Please use this identifier to cite or link to this item: http://hdl.handle.net/10603/423235
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dc.date.accessioned2022-12-08T12:29:07Z-
dc.date.available2022-12-08T12:29:07Z-
dc.identifier.urihttp://hdl.handle.net/10603/423235-
dc.description.abstractThe perovskite solar cells are an emerging photovoltaic technology as it reaches 25.5% efficiency within a decade. Due to this rapid advancement researchers have developed various perovskite absorber layers, charge transport layers, transparent conducting oxides and metal contacts. However, it is quite complicated to fabricate numerous combinations of these layers and hence the simulation is an efficient way to analyse the best possible combination which can result in higher device performance. In the present thesis work, the numerical simulation of lead-free perovskite solar cells is performed using SCAPS 1D software. The current study brings forth the numerical simulation of various lead-free perovskite alternatives having narrow and wide bandgap configurations. For the narrow bandgap configuration, the FA0.75MA0.25Sn0.25 Ge0.5I3 and CsSnGeI3 based perovskite layers are considered. However, for the wide bandgap application, the CH3NH3GeI3 based perovskite layer is considered. The perovskite solar cells using these layers are optimized based on charge transport layers, perovskite absorber layer thickness, perovskite absorber defect density and their energy band alignment with respect to the contacts. To investigate the effect of charge transport layers (i.e., hole transport layer and electron transport layer), the work shows that the correlation of VOC with the built-in potential (Vbi). The results disclosed that to attain better VOC and PV performance, the device should exhibit the better Vbi and proper band alignment that allows the efficient facilitation of charge carriers, along with good charge carrier mobility. Thus, it is suggested that for the proper transport of electrons, the conduction band minimum of the electron transport layer (ETL) must lie below the conduction band minimum of the perovskite layer. Similarly, in the case of hole transport, the valence band maximum of the hole transport layer must lie above that of the perovskite layer.
dc.format.extent139p.
dc.languageEnglish
dc.relation
dc.rightsuniversity
dc.titleDesign and Simulation of Electron and Hole Transport Layer for Lead Free Perovskite Solar Cell Application
dc.title.alternative
dc.creator.researcherSingh, Neelima
dc.subject.keywordEngineering
dc.subject.keywordEngineering and Technology
dc.subject.keywordEngineering Electrical and Electronic
dc.subject.keywordPerovskite
dc.subject.keywordPerovskite Solar Cell
dc.description.note
dc.contributor.guideAgarwal, Mohit and Agarwal, Alpana
dc.publisher.placePatiala
dc.publisher.universityThapar Institute of Engineering and Technology
dc.publisher.institutionDepartment of Electronics and Communication Engineering
dc.date.registered
dc.date.completed2022
dc.date.awarded2022
dc.format.dimensions
dc.format.accompanyingmaterialNone
dc.source.universityUniversity
dc.type.degreePh.D.
Appears in Departments:Department of Electronics and Communication Engineering

Files in This Item:
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01_title.pdfAttached File219.32 kBAdobe PDFView/Open
02_prelim pages.pdf935.5 kBAdobe PDFView/Open
03_content.pdf214.05 kBAdobe PDFView/Open
04_abstract.pdf226.97 kBAdobe PDFView/Open
05_chapter 1.pdf1.41 MBAdobe PDFView/Open
06_chapter 2.pdf471.94 kBAdobe PDFView/Open
07_chapter 3.pdf3.91 MBAdobe PDFView/Open
08_chapter 4.pdf1.89 MBAdobe PDFView/Open
09_chapter 5.pdf6.43 MBAdobe PDFView/Open
10_chapter 6.pdf236.24 kBAdobe PDFView/Open
11_annexures.pdf331.92 kBAdobe PDFView/Open
80_recommendation.pdf356.98 kBAdobe PDFView/Open


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