TY - JOUR
T1 - Chemistry and Charge Trapping at the Interface of Silver and Ultrathin Layers of Zinc Oxide
AU - Rahamim, M
AU - Cohen, H
AU - Edri, E
N1 - Funding Information: The authors are thankful to the Israeli Ministry of Energy and Water for support through grant no. 28-11-031, and the Ben-Gurion University of the Negev (start-up grant). The authors are also grateful to Dr. Muhammad Bashouti (Alexandre Yersin Department of Solar Energy and Environmental Physics and Jacob Blaustein Institutes for Desert Research, BGU) for providing access to Surface Photovoltage (SPV) and CPD measurement facilities, and to Dr. Natalya Froumin, Dr. Mariela Pavan, Dr. Upcher Alexander, and Dr. Nitzan Maman from the Ilse Katz Institute for Nanoscale Science and Technology at Ben-Gurion University for XPS and Raman measurements, FIB-TEM sample preparation, and imaging. The authors thank Dr. Roksana Vidruk (Blechner Center for Industrial Catalysis, and the Department of Chemical Engineering, BGU) for her review and comments on the manuscript. Publisher Copyright: © 2021 American Chemical Society.
PY - 2021/10/20
Y1 - 2021/10/20
N2 - Zinc oxide, a wide-band-gap semiconductor, shows intriguing optoelectronic properties when coupled with Ag. Specifically, an absorbance band in the visible range that is not apparent in the separated materials emerges when the interface is formed. Interestingly, photoexcitation of this "interface band"or band-to-band results in a counterintuitive photovoltaic response when a supra/sub-band-gap light is shone. To investigate the origin of this absorbance band and photovoltaic response, we studied in detail the energy-band alignment of ultrathin layers of ZnO (3-60 nm) with Ag. Our analysis indicated that an ‘electrostatic potential cliff' is formed within the first 1-2 nm of ZnO. In addition, oxygen vacancies, presumably generated by AgxO-Zn bonds, form mid-gap acceptor states within these first few nm. Both effects facilitate a valence band-to-defect state optical transition that is confined to the interface region. The second type of defects - hole-trap states associated with zinc hydroxide - are spread throughout the ZnO layer and dominate the supra-band-gap photovoltaic response. These findings have potential implications in emerging technologies such as photocatalytic Ag/ZnO heterostructures that will utilize the long-lived charges for chemical work or other optoelectronic applications.
AB - Zinc oxide, a wide-band-gap semiconductor, shows intriguing optoelectronic properties when coupled with Ag. Specifically, an absorbance band in the visible range that is not apparent in the separated materials emerges when the interface is formed. Interestingly, photoexcitation of this "interface band"or band-to-band results in a counterintuitive photovoltaic response when a supra/sub-band-gap light is shone. To investigate the origin of this absorbance band and photovoltaic response, we studied in detail the energy-band alignment of ultrathin layers of ZnO (3-60 nm) with Ag. Our analysis indicated that an ‘electrostatic potential cliff' is formed within the first 1-2 nm of ZnO. In addition, oxygen vacancies, presumably generated by AgxO-Zn bonds, form mid-gap acceptor states within these first few nm. Both effects facilitate a valence band-to-defect state optical transition that is confined to the interface region. The second type of defects - hole-trap states associated with zinc hydroxide - are spread throughout the ZnO layer and dominate the supra-band-gap photovoltaic response. These findings have potential implications in emerging technologies such as photocatalytic Ag/ZnO heterostructures that will utilize the long-lived charges for chemical work or other optoelectronic applications.
KW - Ag-ZnO
KW - atomic layer deposition
KW - interface defect states
KW - surface photovoltage
KW - thin films
UR - http://www.scopus.com/inward/record.url?scp=85117782521&partnerID=8YFLogxK
U2 - https://doi.org/10.1021/acsami.1c11566
DO - https://doi.org/10.1021/acsami.1c11566
M3 - Article
C2 - 34628851
SN - 1944-8244
VL - 13
SP - 49423
EP - 49432
JO - ACS applied materials & interfaces
JF - ACS applied materials & interfaces
IS - 41
ER -