Experimental Insights of CZTS Thin Film as a Photovoltaic Absorber Deposited by RF Magnetron Sputtering and Spin Coating
| dc.contributor.author | Gupta, Ashoke Kumar Sen | |
| dc.date.accessioned | 2026-07-06T20:58:30Z | |
| dc.date.available | 2026-07-06T20:58:30Z | |
| dc.date.issued | 31-Jul-2023 | |
| dc.description | A PhD Thesis from the Department of Electrical and Electronic Engineering | |
| dc.description.abstract | This thesis investigates the impact of deposition procedures on the properties of Cu2ZnSnS4 | |
| dc.description.abstract | (CZTS) thin films and the resultant characteristics of CZTS thin film solar cells. The present | |
| dc.description.abstract | study investigated CZTS absorber layer deposited by two distinct techniques namely RF | |
| dc.description.abstract | magnetron sputtering utilizing an off-stoichiometric single quaternary CZTS target and sol-gel | |
| dc.description.abstract | spin coating. The focus of investigation pertains to buffer materials that are free from Cd | |
| dc.description.abstract | and have the potential to improve band alignment. The present study also investigates the | |
| dc.description.abstract | potential of ZnO:Ga (GZO) as a transparent conducting oxide (TCO) layer for CZTS solar | |
| dc.description.abstract | cell applications as an alternative to the conventional ZnO:Al (AZO). Because of its longevity, | |
| dc.description.abstract | microelectronic compatibility, and efficiency, Si-based PV technology dominates. Si with low | |
| dc.description.abstract | indirect band gap absorption and sophisticated production methods like high temperature | |
| dc.description.abstract | treatment and ion implantation are bottlenecks. Chalcogenide-based thin film PV technologies | |
| dc.description.abstract | may lower PV costs. Because of their availability and non-toxicity, kesterite semiconductors | |
| dc.description.abstract | containing copper, zinc, tin, sulfur, and selenium are attractive alternatives to CdTe and | |
| dc.description.abstract | CIGS. Because of its 1.5 eV direct band gap, pure sulfide CZTS seems promising among | |
| dc.description.abstract | the three kesterites. Vacuum-based sputtering produces clean, homogenous kesterite thin | |
| dc.description.abstract | films, whereas non-vacuum spin-coating is appealing for component control and large-scale | |
| dc.description.abstract | manufacturing. Irrespective of the two fabrication processes described in this thesis, in order | |
| dc.description.abstract | to explore microstructural, morphological, optical, electrical, chemical oxidation states, and | |
| dc.description.abstract | photovoltaic properties, numerous characterization tools were used at the film and device | |
| dc.description.abstract | levels. These are X-ray Diffractometry (XRD), Raman spectroscopy, Field Emission Scanning | |
| dc.description.abstract | Electron Microscopy (FESEM), 3D profilometry, Ultraviolet-Visible Near Infra Red (UV-Vis | |
| dc.description.abstract | NIR) spectroscopy, X-Ray Photoelectron Spectroscopy (XPS), Hall-effect measurements, and I-V | |
| dc.description.abstract | characteristics. Some numerical studies were carried out using SCAPS-1D simulation tools in | |
| dc.description.abstract | accordance with experimental results to validate them. The process of sputtering thin films has | |
| dc.description.abstract | traditionally included a two-step approach. The use of elemental sulfur in conjunction with | |
| dc.description.abstract | vacuum deposition for the purpose of Rapid Thermal Annealing (RTA). Firstly, RF magnetron sputtered CZTS thin films with a single off-stoichiometric quaternary target were examined for | |
| dc.description.abstract | substrate temperature effects. It was found that, in-situ deposition may potentially replace | |
| dc.description.abstract | the necessity of a high-temperature annealing stage. Research conducted on the literature | |
| dc.description.abstract | pertaining to the alloying of CZTS with various elements such as Ag/Cu, Cd/Zn, Cd/Mg, and | |
| dc.description.abstract | Ge/Sn has demonstrated the potential to enhance device efficiencies through the manipulation | |
| dc.description.abstract | of band gap, control of defect size, mitigation of unwanted secondary phases, and modulation | |
| dc.description.abstract | of carrier concentration. However, despite these advancements, the efficiencies achieved by | |
| dc.description.abstract | these alloyed devices have not yet surpassed those of the devices currently in production. | |
| dc.description.abstract | Previous research have successfully adjusted the partial replacement of Zn cation with Cd, | |
| dc.description.abstract | leading to enhanced power conversion efficiency (PCE). Secondly, Ge-alloyed CZTS samples | |
| dc.description.abstract | were fabricated and examined. This work hypothesized that Ge-alloying, in which Sn is partly | |
| dc.description.abstract | replaced by Ge atoms, would minimize band gap fluctuations and band tailing, reducing the | |
| dc.description.abstract | open-circuit voltage deficit and improving device performance. It was found that, alloyed films | |
| dc.description.abstract | with G = 0.38 exhibited better morphology, crystallite size, microstrain, and dislocation density. | |
| dc.description.abstract | Thirdly, a novel co-doped (Cd,Mg) CZTS thin films and superstrate structured thin film solar | |
| dc.description.abstract | cells were fabricated and evaluated. Co-doped CZTS films and standard CdS heterointerface | |
| dc.description.abstract | band alignments have been investigated. Numerical simulation verified both tasks. This | |
| dc.description.abstract | task was predicted to lower the Cd content in the doped sample by adding Mg without | |
| dc.description.abstract | compromising the benefits of Cd alone. Cadmium (Cd) and Magnesium (Mg) exhibit partial | |
| dc.description.abstract | isoelectronic substitution at the Zn-site in kesterite CZTS. PCE increases significantly with 40% | |
| dc.description.abstract | partial cation substitution of Zn by Cd and Mg. +>2 deficit was reduced by 23% and "cliff-like" | |
| dc.description.abstract | CBO with a minimum energy of 0.12 eV was detected. In practical applications and in various | |
| dc.description.abstract | academic papers, it is often observed that there is a discrepancy in the conduction band offsets | |
| dc.description.abstract | between the absorber and buffer layers. Fourthly, in a study of the potential substitution of | |
| dc.description.abstract | the traditional CdS buffer layer by ZnS fabricated by SILAR, results suggested that favorable | |
| dc.description.abstract | "spike-like" CBO could be achieved. Finally, an alternative to the AZO window layer, GZO, | |
| dc.description.abstract | was proposed, and encouraging results were found in film transmittance and resistivity. | |
| dc.identifier.other | http://103.99.128.19:8080/jspui/handle/123456789/469 | |
| dc.identifier.uri | http://103.99.128.19:8080/xmlui/handle/123456789/469 | |
| dc.publisher | CUET | |
| dc.source | CUET Digital Repository | |
| dc.subject | d-free Solar Cells | |
| dc.subject | TCO Layer Optimization | |
| dc.subject | Buffer Layer Replacement | |
| dc.subject | Alloying and Co-doping Effects | |
| dc.subject | Energy Band Engineering | |
| dc.subject | Thin Film Solar Cell Efficiency Enhancement | |
| dc.title | Experimental Insights of CZTS Thin Film as a Photovoltaic Absorber Deposited by RF Magnetron Sputtering and Spin Coating |
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