Vacancy Ordered Double Perovskites [N(CH <sub>3</sub> ) <sub>4</sub> ] <sub>2</sub> SnX <sub>6</sub> (X=Cl, Br, I): Thermal Phase Transition and Wide Range Optical Absorption

(TMA)<sub>2</sub>SnX<sub>6</sub> (TMA=tetramethylammonium; X=Cl, Br, I) compounds form vacancy-ordered halide double perovskites (VODPs) with TMA<sup>+</sup> cation in the A-site, Sn<sup>4+</sup> cation in the M-site and X<sup>-</sup> anion in the halide site. This study reports the synthesis and the structural phase transition of (TMA)₂SnCl₆, (TMA)<sub>2</sub>SnCl<sub>0.7</sub>Br<sub>5.3</sub>, (TMA)₂SnBr₆, and (TMA)₂SnI₆. All four halides crystallize in a cubic Fd <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mover><mml:mn>3</mml:mn> <mml:mo>‾</mml:mo></mml:mover> <mml:annotation>${\bar{3}}$</mml:annotation> </mml:semantics> </mml:math> c symmetry at room temperature. At elevated temperatures, (TMA)<sub>2</sub>SnCl<sub>6</sub> and (TMA)<sub>2</sub>SnBr<sub>6</sub> show phase transition to a cubic Fm <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mover><mml:mn>3</mml:mn> <mml:mo>‾</mml:mo></mml:mover> <mml:annotation>${\bar{3}}$</mml:annotation> </mml:semantics> </mml:math> m symmetry at 364 K and 369 K, respectively. While the phase transition of (TMA)<sub>2</sub>SnCl<sub>6</sub> was reported earlier, that of (TMA)<sub>2</sub>SnBr<sub>6</sub> is reported for the first time in this study. The synthesis and structures of (TMA)<sub>2</sub>SnCl<sub>0.7</sub>Br<sub>5.3</sub> and (TMA)<sub>2</sub>SnI<sub>6</sub> are reported for the first time in this study, with calorimetry data showing a reversible transition at 363 K and 325 K, respectively. Further, the choice of halide ligand influences the bandgap and the colour of the compounds. The absorption edge lies at 3.60 eV for (TMA)<sub>2</sub>SnCl<sub>6</sub>, at 2.64 eV for (TMA)<sub>2</sub>SnBr<sub>6</sub>, and at 1.12 eV for (TMA)<sub>2</sub>SnI<sub>6</sub>. Such a wide tunability of bandgap across the ultraviolet to infrared regions in combination with the thermal phase change makes these perovskites interesting materials for thermal and solar energy storage applications.

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Journal
Chemistry - An Asian Journal
Published
2025-03-11
DOI
https://doi.org/10.1002/asia.202401483
Citations
3
Primary Topic
Perovskite Materials and Applications
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article
Field-Weighted Citation Impact
2.19
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article

Vacancy Ordered Double Perovskites [N(CH 3 ) 4 ] 2 SnX 6 (X=Cl, Br, I): Thermal Phase Transition and Wide Range Optical Absorption

Pratap Vishnoi, Nagale S. Vishwajith, Digvijay Singh, A. Arun Prasad
3 citations
Chemistry - An Asian Journal
Perovskite Materials and Applications
2.19
article

Vacancy Ordered Double Perovskites [N(CH 3 ) 4 ] 2 SnX 6 (X=Cl, Br, I): Thermal Phase Transition and Wide Range Optical Absorption

Pratap Vishnoi, Nagale S. Vishwajith, Digvijay Singh, A. Arun Prasad
article en
3 citations

Abstract

(TMA)<sub>2</sub>SnX<sub>6</sub> (TMA=tetramethylammonium; X=Cl, Br, I) compounds form vacancy-ordered halide double perovskites (VODPs) with TMA<sup>+</sup> cation in the A-site, Sn<sup>4+</sup> cation in the M-site and X<sup>-</sup> anion in the halide site. This study reports the synthesis and the structural phase transition of (TMA)₂SnCl₆, (TMA)<sub>2</sub>SnCl<sub>0.7</sub>Br<sub>5.3</sub>, (TMA)₂SnBr₆, and (TMA)₂SnI₆. All four halides crystallize in a cubic Fd <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mover><mml:mn>3</mml:mn> <mml:mo>‾</mml:mo></mml:mover> <mml:annotation>${\bar{3}}$</mml:annotation> </mml:semantics> </mml:math> c symmetry at room temperature. At elevated temperatures, (TMA)<sub>2</sub>SnCl<sub>6</sub> and (TMA)<sub>2</sub>SnBr<sub>6</sub> show phase transition to a cubic Fm <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mover><mml:mn>3</mml:mn> <mml:mo>‾</mml:mo></mml:mover> <mml:annotation>${\bar{3}}$</mml:annotation> </mml:semantics> </mml:math> m symmetry at 364 K and 369 K, respectively. While the phase transition of (TMA)<sub>2</sub>SnCl<sub>6</sub> was reported earlier, that of (TMA)<sub>2</sub>SnBr<sub>6</sub> is reported for the first time in this study. The synthesis and structures of (TMA)<sub>2</sub>SnCl<sub>0.7</sub>Br<sub>5.3</sub> and (TMA)<sub>2</sub>SnI<sub>6</sub> are reported for the first time in this study, with calorimetry data showing a reversible transition at 363 K and 325 K, respectively. Further, the choice of halide ligand influences the bandgap and the colour of the compounds. The absorption edge lies at 3.60 eV for (TMA)<sub>2</sub>SnCl<sub>6</sub>, at 2.64 eV for (TMA)<sub>2</sub>SnBr<sub>6</sub>, and at 1.12 eV for (TMA)<sub>2</sub>SnI<sub>6</sub>. Such a wide tunability of bandgap across the ultraviolet to infrared regions in combination with the thermal phase change makes these perovskites interesting materials for thermal and solar energy storage applications.

Chemistry - An Asian JournalVol. 20(8)
Jawaharlal Nehru Centre for Advanced Scientific Research (IN), Indian Institute of Science Bangalore (IN), Dr. Hari Singh Gour University (IN)
Affordable and clean energy
Openalex Percentile: Top 13%
Perovskite Materials and Applications
2.19
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