2018
DOI: 10.1016/j.ssc.2018.03.014
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Compressibility of Cs 2 SnBr 6 by X-ray diffraction and Raman spectroscopy

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Cited by 27 publications
(19 citation statements)
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“…Raman spectra further highlighted the observed lattice expansion. As shown in Figure 1j the Raman active mode, ν ( A 1 g ), related to the SnBr symmetric stretching inside [SnBr 6 ] 4− octahedra, [ 22 ] first appeared in the pristine ODASnBr 4 [2%] at 197 cm −1 and then gradually shifted to 191 cm −1 for ODASnBr 4 [2%‐DCM], and to 184 cm −1 for ODASnBr 4 [2%‐CFM]. This indicates that, consequent to the doping process, the [SnBr 6 ] 4− octahedra were under increased tensile strain resulting in longer SnBr bond lengths, and thus a shift to lower resonant frequencies for the Raman active vibrational mode was observed.…”
Section: Resultsmentioning
confidence: 99%
“…Raman spectra further highlighted the observed lattice expansion. As shown in Figure 1j the Raman active mode, ν ( A 1 g ), related to the SnBr symmetric stretching inside [SnBr 6 ] 4− octahedra, [ 22 ] first appeared in the pristine ODASnBr 4 [2%] at 197 cm −1 and then gradually shifted to 191 cm −1 for ODASnBr 4 [2%‐DCM], and to 184 cm −1 for ODASnBr 4 [2%‐CFM]. This indicates that, consequent to the doping process, the [SnBr 6 ] 4− octahedra were under increased tensile strain resulting in longer SnBr bond lengths, and thus a shift to lower resonant frequencies for the Raman active vibrational mode was observed.…”
Section: Resultsmentioning
confidence: 99%
“…According to the characterization data in Figure 2 labeled in orange, the Cs-Sn-Br powders exhibited the well-defined Cs 2 SnBr 6 crystalline structure and regular octahedral morphology. [36] Specifically, compared to Cs 2 SnI 6 , the Cs 2 SnBr 6 crystals showed better high-temperature stability with the decomposition temperature of ≈439 °C. XPS analysis verified the existence of cesium, tin and bromide in the form of Cs + , Sn 4+ , and Br − respectively.…”
Section: Doi: 101002/smll201901650mentioning
confidence: 93%
“…In this work, we also synthesized Cs 2 SnBr 6 powders successfully by replacing the precursors (CsI, SnI 2 , HI solution) with CsBr, SnBr 2 , and HBr solution. According to the characterization data in Figure labeled in orange, the Cs–Sn–Br powders exhibited the well‐defined Cs 2 SnBr 6 crystalline structure and regular octahedral morphology . Specifically, compared to Cs 2 SnI 6 , the Cs 2 SnBr 6 crystals showed better high‐temperature stability with the decomposition temperature of ≈439 °C.…”
mentioning
confidence: 98%
“…[63][64][65][66] It therefore follows that similar electron-phonon coupling processes occur in the vacancy-ordered double perovskites and may even be enhanced by the presence of relatively decoupled octahedral units. 14,67 As the lattice dynamics of vacancy-ordered double perovskites are intimately linked with the A-site cation species and its interaction with the surrounding octahedral framework, the electronphonon coupling behavior in vacancy-ordered double perovskites follows trends predicted by the perovskite tolerance factor. As shown in Figure 9, the trend in experimental carrier mobilities across the A 2 SnI 6 series is reproduced by computationally-derived carrier mobilities calculated within a polaron model, indicating that electron-phonon coupling processes dominate the charge transport behavior in vacancy-ordered double perovskites.…”
Section: Lattice Dynamics and Electron-phonon Couplingmentioning
confidence: 99%