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Although back-surface passivation plays an important role in high-efficiency photovoltaics, it has not yet been definitively demonstrated for CdTe. Here, we present a solution-based process, which achieves passivation and improved electrical performance when very small amounts of oxidized Al species are deposited at the back surface of CdTe devices. The open circuit voltage () is increased and the fill factor (FF) and photoconversion efficiency (PCE) are optimized when the total amount added corresponds to ∼1 monolayer, suggesting that the passivation is surface specific. Addition of further Al species, present in a sparse alumina-like layer, causes the FF and PCE to drop as the interface layer becomes blocking to current flow. The optimized deposit increases the average baseline PCE for both Cu-free devices and devices where Cu is present as a dopant. The greatest improvement is found when the Al species are deposited prior to the CdCl activation step and Cu is employed. In this case, the best-cell efficiency was improved from 12.6 to 14.4%. Time-resolved photoluminescence measurements at the back surface and quantum efficiency measurements performed at the maximum power point indicate that the performance enhancement is due to a reduction in the interface recombination current at the back surface.
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http://dx.doi.org/10.1021/acsami.0c12800 | DOI Listing |
Adv Mater
July 2025
Michael Grätzel Center for Mesoscopic Solar Cells, Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Luoyu Road 1037, Wuhan, Hubei, 430074, P. R. China.
Carbon-based hole transport layer-free (C-HTL-free) perovskite solar cells (PSCs) are promising for low-cost and stable photovoltaics, but the HTL absence deteriorates their power conversion efficiency (PCE) due to the lack of back surface field (BSF). In this work, the benefits of forming dual BSFs in improving the PCE of C-HTL-free PSCs are first investigated by simulation. Then, trityl tetrakis(pentafluorophenyl)borate (TrTPFB) is introduced into the C-HTL-free PSCs by post-treatment for the first time, which enables the formation of dual BSFs.
View Article and Find Full Text PDFJ Environ Manage
March 2025
Photovoltaic Reliability Laboratory, Arizona State University, Mesa, AZ, USA.
This paper presents a database compiling 97 sample results based on U.S. Environmental Protection Agency (EPA) Toxicity Characteristic Leaching Procedure (TCLP) testing of 33 photovoltaic (PV) modules (1-3 samples per module) of differing designs covering 16 different manufacturers.
View Article and Find Full Text PDFACS Appl Mater Interfaces
January 2025
National Renewable Energy Laboratory, Golden, Colorado 80401, United States.
The direct epitaxial growth of high-quality III-V semiconductors on Si is a challenging materials science problem with a number of applications in optoelectronic devices, such as solar cells and on-chip lasers. We report the reduction of dislocation density in GaAs solar cells grown directly on nanopatterned V-groove Si substrates by metal-organic vapor-phase epitaxy. Starting from a template of GaP on V-groove Si, we achieved a low threading dislocation density (TDD) of 3 × 10 cm in the GaAs by performing thermal cycle annealing of the GaAs followed by growth of InGaAs dislocation filter layers.
View Article and Find Full Text PDFSmall
December 2024
Institute of Micronano Devices & Solar Cells, College of Physics & Information Engineering, Fuzhou University, Fuzhou, 350108, Peoples Republic of China.
Antimony selenosulfide (Sb(S,Se)) solar cells have achieved an efficiency of over 10.0%. However, the uncontrollable hydrothermal process makes preparing high-quality Sb(S,Se) thin films a bottleneck for efficient Sb(S,Se) solar cell.
View Article and Find Full Text PDFNanomaterials (Basel)
May 2024
Department of Physics, School of Science, Wuhan University of Technology, Wuhan 430070, China.
The recombination of charges and thermal excitation of carriers at the interface between methylammonium lead iodide perovskite (PVK) and the carbon electrode are crucial factors that affect the optoelectronic performance of carbon-based hole transport layer (HTL)-free perovskite photodetectors. In this work, a method was employed to introduce SnS quantum dots (QDs) on the back surface of perovskite, which passivated the defect states on the back surface of perovskite and addressed the energy-level mismatch issue between perovskite and carbon electrode. Performance testing of the QDs and the photodetector revealed that SnS QDs possess energy-level structures that are well matched with perovskite and have high absorption coefficients.
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