Interplaybetween Two Structure Types in the IncommensuratelyModulated A<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> Compounds(A = Rb, Cs)

Incommensurately modulated crystals are a rare class of materials that are notoriously difficult to characterize properly. We have synthesized two new incommensurately modulated compounds, Rb<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> and Cs<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub>, based on the M<sub>2</sub>Q<sub>11</sub> (M = Nb, Ta; Q = S, Se) unit using high-temperature solid-state synthesis. Using superspace crystallography in combination with second harmonic generation measurements, we confirmed both materials to be noncentrosymmetric, falling into the superspace group <i>P</i>1(αβγ)0, while the basic cell suggests <i>C</i>2/<i>c</i>. These materials can be structurally understood as ordered combinations of two known structure types, A<sub>6</sub>Ta<sub>4</sub>Se<sub>22</sub> and A<sub>12</sub>Ta<sub>6</sub>Se<sub>35</sub> (A = K, Rb, Cs). While both modulated compounds share structural similarities with the aforementioned known phases, they represent novel structures rather than a literal combination of the two phases, such as a composite. Additionally, both Rb<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> and Cs<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> were optically and thermally characterized, revealing identical band gaps of 1.63 eV and congruent melting points at 434 and 417 °C, respectively.

Publication Details

Journal
Figshare
Published
2025-01-28
DOI
https://doi.org/10.1021/acs.inorgchem.4c04707.s001
Primary Topic
Crystal Structures and Properties
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article
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article

Interplaybetween Two Structure Types in the IncommensuratelyModulated A14+2/3Ta8Se46+2/3 Compounds(A = Rb, Cs)

Figshare
Crystal Structures and Properties
article

Interplaybetween Two Structure Types in the IncommensuratelyModulated A14+2/3Ta8Se46+2/3 Compounds(A = Rb, Cs)

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Abstract

Incommensurately modulated crystals are a rare class of materials that are notoriously difficult to characterize properly. We have synthesized two new incommensurately modulated compounds, Rb<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> and Cs<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub>, based on the M<sub>2</sub>Q<sub>11</sub> (M = Nb, Ta; Q = S, Se) unit using high-temperature solid-state synthesis. Using superspace crystallography in combination with second harmonic generation measurements, we confirmed both materials to be noncentrosymmetric, falling into the superspace group <i>P</i>1(αβγ)0, while the basic cell suggests <i>C</i>2/<i>c</i>. These materials can be structurally understood as ordered combinations of two known structure types, A<sub>6</sub>Ta<sub>4</sub>Se<sub>22</sub> and A<sub>12</sub>Ta<sub>6</sub>Se<sub>35</sub> (A = K, Rb, Cs). While both modulated compounds share structural similarities with the aforementioned known phases, they represent novel structures rather than a literal combination of the two phases, such as a composite. Additionally, both Rb<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> and Cs<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> were optically and thermally characterized, revealing identical band gaps of 1.63 eV and congruent melting points at 434 and 417 °C, respectively.

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Crystal Structures and Properties
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Interplaybetween Two Structure Types in the IncommensuratelyModulated A<sub>14+2/3</sub>Ta<sub>8</sub>Se<sub>46+2/3</sub> Compounds(A = Rb, Cs) · Figshare (2025) | TGRS Research Map | TGRS