Abstract
Cu 2ZnSn(S,Se) 4 (CZTSSe) is a promising material for thin-film photovoltaics, however, the open-circuit voltage ( V OC) deficit of CZTSSe prevents the device performance from exceeding 13% conversion efficiency. CZTSSe is a heavily compensated material that is rich in point defects and prone to the formation of secondary phases. The landscape of these defects is complex and some mitigation is possible by employing non-stoichiometric conditions. Another route used to reduce the effects of undesirable defects is the doping and alloying of the material to suppress certain defects and improve crystallization, such as with germanium. The majority of works deposit Ge adjacent to a stacked metallic precursor deposited by physical vapour deposition before annealing in a selenium rich atmosphere. Here, we use an established hot-injection process to synthesise Cu 2ZnSnS 4 nanocrystals of a pre-determined composition, which are subsequently doped with Ge during selenisation to aid recrystallisation and reduce the effects of Sn species. Through Ge incorporation, we demonstrate structural changes with a negligible change in the energy bandgap but substantial increases in the crystallinity and grain morphology, which are associated with a Ge-Se growth mechanism, and gains in both the V OC and conversion efficiency. We use surface energy-filtered photoelectron emission microscopy (EF-PEEM) to map the surface work function terrains and show an improved electronic landscape, which we attribute to a reduction in the segregation of low local effective work function (LEWF) Sn(II) chalcogenide phases.
Original language | English |
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Pages (from-to) | 70-84 |
Number of pages | 15 |
Journal | Faraday Discussions |
Volume | 239 |
Early online date | 13 Jul 2022 |
DOIs | |
Publication status | E-pub ahead of print - 13 Jul 2022 |
Bibliographical note
Funding Information:This work was supported by the Engineering and Physical Sciences Research Council (EPSRC) via grants EP/S023836/1, EP/V008692/1, EP/V008676/1, EP/L017792/1, and EP/T005491/1. We are thankful for the EPSRC strategic equipment grants EP/K035746/1 and EP/M000605/1. The authors also appreciate the support from the North East Centre for Energy Materials (NECEM) (EP/R021503/1), the British Council Newton Fund Institutional Links Grant (CRP01286) and the Royal Society of Chemistry (E20-9404). The authors thank and acknowledge use of the University of Bristol NanoESCA II Laboratory.
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© 2022 The Royal Society of Chemistry