2017
DOI: 10.1021/acs.inorgchem.7b01863
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Lead-Free Hybrid Material with an Exceptional Dielectric Phase Transition Induced by a Chair-to-Boat Conformation Change of the Organic Cation

Abstract: Hybrid organic-inorganic perovskite materials have demonstrated great potential in the field of photovoltaics and photoelectronics. On the basis of the high degree of structural flexibility and compatibility, diverse molecular functional materials have been assembled by modifying the length of the organic components and/or dimensionality of the inorganic frameworks. In this paper, we present a chiral lead-free organic-inorganic hybrid, (piperidinium)SbCl (1), which follows the one-dimensional inorganic framewo… Show more

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Cited by 35 publications
(12 citation statements)
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References 77 publications
(88 reference statements)
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“…As shown in the band structures diagram (Figure 2 b), the bottom of conduction band locates at the S point, while the topmost of valence band is at the G point, revealing its indirect band gap feature. [17] The value of band gap from band structure calculation is about 2.35 eV, in accordance with our experiment value. From the partial density of states (PDOS), we can assert AgBr 6 and BiBr 6 octahedra dominate the optical band gap of 1, since the orbital states near the Fermi level mainly derive from the inorganic octahedra (Supporting Information, Figure S5).…”
supporting
confidence: 89%
“…As shown in the band structures diagram (Figure 2 b), the bottom of conduction band locates at the S point, while the topmost of valence band is at the G point, revealing its indirect band gap feature. [17] The value of band gap from band structure calculation is about 2.35 eV, in accordance with our experiment value. From the partial density of states (PDOS), we can assert AgBr 6 and BiBr 6 octahedra dominate the optical band gap of 1, since the orbital states near the Fermi level mainly derive from the inorganic octahedra (Supporting Information, Figure S5).…”
supporting
confidence: 89%
“…The relatively large thermal hysteresis discloses the first-order feature for the phase transitions. In addition, the number of the possible molecular orientations ( N ) can be estimated to be 2.05 from the Boltzmann formula Δ S = nR ln N (where n is the number of guest molecules per mole and R is the gas constant), which reveals the typical order–disorder phase transition ( N = 2) . In addition, the variable-temperature PXRD measurements also verify the occurrence of its successive phase transitions, as shown in Figure S4.…”
Section: Resultsmentioning
confidence: 88%
“…Based on the DSC curves, the associated entropy change Δ S was estimated with a value of 2.74 J/mol K for the phase transition at 284 K. According to the Boltzmann equation Δ S = R ln ( N 1/ N 2), in which R denotes the gas constant 8.314 and N 1 and N 2 are the numbers of independent directions of motion in the HTP and LTP. During cooling, the result showed that N = 1.39, manifesting a more complicated phase transition rather than the order‐disorder mechanism ( N = 2), the structural analysis will further confirmed it.…”
Section: Resultsmentioning
confidence: 69%