Fundamental Properties of Low-Dimensional Perovskite-Related Light Absorbers: [(CH <sub>2</sub> ) <sub>3</sub> NH <sub>2</sub> ] <sub>3</sub> Sb <sub>2</sub> X <sub>9</sub> (X = I, Br, Cl), Azetidinium Antimony Halides

Over the past decade, many Sb-based organohalides have been synthesized and analyzed due to their intriguing optical and electronic properties. They form low-dimensional (0D, 1D, and 2D) metal halide frameworks due to the 3+ oxidation state of antimony (Sb<sup>3+</sup>). The low-dimensional perovskite derivatives commonly have good moisture stability which makes them attractive for replacing the lead-containing halide perovskites. We focus on the A<sub>3</sub>Sb<sub>2</sub>X<sub>9</sub> compositions since the band gap tunability of the compounds is noteworthy. Cs<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> is known to form both 0D and 2D octahedral networks at room temperature. The A-site in A<sub>3</sub>Sb<sub>2</sub>X<sub>9</sub> is crucial in determining the configuration of the metal halide framework. Within the hybrid A<sub>3</sub>Sb<sub>2</sub>X<sub>9</sub> systems, the azetidinium cation (Az<sup>+</sup>, [(CH<sub>2</sub>)<sub>3</sub>NH<sub>2</sub>]<sup>+</sup>) has rarely been studied as a potential A-site candidate. We confirm that the polycrystalline powders and thin films of (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> exhibit a 0D dimer structure, while (Az)<sub>3</sub>Sb<sub>2</sub>Br<sub>9</sub> and (Az)<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub> adopt a 2D corrugated layer structure at the molecular level. (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> and (Az)<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub> exhibit phase transitions at low temperatures, as shown by differential scanning calorimetry. Thin films grow with a strongly preferred (00<i>l</i>) orientation perpendicular to glass substrates. The Tauc plot analysis from diffuse reflectance spectra exhibits a band edge at 2.11 eV in (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub>, at 2.63 eV in (Az)<sub>3</sub>Sb<sub>2</sub>Br<sub>9</sub>, and at 3.26 eV in (Az)<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub>. A weak excitonic band is identified in the absorption spectrum of the (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> thin film. Interestingly, there is a severe morphological difference in the thin films, depending on the solvent used, resulting in a band edge shift. The temperature dependence of the (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> thin-film XRD data indicates the existence of an intermediate phase.

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Journal
ACS Omega
Published
2025-12-24
DOI
https://doi.org/10.1021/acsomega.5c08306
Primary Topic
Perovskite Materials and Applications
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article

Fundamental Properties of Low-Dimensional Perovskite-Related Light Absorbers: [(CH 2 ) 3 NH 2 ] 3 Sb 2 X 9 (X = I, Br, Cl), Azetidinium Antimony Halides

L. Leander Schaberg, Doru C. Lupascu, M. Escobar-Castillo, B. Marler et al.
ACS Omega
Perovskite Materials and Applications
article

Fundamental Properties of Low-Dimensional Perovskite-Related Light Absorbers: [(CH 2 ) 3 NH 2 ] 3 Sb 2 X 9 (X = I, Br, Cl), Azetidinium Antimony Halides

L. Leander Schaberg, Doru C. Lupascu, M. Escobar-Castillo, B. Marler, Young Jin, Erik Elkaïm, Andrei N. Salak, Niels Benson
article en

Abstract

Over the past decade, many Sb-based organohalides have been synthesized and analyzed due to their intriguing optical and electronic properties. They form low-dimensional (0D, 1D, and 2D) metal halide frameworks due to the 3+ oxidation state of antimony (Sb<sup>3+</sup>). The low-dimensional perovskite derivatives commonly have good moisture stability which makes them attractive for replacing the lead-containing halide perovskites. We focus on the A<sub>3</sub>Sb<sub>2</sub>X<sub>9</sub> compositions since the band gap tunability of the compounds is noteworthy. Cs<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> is known to form both 0D and 2D octahedral networks at room temperature. The A-site in A<sub>3</sub>Sb<sub>2</sub>X<sub>9</sub> is crucial in determining the configuration of the metal halide framework. Within the hybrid A<sub>3</sub>Sb<sub>2</sub>X<sub>9</sub> systems, the azetidinium cation (Az<sup>+</sup>, [(CH<sub>2</sub>)<sub>3</sub>NH<sub>2</sub>]<sup>+</sup>) has rarely been studied as a potential A-site candidate. We confirm that the polycrystalline powders and thin films of (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> exhibit a 0D dimer structure, while (Az)<sub>3</sub>Sb<sub>2</sub>Br<sub>9</sub> and (Az)<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub> adopt a 2D corrugated layer structure at the molecular level. (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> and (Az)<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub> exhibit phase transitions at low temperatures, as shown by differential scanning calorimetry. Thin films grow with a strongly preferred (00<i>l</i>) orientation perpendicular to glass substrates. The Tauc plot analysis from diffuse reflectance spectra exhibits a band edge at 2.11 eV in (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub>, at 2.63 eV in (Az)<sub>3</sub>Sb<sub>2</sub>Br<sub>9</sub>, and at 3.26 eV in (Az)<sub>3</sub>Sb<sub>2</sub>Cl<sub>9</sub>. A weak excitonic band is identified in the absorption spectrum of the (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> thin film. Interestingly, there is a severe morphological difference in the thin films, depending on the solvent used, resulting in a band edge shift. The temperature dependence of the (Az)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> thin-film XRD data indicates the existence of an intermediate phase.

ACS OmegaVol. 11(1)
Synchrotron soleil (FR), Czech Academy of Sciences, Institute of Geology (CZ), University of Aveiro (PT), University of Duisburg-Essen (DE), Ruhr University Bochum (DE)
Openalex Percentile: Top 42%
Perovskite Materials and Applications
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