Cuprous oxide (CuO) thin films were chemically deposited from a solution onto GaAs(100) and (111) substrates using a simple three-component solution at near-ambient temperatures (10-60 °C). Interestingly, a similar deposition onto various other substrates including Si(100), Si(111), glass, fluorine-doped tin oxide, InP, and quartz resulted in no film formation. Films deposited on both GaAs(100) and (111) were found alongside substantial etching of the substrates. The etching of GaAs(100) was uneven, resulting in pyramid-like vacancies, while for GaAs(111), the etching was more even and resulted in a flat interface. X-ray diffraction measurements indicated highly preferential (110) growth of CuO regardless of GaAs substrate orientation, while TEM and a selected area of electron diffraction pointed out epitaxial growth on both substrates. X-ray photoelectron spectroscopy confirmed the diffusion of copper ions into the GaAs up to depths of 20 nm and the formation of intermediate phases at the interface. Raman spectroscopy indicated high structural quality of the films and showed good agreement with TEM and XRD results and Raman shifts corresponding to CuO, with no frequencies typical of CuO. The GaAs substrate appears to play a critical and unusual role in the deposition of CuO thin films on GaAs, which allows for growth of CuO in a previously unreported mechanism.
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http://dx.doi.org/10.1021/acsami.4c16485 | DOI Listing |
ACS Appl Mater Interfaces
January 2025
Department of Materials Engineering, Ben-Gurion University of the Negev, Beer-Sheva 8410501, Israel.
Cuprous oxide (CuO) thin films were chemically deposited from a solution onto GaAs(100) and (111) substrates using a simple three-component solution at near-ambient temperatures (10-60 °C). Interestingly, a similar deposition onto various other substrates including Si(100), Si(111), glass, fluorine-doped tin oxide, InP, and quartz resulted in no film formation. Films deposited on both GaAs(100) and (111) were found alongside substantial etching of the substrates.
View Article and Find Full Text PDFSensors (Basel)
December 2024
School of Microelectronics, Xi'an Jiaotong University, Xi'an 710049, China.
The combination of ZnO with narrow bandgap materials such as CuO is now a common method to synthesize high-performance optoelectronic devices. This study focuses on optimizing the performance of p-CuO/n-ZnO heterojunction pyroelectric photodetectors, fabricated through magnetron sputtering, by leveraging the pyro-phototronic effect. The devices' photoresponse to UV (365 nm) and visible (405 nm) lasers is thoroughly examined.
View Article and Find Full Text PDFMaterials (Basel)
December 2024
Department of Mechatronics Engineering, National Changhua University of Education, Changhua 50007, Taiwan.
Antimony selenide (SbSe) shows promise for photovoltaics due to its favorable properties and low toxicity. However, current SbSe solar cells exhibit efficiencies significantly below their theoretical limits, primarily due to interface recombination and non-optimal device architectures. This study presents a comprehensive numerical investigation of SbSe thin-film solar cells using SCAPS-1D simulation software, focusing on device architecture optimization and interface engineering.
View Article and Find Full Text PDFACS Appl Mater Interfaces
January 2025
Gordon A. and Mary Cain Department of Chemical Engineering, Louisiana State University, Baton Rouge, Louisiana 70803, United States.
Future processes and materials are needed to enable multichip packages with chip-to-chip (C2C) data rates of 50 GB/s or higher. This presents a fundamental challenge because of the skin effect, which exacerbates signal transmission losses at high frequencies. Our results indicate that smooth copper interconnects with relatively thin cuprous oxides (CuO, Cu) and amine-functional silane adhesion promoters improve interfacial adhesion with epoxy dielectrics by nearly an order of magnitude.
View Article and Find Full Text PDFMicrosc Microanal
November 2024
NCEM, Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley 94720, USA.
A new method for dark field imaging is introduced, which uses scanned electron diffraction (or 4DSTEM-4-dimensional scanning transmission electron microscopy) datasets as its input. Instead of working on simple summation of intensity, it works on a sparse representation of the diffraction patterns in terms of a list of their diffraction peaks. This is tested on a thin perovskite film containing structural ordering resulting in additional superlattice spots that reveal details of domain structures, and is shown to give much better selectivity and contrast than conventional virtual dark field imaging.
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