JOURNAL ARTICLE

Structural\nTransition in (C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>3</sub>Bi<sub>2–<i>x</i></sub>Sb<sub><i>x</i></sub>I<sub>9</sub>:[(Bi/Sb)<sub>2</sub>I<sub>9</sub>]<sup>3–</sup> Dimers to [(Bi/Sb)<sub>3</sub>I<sub>12</sub>]<sup>3–</sup> Trimers to (∞<sup><b>1</b></sup>)[(Bi/Sb)<sub>2</sub>I<sub>9</sub><sup>3–</sup>] 1D Infinite Chains

Abinash Pradhan (8764119)Saroj L. Samal (2179826)

Year: 2023 Journal:   OPAL (Open@LaTrobe) (La Trobe University)   Publisher: La Trobe University

Abstract

Antimony/bismuth-based lead-free hybrid halide defect\n2D perovskites\nhave been generating enormous research interest due to their inherent\nexcellent optical properties. Exploration of new phases and understanding\nof their structural and optoelectronic properties are of paramount\nimportance in the process of developing materials for practical solar\ncell applications. In this article, we have reported a structural\ntransition from the 0D hexagonal phase containing isolated [M<sub>2</sub>I<sub>9</sub>]<sup>3–</sup> (M = Bi/Sb) units to the\n1D orthorhombic phase via a new monoclinic phase with novel isolated\ntrimeric [M<sub>3</sub>I<sub>12</sub>]<sup>3–</sup> units in\n(C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>3</sub>Bi<sub>2–2<i>x</i></sub>Sb<sub>2<i>x</i></sub>I<sub>9</sub>. The\nhexagonal phase is stable up to 2<i>x</i> = 0.6 in (C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>3</sub>Bi<sub>2–2<i>x</i></sub>Sb<sub>2<i>x</i></sub>I<sub>9</sub>. With\ngradual substitution of Sb, the cation–cation repulsion increases,\nwhich destabilizes the [M<sub>2</sub>I<sub>9</sub>]<sup>3–</sup> unit, and hence, the hexagonal phase becomes unstable. At intermediate\ncomposition, 2<i>x</i> = 0.8–1.6, a new monoclinic\nphase (S.G.: <i>C</i>2/<i>m</i>) with the composition\n(C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>2</sub>Bi<sub>2–2<i>x</i></sub>Sb<sub>2<i>x</i></sub>I<sub>8</sub> is\nformed, containing isolated [M<sub>3</sub>I<sub>12</sub>]<sup>3–</sup> units. The symmetry reduction resulted in larger distortion, which\nrelaxes the strain and stabilizes the trimeric unit in the intermediate\ncompositions. Finally, at higher Sb compositions (2<i>x</i> = 1.9–2.0), the compounds crystallize in the orthorhombic\n1D phase. In all three phases of (C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>3</sub>Bi<sub>2–2<i>x</i></sub>Sb<sub>2<i>x</i></sub>I<sub>9</sub>, the cationic ethylammonium\nunits are completely disordered over the whole unit cell. Raman study\nclearly shows the phase transition in (C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>3</sub>Bi<sub>2–2<i>x</i></sub>Sb<sub>2<i>x</i></sub>I<sub>9</sub> and also the structural distortion\nin (C<sub>2</sub>H<sub>5</sub>NH<sub>3</sub>)<sub>2</sub>Bi<sub>2–2<i>x</i></sub>Sb<sub>2<i>x</i></sub>I<sub>8</sub>. Optical\nproperty study shows that all the compounds are of indirect band gap\ntype. Furthermore, PL study shows better emission properties of the\n1D orthorhombic Sb compounds as compared to the 0D hexagonal and monoclinic\nphases.

Keywords:
Orthorhombic crystal system Monoclinic crystal system Phase (matter) Hexagonal crystal system Hexagonal phase Raman spectroscopy Phase transition Halide Cationic polymerization

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Topics

Perovskite Materials and Applications
Physical Sciences →  Engineering →  Electrical and Electronic Engineering
Inorganic Fluorides and Related Compounds
Physical Sciences →  Chemistry →  Inorganic Chemistry
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Physical Sciences →  Materials Science →  Materials Chemistry

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