Abstract:͑͒The chemical structure of the interface between a nominal In 2 S 3 buffer and a Cu͑In, Ga͒Se 2 ͑CIGSe͒ thin-film solar cell absorber was investigated by soft x-ray photoelectron and emission spectroscopy. We find a heavily intermixed, complex interface structure, in which Cu diffuses into ͑and Na through͒ the buffer layer, while the CIGSe absorber surface/interface region is partially sulfurized. Based on our spectroscopic analysis, a comprehensive picture of the chemical interface structure is proposed. ͓͔ … Show more
“…The XPS data of the as‐deposited samples with varying buffer layer thickness with and without the addition of Na points towards an interface with a small degree of Cu diffusion from the absorber into the buffer layer . Our XPS/XES study of In 2 S 3 layers from the Institut des Matériaux Jean Rouxel (IMN, University of Nantes) revealed a similar diffusion of Cu into the buffer …”
Section: The Chemical Structure Of Thin‐film Solar Cell Surfaces and mentioning
Thin‐film solar cells have great potential to overtake the currently dominant silicon‐based solar cell technologies in a strongly growing market. Such thin‐film devices consist of a multilayer structure, for which charge‐carrier transport across interfaces plays a crucial role in minimizing the associated recombination losses and achieving high solar conversion efficiencies. Further development can strongly profit from a high‐level characterization that gives a local, electronic, and chemical picture of the interface properties, which allows for an insight‐driven optimization. Herein, the authors' recent progress of applying a “toolbox” of high‐level laboratory‐ and synchrotron‐based electron and soft X‐ray spectroscopies to characterize the chemical and electronic properties of such applied interfaces is provided. With this toolbox in hand, the activities are paired with those of experts in thin‐film solar cell preparation at the cutting edge of current developments to obtain a deeper understanding of the recent improvements in the field, e.g., by studying the influence of so‐called “post‐deposition treatments”, as well as characterizing the properties of interfaces with alternative buffer layer materials that give superior efficiencies on large, module‐sized areas.
“…The XPS data of the as‐deposited samples with varying buffer layer thickness with and without the addition of Na points towards an interface with a small degree of Cu diffusion from the absorber into the buffer layer . Our XPS/XES study of In 2 S 3 layers from the Institut des Matériaux Jean Rouxel (IMN, University of Nantes) revealed a similar diffusion of Cu into the buffer …”
Section: The Chemical Structure Of Thin‐film Solar Cell Surfaces and mentioning
Thin‐film solar cells have great potential to overtake the currently dominant silicon‐based solar cell technologies in a strongly growing market. Such thin‐film devices consist of a multilayer structure, for which charge‐carrier transport across interfaces plays a crucial role in minimizing the associated recombination losses and achieving high solar conversion efficiencies. Further development can strongly profit from a high‐level characterization that gives a local, electronic, and chemical picture of the interface properties, which allows for an insight‐driven optimization. Herein, the authors' recent progress of applying a “toolbox” of high‐level laboratory‐ and synchrotron‐based electron and soft X‐ray spectroscopies to characterize the chemical and electronic properties of such applied interfaces is provided. With this toolbox in hand, the activities are paired with those of experts in thin‐film solar cell preparation at the cutting edge of current developments to obtain a deeper understanding of the recent improvements in the field, e.g., by studying the influence of so‐called “post‐deposition treatments”, as well as characterizing the properties of interfaces with alternative buffer layer materials that give superior efficiencies on large, module‐sized areas.
“…Soft X-ray techniques have proven to be very powerful for the investigation of applied systems such as thin-film solar cells [66][67][68][69][70][71], since they give detailed information about the local chemical environment of specific elements and the band gap in the surface-near bulk region [72]. In such applied systems, it would be especially interesting to perform in situ investigations, e.g., during wet-chemical treatment or deposition steps, of catalysts in operation, of batteries during charge/discharge cycles, and many more.…”
Section: H 2 O/cuin(sse) 2 -A Liquid/solid-interfacementioning
“…Solar cells with an indium sulfide buffer, as well as its interface with CIGSSe absorbers, have previously been well investigated . For undoped indium sulfide, the highest efficiencies have been reported after a thermal treatment that leads to a strong copper and sodium diffusion from the absorber into the buffer .…”
Doping an indium sulfide buffer layer with sodium is a promising route to replace the "state-of-the-art" CdS buffer layer in chalcopyrite-based thin-film solar cells, as it achieves efficiencies as high as 17.9% for large-area devices (30 cm × 30 cm). We report on the chemical and electronic structure of the In x S y :Na/CuIn(S,Se) 2 (CISSe) interface for thin-film solar cells by means of photoelectron, soft x-ray emission, and inverse photoemission spectroscopy. For as-deposited In x S y :Na buffer layers, we find a sulfur-poor surface and, in comparison to undoped In x S y and the standard CdS buffer, derive a large electronic surface band gap of 2.60 ± 0.11 eV.The conduction band offset at the buffer/absorber interface is a spike of 0.32 ± 0.10 eV. After annealing at 200°C to simulate the thermal load of subsequent cell manufacturing processes, an additional diffusion of copper and selenium from the absorber towards the buffer layer surface is observed, leading to a distinct electronic surface band gap decrease of the In x S y :Na buffer layer (to 2.11 ± 0.11 eV). We speculate that the diffusion of absorber elements causes a band gap widening at the former absorber surface and that both effects lead to a reduction of the conduction band spike for the buried In x S y :Na/CISSe interface after annealing. KEYWORDS band alignment, electronic structure, photoelectron spectroscopy, thin-film solar cells, x-ray emission spectroscopy
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