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Rb<sub>3</sub>InCl<sub>6</sub>: A Monoclinic Double Perovskite Derivative with Bright Sb<sup>3+</sup>-Activated Photoluminescence
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50
References
2020
Year
Here, we present the synthesis and crystal structure of Rb<sub>3</sub>InCl<sub>6</sub> prepared from air stable reagents via a two-step process that proceeds through the intermediate Rb<sub>2</sub>InCl<sub>5</sub>·H<sub>2</sub>O. Rb<sub>3</sub>InCl<sub>6</sub> crystallizes with the Rb<sub>3</sub>YCl<sub>6</sub> structure type (<i>C</i>2/<i>c</i>), which can be derived from the double perovskite structure by noncooperative tilting of isolated [InCl<sub>6</sub>]<sup>3-</sup> octahedra. Despite this lowering of symmetry, the optical properties are similar to the cubic double perovskite Cs<sub>2</sub>NaInCl<sub>6</sub>. Partial substitution of In<sup>3+</sup> with Sb<sup>3+</sup> in Rb<sub>3</sub>InCl<sub>6</sub> results in intense cyan-green photoluminescence originating from localized 5s<sup>2</sup> to 5s<sup>1</sup>5p<sup>1</sup> electronic transitions of [SbCl<sub>6</sub>]<sup>3-</sup> polyatomic anions. In comparison with the cubic double perovskite phosphor Cs<sub>2</sub>NaInCl<sub>6</sub>:Sb<sup>3+</sup>, the octahedral tilting distortion increases the electronic isolation of the In/Sb-centered octahedra thus facilitating electron and hole localization on Sb<sup>3+</sup> sites, leading to bright photoluminescence. The distorted crystal structure also leads to a larger Stokes shift (1.29 eV) and a corresponding red shift of the emission peak (λ<sub>max</sub> = 522 nm) compared to the more symmetric Cs<sub>2</sub>NaInCl<sub>6</sub>:Sb<sup>3+</sup> (Stokes shift ≈ 0.94 eV, λ<sub>max</sub> = 445 nm).
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