Ae<sub>3</sub>[TO<sub>3</sub>][SnOQ<sub>3</sub>] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se) and Ba<sub>3</sub>[CO<sub>3</sub>][MQ<sub>4</sub>] (M = Ge, Sn; Q = S, Se): Design and Syntheses of a Series of Heteroanionic Antiperovskite-Type Oxychalcogenides

The heteroanionic materials (HAMs) have attracted more and more attention because they can better balance the functional properties of materials. However, their rational structural design is still a great challenge. Here, by using the antiperovskite Ba<sub>3</sub>S[GeS<sub>4</sub>] as a template and calculating the tolerance factor (<i>t</i>) as a reference, eight heteroanionic oxychalcogenides with balanced properties were finally synthesized by a partially group-substitution method. Among them, Ba<sub>3</sub>[CO<sub>3</sub>][MQ<sub>4</sub>] (M = Ge, Sn; Q = S, Se) are centrosymmetric (CS) crystals and realize optimization of band gaps and birefringence. For Ae<sub>3</sub>[TO<sub>3</sub>][SnOQ<sub>3</sub>] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se), thanks to the novel [TO<sub>4</sub>SnQ<sub>3</sub>] polyanionic groups for the regulation to the antiperovskite structures and the contributions to the nonlinear optical (NLO) properties, they achieve the structural transition from CS to noncentrosymmetry and accomplish an excellent balance among the critical performance parameters as the potential candidates for the infrared NLO materials, including phase-matchable behavior, wide band gaps (<i>E</i><sub>g</sub> = 3.26-3.95 eV), high laser damage threshold (LDT = 3.2-4.4 × AgGaS<sub>2</sub>), suitable birefringence (Δ<i>n</i> = 0.065-0.098@2090 nm) and sufficiently strong second-harmonic generation responses (about 0.6-0.9 × AgGaS<sub>2</sub>). Moreover, benefiting from crystallization in the polar space groups, they exhibit ferroelectricity and piezoelectricity at room temperature. As far as we know, this is the first reported fully inorganic antiperovskite ferroelectric. These demonstrate that our strategy is desirable and can provide some unique insights into the development of HAMs or antiperovskite materials with specific functions or structures.

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Publication Details

Journal
Journal of the American Chemical Society
Published
2024-09-16
DOI
https://doi.org/10.1021/jacs.4c06381
Citations
17
Primary Topic
Crystal Structures and Properties
Type
article
Field-Weighted Citation Impact
2.00

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Ae3[TO3][SnOQ3] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se) and Ba3[CO3][MQ4] (M = Ge, Sn; Q = S, Se): Design and Syntheses of a Series of Heteroanionic Antiperovskite-Type Oxychalcogenides

Zhanggui Hu, Hongping Wu, Hongwei Yu, Yicheng Wu et al.
17 citations
Journal of the American Chemical Society
Crystal Structures and Properties
2.00
article

Ae3[TO3][SnOQ3] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se) and Ba3[CO3][MQ4] (M = Ge, Sn; Q = S, Se): Design and Syntheses of a Series of Heteroanionic Antiperovskite-Type Oxychalcogenides

Zhanggui Hu, Hongping Wu, Hongwei Yu, Yicheng Wu, Jiyang Wang, Yuanding Yu, Shiyi Zhang
article en
17 citations

Abstract

The heteroanionic materials (HAMs) have attracted more and more attention because they can better balance the functional properties of materials. However, their rational structural design is still a great challenge. Here, by using the antiperovskite Ba<sub>3</sub>S[GeS<sub>4</sub>] as a template and calculating the tolerance factor (<i>t</i>) as a reference, eight heteroanionic oxychalcogenides with balanced properties were finally synthesized by a partially group-substitution method. Among them, Ba<sub>3</sub>[CO<sub>3</sub>][MQ<sub>4</sub>] (M = Ge, Sn; Q = S, Se) are centrosymmetric (CS) crystals and realize optimization of band gaps and birefringence. For Ae<sub>3</sub>[TO<sub>3</sub>][SnOQ<sub>3</sub>] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se), thanks to the novel [TO<sub>4</sub>SnQ<sub>3</sub>] polyanionic groups for the regulation to the antiperovskite structures and the contributions to the nonlinear optical (NLO) properties, they achieve the structural transition from CS to noncentrosymmetry and accomplish an excellent balance among the critical performance parameters as the potential candidates for the infrared NLO materials, including phase-matchable behavior, wide band gaps (<i>E</i><sub>g</sub> = 3.26-3.95 eV), high laser damage threshold (LDT = 3.2-4.4 × AgGaS<sub>2</sub>), suitable birefringence (Δ<i>n</i> = 0.065-0.098@2090 nm) and sufficiently strong second-harmonic generation responses (about 0.6-0.9 × AgGaS<sub>2</sub>). Moreover, benefiting from crystallization in the polar space groups, they exhibit ferroelectricity and piezoelectricity at room temperature. As far as we know, this is the first reported fully inorganic antiperovskite ferroelectric. These demonstrate that our strategy is desirable and can provide some unique insights into the development of HAMs or antiperovskite materials with specific functions or structures.

Journal of the American Chemical SocietyVol. 146(38)
Tianjin University of Technology (CN)
National Natural Science Foundation of China, Natural Science Foundation of Tianjin City
Sustainable cities and communities
Openalex Percentile: Top 13%
Crystal Structures and Properties
2.00
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