2014
DOI: 10.1142/9781848167681_0003
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Crystalline Silicon Solar Cells

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Cited by 5 publications
(2 citation statements)
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“…Since the bandgap difference of ∼0.1 eV at the bandgap of ∼1.5 eV should ideally lead to a J sc difference of ∼4 mA cm − 2 (ref. 31 ), the observed substantially lower J sc value indicates inadequate light absorption, which is attributable to the thin absorber layer. Although PS absorbs light strongly, its absorption at the long wavelength range near the absorption edge (∼800 nm) is less ideal.…”
Section: Discussionmentioning
confidence: 94%
“…Since the bandgap difference of ∼0.1 eV at the bandgap of ∼1.5 eV should ideally lead to a J sc difference of ∼4 mA cm − 2 (ref. 31 ), the observed substantially lower J sc value indicates inadequate light absorption, which is attributable to the thin absorber layer. Although PS absorbs light strongly, its absorption at the long wavelength range near the absorption edge (∼800 nm) is less ideal.…”
Section: Discussionmentioning
confidence: 94%
“…[12][13][14] The core structure of c-Si solar cells is a pn-homojunction by diffusing n (or p)-type emitter on p (or n)-type silicon substrate. [15] In c-Si solar cells, this pn-homojunction is still used today and can achieve high power conversion efficiency (PCE) of ≈25% by the well-known passivated emitter and rear cell and related architectures, such as passivated emitter locally diffused and passivated emitter rear totally diffused cells. [16][17][18] Unlike c-Si solar cells, the CIGS solar cell device is based on a pn-heterojunction which formed between p-type CIGS and n-type CdS layer.…”
mentioning
confidence: 99%