2014
DOI: 10.1063/1.4894319
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Effect of structural phase transitions on the exciton absorption spectrum of thin CsPbCl3 films

Abstract: The absorption spectrum of thin film CsPbCl3 in the 2–6 eV range is studied at temperatures of 90–500 K. Sudden changes show up in the temperature dependences of the parameters of the long-wavelength exciton band (spectral position Em(T), half width Γ(T), and oscillator strength f(T)) at the first order phase transitions at 310 and 320. No phase transitions in Em(T), Γ(T), and f(T) are detected at low temperatures. The exciton excitations in CsPbCl3 are found to have a three-dimensional character.

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Cited by 21 publications
(12 citation statements)
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“…Moreover, to the best of our knowledge the deposition of CsPbCl 3 films through dissolution of its precursor salts is not achievable. Different strategies for the synthesis of CsPbCl 3 have been reported in literature: bulk crystals by the Bridgman method [ 12 ]; nanocrystals by high temperature solvent [ 9 ] and similar methods; thin films by evaporation [ 13 , 14 , 15 , 16 , 17 ]. It is worth mentioning that the possibility of realizing large-area compact films of nanometric thickness is relevant for the scalability of innovative devices.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, to the best of our knowledge the deposition of CsPbCl 3 films through dissolution of its precursor salts is not achievable. Different strategies for the synthesis of CsPbCl 3 have been reported in literature: bulk crystals by the Bridgman method [ 12 ]; nanocrystals by high temperature solvent [ 9 ] and similar methods; thin films by evaporation [ 13 , 14 , 15 , 16 , 17 ]. It is worth mentioning that the possibility of realizing large-area compact films of nanometric thickness is relevant for the scalability of innovative devices.…”
Section: Introductionmentioning
confidence: 99%
“…The excitonic peak firstly shows a fast redshift trend until 320 K, followed by a slower redshift trend below 320 K. This phenomenon is attributed to a phase transition from cubic phase to tetragonal phase which occurs at around 320 K during the cooling process. The excitonic peak position is well fitted by using the Varshni equation with α1= 3.382 × 10 -4 eV/K for the cubic phase and α2= 2.376 × 10 -5 eV/K for the tetragonal phase, which is in good agreement with previous reports (77).…”
Section: Temperature-dependent Optical Absorption Spectroscopy Is Consupporting
confidence: 91%
“…For example, CsPbBr3 perovskite possesses a cubic structure at a temperature above 130°C, a tetragonal structure at a temperature between 88-130 °C and an orthorhombic structure at a temperature below 88 °C (76). CsPbCl3 perovskite exhibits the cubic structure at a temperature above 30 °C while it changes into a tetragonal phase at a temperature below 30 °C(76,77).…”
mentioning
confidence: 99%
“…Although the mixing phenomena of CsPbBr 3 and CsPbCl 3 has been reported by several groups, some of which have even fabricated perovskite LED devices taking advantage of the adjustable bandgap through mixing, the influence of mixing on both particle and film morphology has not yet been well studied. Perovskite materials are known for their structural sensitivity to external conditions, where phase transitions, structural distortion, and even degradation may occur . Therefore, it is reasonable to investigate the possible effects induced by mixing of CsPbBr 3 and CsPbCl 3 perovskite materials, especially in terms of their influence on film morphology, which essentially determines the performance of LED devices.…”
mentioning
confidence: 99%