TY - JOUR
T1 - Interplay between Two Structure Types in the Incommensurately Modulated A14+2/3Ta8Se46+2/3 Compounds (A = Rb, Cs)
AU - Ie, Thomas S.
AU - Balvanz, Adam
AU - Malliakas, Christos D.
AU - Nag, Jadupati
AU - Sarker, Saugata
AU - Marmer, Avani
AU - Gopalan, Venkatraman
AU - Kanatzidis, Mercouri G.
N1 - Publisher Copyright:
© 2025 American Chemical Society.
PY - 2025/2/10
Y1 - 2025/2/10
N2 - Incommensurately modulated crystals are a rare class of materials that are notoriously difficult to characterize properly. We have synthesized two new incommensurately modulated compounds, Rb14+2/3Ta8Se46+2/3 and Cs14+2/3Ta8Se46+2/3, based on the M2Q11 (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 P1(αβγ)0, while the basic cell suggests C2/c. These materials can be structurally understood as ordered combinations of two known structure types, A6Ta4Se22 and A12Ta6Se35 (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 Rb14+2/3Ta8Se46+2/3 and Cs14+2/3Ta8Se46+2/3 were optically and thermally characterized, revealing identical band gaps of 1.63 eV and congruent melting points at 434 and 417 °C, respectively.
AB - Incommensurately modulated crystals are a rare class of materials that are notoriously difficult to characterize properly. We have synthesized two new incommensurately modulated compounds, Rb14+2/3Ta8Se46+2/3 and Cs14+2/3Ta8Se46+2/3, based on the M2Q11 (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 P1(αβγ)0, while the basic cell suggests C2/c. These materials can be structurally understood as ordered combinations of two known structure types, A6Ta4Se22 and A12Ta6Se35 (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 Rb14+2/3Ta8Se46+2/3 and Cs14+2/3Ta8Se46+2/3 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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U2 - 10.1021/acs.inorgchem.4c04707
DO - 10.1021/acs.inorgchem.4c04707
M3 - Article
C2 - 39870572
AN - SCOPUS:85216331792
SN - 0020-1669
VL - 64
SP - 2403
EP - 2414
JO - Inorganic chemistry
JF - Inorganic chemistry
IS - 5
ER -