2015
DOI: 10.1002/aelm.201500044
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Origin of High Electronic Quality in Structurally Disordered CH3NH3PbI3 and the Passivation Effect of Cl and O at Grain Boundaries

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Cited by 195 publications
(206 citation statements)
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References 57 publications
(74 reference statements)
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“…The lattice parameters a and c in tetragonal (space group I4/m) are changed, respectively, from 0.892 to 0.886 nm and from 1.261 to 1.251 nm. The apparent optical bandgap can vary by the Cl concentration in MAPbI 3 (Cl), Burstein-Moss effect (carrier concentration), quantum confinement effect, and/or grains and grain boundaries [9, 10, 26, 3537]. The Burstein-Moss and quantum confinement effects are not pertinent to this system considering that the composition of perovskite was confirmed to be the same for all the cases, and the grain size was out of the regime where the quantum confinement effect works in [36, 37].…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The lattice parameters a and c in tetragonal (space group I4/m) are changed, respectively, from 0.892 to 0.886 nm and from 1.261 to 1.251 nm. The apparent optical bandgap can vary by the Cl concentration in MAPbI 3 (Cl), Burstein-Moss effect (carrier concentration), quantum confinement effect, and/or grains and grain boundaries [9, 10, 26, 3537]. The Burstein-Moss and quantum confinement effects are not pertinent to this system considering that the composition of perovskite was confirmed to be the same for all the cases, and the grain size was out of the regime where the quantum confinement effect works in [36, 37].…”
Section: Resultsmentioning
confidence: 99%
“…Generally, defects in grains or grain boundaries act as trap sites for the charge carriers and consequently decrease the charge collection efficiency [36]. Indeed, much effort aimed at the single-crystal perovskites caused successful results for the high photon-to-charge conversion efficiency [710]. Therefore, examining the strategies to control the crystallization for the defect reduction is necessary to achieve better-performing perovskite photovoltaics.…”
Section: Introductionmentioning
confidence: 99%
“…of perovskite films prepared on spectrosil using the PbAc 2 and sol-eng methods and exposed to solar simulator illumination at various oxygen levels for 10 h. The pristine perovskite films prepared by both recipes exhibit a clear onset at 780 nm. [21,23,[50][51][52][53] By fitting the exponential increase in absorption at the band edge an Urbach energy (Eu) can be calculated, representing the degree of energetic disorder within the bulk of the film. At relatively low oxygen levels, the PbAc 2 absorption at 700 nm is reduced by less than 15%, while when the oxygen concentration is higher than 12%, the absorption starts to drop abruptly.…”
Section: Effect Of Degradation On the Optical Properties Of Perovskitmentioning
confidence: 99%
“…Yin et al also suggested that chlorine and oxygen could spontaneously segregate into the grain boundaries and passivate those defect levels and deactivate the trap state. [53] Another way to minimize the negative impact of the grain boundaries was investigated by Son et al [54] They added excessive amounts of CH 3 NH 3 I to the precursor solution, and noted that at 6 mole-% excess, CH 3 NH 3 I layers formed at the perovskite grain boundaries, which helped suppress non-radiative recombination and formed highly conductive ionic pathways that improved electron and hole extraction at the grain. [54] Conductive AFM (c-AFM) was used to investigate the conductive properties at the grain boundaries through local current-voltage measurements, with Figure 4a,b showing a film without excess CH 3 NH 3 I and one with 6 mole-% excess, respectively.…”
Section: Grain Boundaries Passivation and Ion Migrationmentioning
confidence: 99%