chemistry A
JF - Journal of Materials Chemistry A
IS - 15
ER -