2021
DOI: 10.3390/molecules26195737
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Exploring the Effect of Ammonium Iodide Salts Employed in Multication Perovskite Solar Cells with a Carbon Electrode

Abstract: Perovskite solar cells that use carbon (C) as a replacement of the typical metal electrodes, which are most commonly employed, have received growing interest over the past years, owing to their low cost, ease of fabrication and high stability under ambient conditions. Even though Power Conversion Efficiencies (PCEs) have increased over the years, there is still room for improvement, in order to compete with metal-based devices, which exceed 25% efficiency. With the scope of increasing the PCE of Carbon based P… Show more

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Cited by 9 publications
(6 citation statements)
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“…All the Oct(A) n−1 Pb n I 3n+1 (where A = FA, Cs 0.12 FA 0.88 and A = Cs 0.1 MA 0.15 FA 0.75 ) films exhibit the APbI 3 perovskite cubic phase peaks corresponding to the (001), (011), (111), (002), (012), (022), and (003) diffraction planes, respectively [ 87 ]. However, virtually all Oct(A) n−1 Pb n I 3n+1 films reveal the additional peak at 7.6°, which can be attributed to the formation of 2D perovskite phase coexisting with the 3D perovskite phase [ 88 , 89 ]. The emergence of additional peaks at around 2θ = 12° and 26.5° for the material formulations with A = FA and Cs 0.12 FA 0.88 is attributed to the formation of quasi-3D perovskites Oct(A) n−1 Pb n I 3n+1 (where n > 10) [ 90 , 91 , 92 ].…”
Section: Resultsmentioning
confidence: 99%
“…All the Oct(A) n−1 Pb n I 3n+1 (where A = FA, Cs 0.12 FA 0.88 and A = Cs 0.1 MA 0.15 FA 0.75 ) films exhibit the APbI 3 perovskite cubic phase peaks corresponding to the (001), (011), (111), (002), (012), (022), and (003) diffraction planes, respectively [ 87 ]. However, virtually all Oct(A) n−1 Pb n I 3n+1 films reveal the additional peak at 7.6°, which can be attributed to the formation of 2D perovskite phase coexisting with the 3D perovskite phase [ 88 , 89 ]. The emergence of additional peaks at around 2θ = 12° and 26.5° for the material formulations with A = FA and Cs 0.12 FA 0.88 is attributed to the formation of quasi-3D perovskites Oct(A) n−1 Pb n I 3n+1 (where n > 10) [ 90 , 91 , 92 ].…”
Section: Resultsmentioning
confidence: 99%
“…[10,16,[25][26][27] This perovskite is also known to develop a better contact surface with TiO 2 with a lower defect concentration. [28][29][30][31] However, the combination of the AVAI additive and the HTL-free device configuration, along with a thick zirconia buffer layer, can leads to a strong hysteresis behavior together with a "bump" patterned observed in the reverse J-V scan. [8,[32][33][34] To address this issue, different strategies have been scouted in literature to enhance charge extraction and transfer.…”
Section: Introductionmentioning
confidence: 99%
“…This PK is also known to develop a better contact surface with TiO 2 with a lower defect concentration. [21][22][23][24] The introduction of this AVAI additive coupled to the HTM-free device configuration having a thick zirconia buffer layer however seems to induce a large hysteresis behavior as well as the appearance of a "bump" in the reverse J-V scan. [9,[25][26][27] To address this problem, different strategies have been used in literature such as the addition of CuSCN, [27,28] a well-known inorganic hole transport material, to the PK solution allowing to form of a bulk heterojunction.…”
Section: Introductionmentioning
confidence: 99%