Two ternary chalcostannates Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> (<i>Q</i> = S and Se): syntheses, crystal structures, and photovoltaic studies

Semiconducting Sn-containing chalcogenides are promising for their photovoltaic properties. Herein, we report the syntheses of two barium tin chalcogenides, Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> (<i>Q</i> = S and Se), by high-temperature reactions of elements. A single-crystal X-ray diffraction study shows that the Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure crystallizes in the monoclinic system (space group: <i>P</i>2<sub>1</sub>/<i>c</i>) with four formula units (<i>Z</i> = 4). The refined lattice constants of the Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure are <i>a</i> = 11.4599(3) Å, <i>b</i> = 6.9268(2) Å, <i>c</i> = 19.6066(6) Å, and <i>β</i> = 101.197(1)°. The Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure is pseudo-zero-dimensional, similar to that of the Ba<sub>3</sub>Sn<sub>2</sub>S<sub>7</sub> structure. However, in contrast to the sulfide counterpart, the Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure features one split barium site (Ba1 and Ba2) arising from positional disorder. All atoms of the Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> structures occupy the general positions. The main building blocks of the Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> structures are the isolated anionic [Sn<sub>2</sub><i>Q</i><sub>7</sub>]<sup>6-</sup> motifs, which are separated and charge-balanced by the filling of Ba<sup>2+</sup> cations. Optical bandgap studies of polycrystalline Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> samples confirm their semiconducting nature with the direct bandgap values of 2.3(1) eV (<i>Q</i> = S) and 1.9(1) eV (<i>Q</i> = Se). DFT studies also predict the semiconducting nature of the title phases, and the theoretical band gaps are in good agreement with the optical absorption studies. Photovoltaic characterization of the polycrystalline Ba<sub>3</sub>Sn<sub>2</sub>S<sub>7</sub> sample reveals a 23.7% increase in power conversion efficiency, attributed to a reduced electron-hole recombination rate. Moreover, the theoretical electronic structures of the title chalcogenides are presented along with the COHPs results, highlighting the relative strengths of chemical bonds and charge transfer between the metals (Ba and Sn) and chalcogen (S/Se) atoms.

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Journal
Dalton Transactions
Published
2025-01-01
DOI
https://doi.org/10.1039/d5dt01399b
Citations
1
Primary Topic
Crystal Structures and Properties
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article
Field-Weighted Citation Impact
0.43

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article

Two ternary chalcostannates Ba3Sn2Q7 (Q = S and Se): syntheses, crystal structures, and photovoltaic studies

Sayani Barman, Sweta Yadav, Ramesh Mamindla, Melepurath Deepa et al.
1 citations
Dalton Transactions
Crystal Structures and Properties
0.43
article

Two ternary chalcostannates Ba3Sn2Q7 (Q = S and Se): syntheses, crystal structures, and photovoltaic studies

Sayani Barman, Sweta Yadav, Ramesh Mamindla, Melepurath Deepa, Swati, Akshay Kumar Ray, Jai Prakash
article en
1 citations

Abstract

Semiconducting Sn-containing chalcogenides are promising for their photovoltaic properties. Herein, we report the syntheses of two barium tin chalcogenides, Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> (<i>Q</i> = S and Se), by high-temperature reactions of elements. A single-crystal X-ray diffraction study shows that the Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure crystallizes in the monoclinic system (space group: <i>P</i>2<sub>1</sub>/<i>c</i>) with four formula units (<i>Z</i> = 4). The refined lattice constants of the Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure are <i>a</i> = 11.4599(3) Å, <i>b</i> = 6.9268(2) Å, <i>c</i> = 19.6066(6) Å, and <i>β</i> = 101.197(1)°. The Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure is pseudo-zero-dimensional, similar to that of the Ba<sub>3</sub>Sn<sub>2</sub>S<sub>7</sub> structure. However, in contrast to the sulfide counterpart, the Ba<sub>3</sub>Sn<sub>2</sub>Se<sub>7</sub> structure features one split barium site (Ba1 and Ba2) arising from positional disorder. All atoms of the Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> structures occupy the general positions. The main building blocks of the Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> structures are the isolated anionic [Sn<sub>2</sub><i>Q</i><sub>7</sub>]<sup>6-</sup> motifs, which are separated and charge-balanced by the filling of Ba<sup>2+</sup> cations. Optical bandgap studies of polycrystalline Ba<sub>3</sub>Sn<sub>2</sub><i>Q</i><sub>7</sub> samples confirm their semiconducting nature with the direct bandgap values of 2.3(1) eV (<i>Q</i> = S) and 1.9(1) eV (<i>Q</i> = Se). DFT studies also predict the semiconducting nature of the title phases, and the theoretical band gaps are in good agreement with the optical absorption studies. Photovoltaic characterization of the polycrystalline Ba<sub>3</sub>Sn<sub>2</sub>S<sub>7</sub> sample reveals a 23.7% increase in power conversion efficiency, attributed to a reduced electron-hole recombination rate. Moreover, the theoretical electronic structures of the title chalcogenides are presented along with the COHPs results, highlighting the relative strengths of chemical bonds and charge transfer between the metals (Ba and Sn) and chalcogen (S/Se) atoms.

Dalton TransactionsVol. 54(34)
Vignana Jyothi Institute of Management (IN), Indian Institute of Technology Hyderabad (IN)
Science and Engineering Research Board
Affordable and clean energy
Openalex Percentile: Top 39%
Crystal Structures and Properties
0.43
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