Sökning: L773:1944 8244 OR L773:1944 8252 >
Influence of the Re...
Influence of the Rear Interface on Composition and Photoluminescence Yield of CZTSSe Absorbers: A Case for an Al2O3 Intermediate Layer
-
Antonio Cabas, Vidani (författare)
-
Léo, Choubrac (författare)
-
Jose, Marquez-Prieto (författare)
-
visa fler...
-
Thomas, Unold (författare)
-
Matthias, Maiberg (författare)
-
Roland, Scheer (författare)
-
- Li, Hu, 1986- (författare)
- Uppsala universitet,Tillämpad materialvetenskap,Shandong Univ, Sch Microelect, Jinan 250100, Peoples R China,Electron microscopy and Nanoengineering
-
- Leifer, Klaus, 1965- (författare)
- Uppsala universitet,Tillämpad materialvetenskap,Electron microscopy and Nanoengineering
-
Robin, Pauer (författare)
-
Evgeniia, Gilshtein (författare)
-
A. N., Tiwari (författare)
-
Yaroslav, Romanyuk (författare)
-
visa färre...
-
(creator_code:org_t)
- 2021-04-19
- 2021
- Engelska.
-
Ingår i: ACS Applied Materials and Interfaces. - : American Chemical Society (ACS). - 1944-8244 .- 1944-8252. ; 13:16, s. 19487-19496
- Relaterad länk:
-
https://doi.org/10.1...
-
visa fler...
-
https://uu.diva-port... (primary) (Raw object)
-
https://pubs.acs.org...
-
https://urn.kb.se/re...
-
https://doi.org/10.1...
-
visa färre...
Abstract
Ämnesord
Stäng
- The rear interface of kesterite absorbers with Mo back contact represents one of the possible sources of nonradiative voltage losses (Delta V-oc,V-nrad) because of the reported decomposition reactions, an uncontrolled growth of MoSe2, or a nonoptimal electrical contact with high recombination. Several intermediate layers (IL), such as MoO3, TiN, and ZnO, have been tested to mitigate these issues, and efficiency improvements have been reported. However, the introduction of IL also triggers other effects such as changes in alkali diffusion, altered morphology, and modifications in the absorber composition, all factors that can also influence Delta V-oc,V-nrad. In this study, the different effects are decoupled by designing a special sample that directly compares four rear structures (SLG, SLG/Mo, SLG/Al2O3, and SLG/Mo/Al2O3) with a Na-doped kesterite absorber optimized for a device efficiency >10%. The IL of choice is Al2O3 because of its reported beneficial effect to reduce the surface recombination velocity at the rear interface of solar cell absorbers. Identical annealing conditions and alkali distribution in the kesterite absorber are preserved, as measured by time-of-flight secondary ion mass spectrometry and energy-dispersive X-ray spectroscopy. The lowest Delta V-oc,V-nrad of 290 mV is measured for kesterite grown on Mo, whereas the kesterite absorber on Al2O3 exhibits higher nonradiative losses up to 350 mV. The anticipated field-effect passivation from Al2O3 at the rear interface could not be observed for the kesterite absorbers prepared by the two-step process, further confirmed by an additional experiment with air annealing. Our results suggest that Mo with an in situ formed MoSe2 remains a suitable back contact for high-efficiency kesterite devices.
Publikations- och innehållstyp
- ref (ämneskategori)
- art (ämneskategori)
Hitta via bibliotek
Till lärosätets databas
- Av författaren/redakt...
-
Antonio Cabas, V ...
-
Léo, Choubrac
-
Jose, Marquez-Pr ...
-
Thomas, Unold
-
Matthias, Maiber ...
-
Roland, Scheer
-
visa fler...
-
Li, Hu, 1986-
-
Leifer, Klaus, 1 ...
-
Robin, Pauer
-
Evgeniia, Gilsht ...
-
A. N., Tiwari
-
Yaroslav, Romany ...
-
visa färre...
- Artiklar i publikationen
-
ACS Applied Mate ...
- Av lärosätet
-
Uppsala universitet