2015
DOI: 10.3390/en8054416
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Graded-Bandgap Solar Cells Using All-Electrodeposited ZnS, CdS and CdTe Thin-Films

Abstract: Abstract:A 3-layer graded-bandgap solar cell with glass/FTO/ZnS/CdS/CdTe/Au structure has been fabricated using all-electrodeposited ZnS, CdS and CdTe thin layers. The three semiconductor layers were electrodeposited using a two-electrode system for process simplification. The incorporation of a wide bandgap amorphous ZnS as a buffer/window layer to form glass/FTO/ZnS/CdS/CdTe/Au solar cell resulted in the formation of this 3-layer graded-bandgap device structure. This has yielded corresponding improvement in … Show more

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Cited by 67 publications
(48 citation statements)
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“…This is possible since only one defect level (1.39 eV) is present in this CdTe and close to the valence band edge therefore making Fermi level pinning highly probable at this level. This particular device structure of g/FTO/n-CdS/n-CdTe/Au n-n heterojunction + Schottky barrier is known to produce solar cells with high short-circuit current density as observed here, due to a possible combination of two depletion regions at both the n-n heterojunction and at the Schottky junction [19,20,32]. This situation creates a combined wide depletion region in the device.…”
Section: G/fto/cds/cdte/au Solar Cell Performance Assessmentmentioning
confidence: 91%
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“…This is possible since only one defect level (1.39 eV) is present in this CdTe and close to the valence band edge therefore making Fermi level pinning highly probable at this level. This particular device structure of g/FTO/n-CdS/n-CdTe/Au n-n heterojunction + Schottky barrier is known to produce solar cells with high short-circuit current density as observed here, due to a possible combination of two depletion regions at both the n-n heterojunction and at the Schottky junction [19,20,32]. This situation creates a combined wide depletion region in the device.…”
Section: G/fto/cds/cdte/au Solar Cell Performance Assessmentmentioning
confidence: 91%
“…This ensures that equal thickness of CdTe is deposited. This is possible because for a given deposition time (t), the theoretical thickness (T) of an electrodeposited semiconductor film according to the Faraday's equation (T = MtJ/nFρ) is known to be directly proportional to the deposition current density (J) [11,18] with the rest of the parameters [molecular mass (M), number of electrons involved in the formation (n), Faraday's constant (F) and density of the material (ρ)] being constants for any given material. In one set of the films deposited, graphite rod was used as anode material while platinum plate was used in the other set in order to study the effect of each of the anode materials on the properties of the CdTe thin films electroplated.…”
Section: Methodsmentioning
confidence: 99%
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“…Both the CCT and GCT treated glass/FTO/n-CdS/n-CdTe/p-CdTe layers were allowed to air-dry before heat treatment. The heat treatment was performed at 430˚C for 20 minutes in air atmosphere for samples undergoing each treatment based on previously optimised conditions [4], [23]- [25]. The CCT and GCT treated glass/FTO/n-CdS/n-CdTe/p-CdTe layers were then rinsed in DI water and dried in a stream of nitrogen afterwards.…”
Section: Post-growth Treatment Preparation and Applicationmentioning
confidence: 99%