2020
DOI: 10.1039/d0ra07668f
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The thermal stability of FAPbBr3nanocrystals from temperature-dependent photoluminescence and first-principles calculations

Abstract: The thermal properties of FAPbBr3 perovskite nanocrystals (PNCs) is investigated by use of temperature-dependent steady-state/time-resolved photoluminescence and first-principle calculations.

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Cited by 17 publications
(9 citation statements)
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“…According to previous reports, , the structural phase transition from orthorhombic to tetragonal should be accounted for this red-shift in FAPbBr 3 PeNCs. Moreover, theoretical calculations show that the tetragonal phase has a smaller band gap than the orthorhombic phase, which also supports this observation. It is noted that the phase transition temperature is lower than that in previous research works, , which may be due to the smaller size of the PeNCs. , The blue-shift of emission with temperature from 140 to 295 K can be described by the temperature coefficient α = ∂ E g /∂ T = 0.359 meV/K.…”
Section: Resultssupporting
confidence: 67%
“…According to previous reports, , the structural phase transition from orthorhombic to tetragonal should be accounted for this red-shift in FAPbBr 3 PeNCs. Moreover, theoretical calculations show that the tetragonal phase has a smaller band gap than the orthorhombic phase, which also supports this observation. It is noted that the phase transition temperature is lower than that in previous research works, , which may be due to the smaller size of the PeNCs. , The blue-shift of emission with temperature from 140 to 295 K can be described by the temperature coefficient α = ∂ E g /∂ T = 0.359 meV/K.…”
Section: Resultssupporting
confidence: 67%
“…Despite several efforts, the accurate description of the band gap of halide perovskites with a single formulation of the exchange–correlation functional in DFT is challenging and often results in relatively large errors. For this reason, it is common practice to study each perovskite with an ad hoc DFT hybrid functional specifically designed to reproduce the band gap of that specific perovskite. Needless to say that this introduces a certain level of empiricism and severely limits the possibility to predict in a reliable way the properties and the band gap of an unknown perovskite, in the attempt to improve the results, it is common practice to include spin–orbit coupling (SOC) effects in the calculations . However, we will show below that this is not always useful and it may result in worsening the agreement with the experiment.…”
Section: Introductionmentioning
confidence: 99%
“…It is well established that organic–inorganic LHP NCs are less stable than all-inorganic LHP NCs at elevated temperatures due to structural phase transition. , Temperature has a great influence on FAPbBr 3 NCs. With the increase of temperature up to 400 K, FAPbBr 3 NCs were easy to change from cubic phase to tetragonal phase . Here, we show that introducing Cs + into organic–inorganic LHP NCs can solve this issue, probably due to the spherical coordination behavior of Cs + compared with asymmetrical FA + cations for the formation of a high-symmetry cubic perovskite structure.…”
Section: Resultsmentioning
confidence: 82%
“…With the increase of temperature up to 400 K, FAPbBr 3 NCs were easy to change from cubic phase to tetragonal phase. 67 Here, we show that introducing Cs + into organic−inorganic LHP NCs can solve this issue, probably due to the spherical coordination behavior of Cs + compared with asymmetrical FA + cations for the formation of a high-symmetry cubic perovskite structure. The 4a), and the PL peak widened and multiple emission peaks appeared, which was an indication of phase transformation and was consistent with previous reports.…”
Section: Resultsmentioning
confidence: 93%