2017
DOI: 10.1021/acsenergylett.7b00236
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Recombination in Perovskite Solar Cells: Significance of Grain Boundaries, Interface Traps, and Defect Ions

Abstract: Trap-assisted recombination, despite being lower as compared with traditional inorganic solar cells, is still the dominant recombination mechanism in perovskite solar cells (PSCs) and limits their efficiency. We investigate the attributes of the primary trap-assisted recombination channels (grain boundaries and interfaces) and their correlation to defect ions in PSCs. We achieve this by using a validated device model to fit the simulations to the experimental data of efficient vacuum-deposited p–i–n and n–i–p … Show more

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Cited by 935 publications
(741 citation statements)
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References 66 publications
(199 reference statements)
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“…As we discuss above, NMA is primarily located at grain surface. There is extensive evidence for trap location at grain surface in MAPbI 3 . We thus conclude that NMA is able to passivate grain surface trap states, resulting in the observed increase in device voltage with NMA concentration.…”
Section: Resultsmentioning
confidence: 62%
“…As we discuss above, NMA is primarily located at grain surface. There is extensive evidence for trap location at grain surface in MAPbI 3 . We thus conclude that NMA is able to passivate grain surface trap states, resulting in the observed increase in device voltage with NMA concentration.…”
Section: Resultsmentioning
confidence: 62%
“…These trapped photo-generated carriers would most probably contribute to recombination loss. Furthermore, the energy levels of H2 and E1 are located near to the midgap, which significantly increase the recombination possibility of photo-generated carriers 46 . Therefore, the H2 and E1 are the dominant defects that influence the shift of quasi-Fermi levels and trap-assisted recombination, and then the V OC and J SC of the solar cells.…”
Section: Resultsmentioning
confidence: 99%
“…For the most stable arrangements ( Figure S13, Supporting Information) of the iodine vacancies in such electron-rich regions, a self-localization of the electronic excitation ensues upon geometric relaxation (Figure 2a) and a discrete trap level emerges below the conduction band edge (Figure 2b). Notably, deep states have been identified experimentally as electron traps, [21,32,36] Since the conduction band is predominantly composed of p orbitals of lead ions, the deep electron traps could possibly originate from the unsaturated lead atoms. The resulting localized electronic excitation in Figure 2a is thus prompted by the formation of a lead-centered defect with two excess holes.…”
Section: Resultsmentioning
confidence: 99%