Ordered Vacancy Compound Formation at the Interface of Cu(In,Ga)Se<sub>2</sub> Absorber with Sputtered In<sub>2</sub>S<sub>3</sub>‐Based Buffers: An Atomic‐Scale Perspective

The design of a Cd‐free and wider‐bandgap buffer layer is stringent for future Cu(In,Ga)Se 2 (CIGSe) thin‐film solar cell applications. For that, an In 2 S 3 buffer layer alloyed with a limited amount of O (well below 25 mol%) has been proposed as a pertinent alternative solution to CdS or Zn(O,S) buffers. However, the chemical stability of the In 2 S 3 /CIGSe heterointerface when O is added is not completely clear. Therefore, in this work, the buffer/absorber interface for a series of sputter‐deposited In 2 S 3 buffers with and without O is investigated. It is found that the solar cell with the highest open‐circuit voltage is obtained for the O‐free In 2 S 3 buffer sputtered at 220 °C. This improved open‐circuit voltage could be explained by the presence of a 20 nm‐thick ordered vacancy compound (OVC) at the absorber surface. A much thinner OVC layer (5 nm) or even the absence of this layer is found for the cell with In 2 (O 0.25 S 0.75 ) 3 buffer layer where O is inserted. The volume fraction of the OVC layer is directly linked with the magnitude of Cu diffusion from the CIGSe surface into the In 2 (O x S 1− x ) 3 buffer layer. The O addition strongly reduces the Cu diffusion inside the buffer layer up to complete suppression for very high O contents in the buffer. Finally, it is discussed that the presence of the OVC layer may lower the valence band maximum, thereby forming a hole barrier, suppressing charge carrier recombination at the In 2 (O x S 1− x ) 3 /CIGSe interface, which could result in an increased open‐circuit voltage.

Authors

Institutions

Publication Details

Journal
Solar RRL
Published
2024-11-24
DOI
https://doi.org/10.1002/solr.202400574
Citations
3
Primary Topic
Chalcogenide Semiconductor Thin Films
Type
article
Field-Weighted Citation Impact
0.63
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

Ordered Vacancy Compound Formation at the Interface of Cu(In,Ga)Se2 Absorber with Sputtered In2S3‐Based Buffers: An Atomic‐Scale Perspective

Ana Kanevce, Dimitrios Hariskos, Roland Scheer, Dagmar Gerthsen et al.
3 citations
Solar RRL
Chalcogenide Semiconductor Thin Films
0.63
article

Ordered Vacancy Compound Formation at the Interface of Cu(In,Ga)Se2 Absorber with Sputtered In2S3‐Based Buffers: An Atomic‐Scale Perspective

Ana Kanevce, Dimitrios Hariskos, Roland Scheer, Dagmar Gerthsen, Jens Keutgen, Xiaowei Jin, Wolfram Witte, Mohit Raghuwanshi, Wolfram Hempel, Oana Cojocaru‐Mirédin, Reinhard Schneider
article en
3 citations

Abstract

The design of a Cd‐free and wider‐bandgap buffer layer is stringent for future Cu(In,Ga)Se 2 (CIGSe) thin‐film solar cell applications. For that, an In 2 S 3 buffer layer alloyed with a limited amount of O (well below 25 mol%) has been proposed as a pertinent alternative solution to CdS or Zn(O,S) buffers. However, the chemical stability of the In 2 S 3 /CIGSe heterointerface when O is added is not completely clear. Therefore, in this work, the buffer/absorber interface for a series of sputter‐deposited In 2 S 3 buffers with and without O is investigated. It is found that the solar cell with the highest open‐circuit voltage is obtained for the O‐free In 2 S 3 buffer sputtered at 220 °C. This improved open‐circuit voltage could be explained by the presence of a 20 nm‐thick ordered vacancy compound (OVC) at the absorber surface. A much thinner OVC layer (5 nm) or even the absence of this layer is found for the cell with In 2 (O 0.25 S 0.75 ) 3 buffer layer where O is inserted. The volume fraction of the OVC layer is directly linked with the magnitude of Cu diffusion from the CIGSe surface into the In 2 (O x S 1− x ) 3 buffer layer. The O addition strongly reduces the Cu diffusion inside the buffer layer up to complete suppression for very high O contents in the buffer. Finally, it is discussed that the presence of the OVC layer may lower the valence band maximum, thereby forming a hole barrier, suppressing charge carrier recombination at the In 2 (O x S 1− x ) 3 /CIGSe interface, which could result in an increased open‐circuit voltage.

Solar RRLVol. 8(23)
Karlsruhe Institute of Technology (DE), University of Freiburg (DE), Fraunhofer Institute for Applied Solid State Physics (DE), Zentrum für Sonnenenergie- und Wasserstoff-Forschung Baden-Württemberg (DE), Martin Luther University Halle-Wittenberg (DE), RWTH Aachen University (DE)
Openalex Percentile: Top 30%
Chalcogenide Semiconductor Thin Films
0.63
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.