2021
DOI: 10.1039/d0ta10535j
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Deep surface passivation for efficient and hydrophobic perovskite solar cells

Abstract: CF3PEAI, an amphipathic passivation agent, can passivate multiple perovskite defects leading to high performance and stability of perovskite solar cells.

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Cited by 78 publications
(79 citation statements)
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“…Very recently, the 4‐trifluoromethylphenylethylamine iodide (CF 3 PEAI, Figure ) or CF 3 PEAI‐based 2D layered perovskite was used to optimize the performance of PSCs on rigid substrate, exhibiting excellent effects on passivating defects and facilitating hole transfer. [ 22–24 ] Herein, efficient f‐PSCs were constructed via interface engineering of 2D/3D perovskite, i.e., the incorporation of a 2D perovskite (CF 3 PEA) 2 (FA) n −1 Pb n I 3 n +1 on top of the 3D perovskite FA 1− x MA x PbI 3 . The ultra‐thin 2D perovskite upshifted the energy level of 3D perovskite and decreased the energy gap between 3D perovskite and the hole transport layer (HTL) 2,2“,7,7”‐tetrakis‐( N , N ‐di(4‐methoxyphenyl‐amino)‐9,9'‐spirobi‐fluorene (Spiro‐OMeTAD), which facilitated the hole transfer due to the reduced energy barriers and charge extraction losses at the interface.…”
Section: Introductionmentioning
confidence: 99%
“…Very recently, the 4‐trifluoromethylphenylethylamine iodide (CF 3 PEAI, Figure ) or CF 3 PEAI‐based 2D layered perovskite was used to optimize the performance of PSCs on rigid substrate, exhibiting excellent effects on passivating defects and facilitating hole transfer. [ 22–24 ] Herein, efficient f‐PSCs were constructed via interface engineering of 2D/3D perovskite, i.e., the incorporation of a 2D perovskite (CF 3 PEA) 2 (FA) n −1 Pb n I 3 n +1 on top of the 3D perovskite FA 1− x MA x PbI 3 . The ultra‐thin 2D perovskite upshifted the energy level of 3D perovskite and decreased the energy gap between 3D perovskite and the hole transport layer (HTL) 2,2“,7,7”‐tetrakis‐( N , N ‐di(4‐methoxyphenyl‐amino)‐9,9'‐spirobi‐fluorene (Spiro‐OMeTAD), which facilitated the hole transfer due to the reduced energy barriers and charge extraction losses at the interface.…”
Section: Introductionmentioning
confidence: 99%
“…Figure 3c shows the 1 H, 19 F, and 11 B NMR patterns of the pure BBF and PbI 2 -BBF composite, respectively. All the characteristic 1 H, 19 F, and 11 B peaks of BFF in PbI 2 -BBF composite show an obvious shift to higher δ value in comparison to pure BBF. The shift of 1 H is obvious in the magnified spectra in Fig.…”
Section: Interaction Between Bbf and Pbimentioning
confidence: 91%
“…Meanwhile, the volatile component of MA + cations tends to escape from FAMAPbI 3 perovskite under thermal stress, which results in the formation of undercoordinated Pb 2+ deep-level defects that serving as electron traps [10]. A great many works have been found that these Pb-related defects (e.g., Pb clusters and uncoordinated Pb 2+ ) in FAMAPbI 3 PSCs lead to deterioration of not only the device PCE but also the stability [11]. Meanwhile, in FAMAPbI 3 perovskite, due to the large size of the cations, shallow iodine interstitial and vacancy defects can be generated unintentionally during thermal annealing or device measurement processes, which can lower activation energy barrier for transformation from the α phase to δ phase [12].…”
Section: Introductionmentioning
confidence: 99%
“…Elsewhere, it has been showed that a 3D CsPbI 2 Br phase encapsulated in between layers of 2D Cs 2 PbCl 2 I 2 nano‐sheets is far more stable in ambient conditions than the 3D material alone and the efficiency of such heterostructure can reach up to 16.6 % [25] . The good stability of the 2D phase against humidity and temperature, which can passivate the perovskite surface, increase hydrophobicity, hamper moisture reaction and change the film morphology is also essential for optoelectronic applications [26–28] …”
Section: Introductionmentioning
confidence: 99%