2023
DOI: 10.1016/j.jechem.2022.10.004
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High efficiency CZTSSe solar cells enabled by dual Ag-passivation approach via aqueous solution process

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Cited by 14 publications
(10 citation statements)
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“…In addition to the E U characterization, we estimated potential fluctuations (γ opt ) using the Shklovskii and Efros model. , As depicted in Figure d, our analysis revealed γ opt values of 57.1, 54.0, and 53.2 meV for CZTSSe-A, CZTSSe-N, and CZTSSe-C solar cells, respectively. The higher γ opt value observed in the CZTSSe-A solar cell can be attributed to an increased number of recombination losses, which is consistent with the E U trend.…”
Section: Resultsmentioning
confidence: 98%
“…In addition to the E U characterization, we estimated potential fluctuations (γ opt ) using the Shklovskii and Efros model. , As depicted in Figure d, our analysis revealed γ opt values of 57.1, 54.0, and 53.2 meV for CZTSSe-A, CZTSSe-N, and CZTSSe-C solar cells, respectively. The higher γ opt value observed in the CZTSSe-A solar cell can be attributed to an increased number of recombination losses, which is consistent with the E U trend.…”
Section: Resultsmentioning
confidence: 98%
“…This downshift in CBM leads to an increase in spike-type conduction band offset (CBO). When the CBO is larger in spike-type configuration, the device exhibits a red kink in the JV curve. , We measured JVT curves for the three devices, and the results are displayed in Figure S8, where JV curves are measured under various conditions: dark, white light illumination, red-filtered illumination with long-pass filter at 665 nm, and yellow-filtered illumination with long-pass filter at 500 nm at 300 and 240 K. The Rb-CIGSSe and Cs-CIGSSe devices exhibit a red kink in the JV curves measured at 240 K, while the CIGSSe device showed no noticeable red kink compared to the other devices. This JV result supports an increase of CBO via the downshift of the CBM in the Rb-CIGSSe and Cs-CIGSSe cells, as shown in Figure .…”
Section: Resultsmentioning
confidence: 99%
“…The full device structure was then completed with the deposition of i-ZnO (∼50 nm) and tin-doped indium oxide (ITO) (∼300 nm) layers by radio frequency (RF) magnetron sputtering. Detailed information on the buffer and window layer fabrication processes can be found elsewhere. ,, No additional antireflection coatings were applied to the fabricated devices. For measurement of device performance, we mechanically scribed the cell with an area of 0.20 cm 2 .…”
Section: Methodsmentioning
confidence: 99%
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“…[23,30] Our group also previously achieved a PCE of 12.43% using Ag-alloyed kesterite (Cu 1-x Ag x ) 2 ZnSn(S,Se) 4 (ACZTSSe) absorbers. [31] 2) For the passivation of the heterojunction interface, wide-bandgap oxide materials have been utilized to suppress the interface recombination, which could increase J SC , V OC , and FF. [32][33][34] For example, Al 2 O 3 , [32] TiO 2 , [33] and SnO 2 [34] films have been applied to kesterite CZTSSe solar cells using atomic layer deposition (ALD), spin coating and successive ionic layer adsorption and reaction, respectively.…”
Section: Introductionmentioning
confidence: 99%