Source abstract
Abstract
Besides the open circuit voltage (VOC) deficit, fill factor (FF) is the second most significant parameter deficit for earth‐abundant kesterite solar cell technology. Here, various pathways for FF loss are discussed, with focus on the series resistance issue and its various contributing factors. Electrical and physical characterizations of the full range of bandgap (Eg = 1.0–1.5 eV) Cu2ZnSn(SxSe1−x)4 (CZTSSe) devices, as well as bare and exfoliated films with various S/(S + Se) ratios, are performed. High intensity Suns‐VOC measurement indicates a nonohmic junction developing in high bandgap CZTSSe. Grazing incidence X‐ray diffraction, Raman mapping, field emission scanning electron microscopy, and X‐ray photoelectron spectroscopy indicate the formation of Sn(S,Se)2, Mo(S,Se)2, and Zn(S,Se) at the high bandgap CZTSSe/Mo interface, contributing to the increased series resistance (RS) and nonohmic back contact characteristics. This study offers some clues as to why the record‐CZTSSe solar cells occur within a bandgap range centered around 1.15 eV and offers some direction for further optimization.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Chalcogenide Semiconductor Thin Films · Quantum Dots Synthesis And Properties · Copper-based nanomaterials and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Division of Physics and Applied Physics School of Physical and Mathematical Sciences Nanyang Technological University 21 Nanyang Link 637371 Singapore
Energy Research Institute @ NTU (ERI@N) Research Techno Plaza Level 5, 50 Nanyang Drive 639798 Singapore
IBM TJ Watson Research Center Physical Sciences Department 1101 Kitchawan Rd Yorktown Heights NY 10598 USA
Tokyo Ohka Kogyo Co. Ltd. 150 Nakamaruko Nakahara‐ku, Kawasaki Kanagawa 211‐0012 Japan
Duke University Durham NC 27708 USA
Funding
ERI@N · U.S. Department of Energy, Energy Efficiency and Renewable Energy Program
References (57)
Show source-provided references
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29. This is mainly due to reduction in carrier density as the band gap increases (see Table 2).
35. TheRSis also extracted using Lambert‐W fitting method.
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