When van der Waals Met Kagome: A 2D Antimonide with a Vanadium-Kagome Network

2D materials showcase unconventional properties emerging from quantum confinement effects. In this work, a "soft chemical" route allows for the deintercalation of K<sup>+</sup> from the layered antimonide KV<sub>6</sub>Sb<sub>6</sub>, resulting in the discovery of a new metastable 2D-Kagome antimonide K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> with a van der Waals gap of 3.2 Å. The structure of K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> was determined via the synergistic techniques, including X-ray pair distribution function analysis, advanced transmission electron microscopy, and density functional theory calculations. The K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> compound crystallizes in the monoclinic space group <i>C</i>2/<i>m</i> (<i>a</i> = 9.57(2) Å, <i>b</i> = 5.502(8) Å, <i>c</i> = 10.23(2) Å, β = 97.6(2)°, <i>Z</i> = 2). The [V<sub>6</sub>Sb<sub>6</sub>] layers in K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> are retained upon deintercalation and closely resemble the layers in the parent compound, yet deintercalation results in a relative shift of the adjacent [V<sub>6</sub>Sb<sub>6</sub>] layers. The magnetic properties of the K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> phase in the 2-300 K range are comparable to those of KV<sub>6</sub>Sb<sub>6</sub> and another Kagome antimonide KV<sub>3</sub>Sb<sub>5</sub>, consistent with nearly temperature-independent paramagnetism. Electronic band structure calculation suggests a nontrivial band topology with flat bands and opening of band crossing afforded by deintercalation. Transport property measurements reveal a metallic nature for K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> and a low thermal conductivity of 0.6 W K<sup>-1</sup> m<sup>-1</sup> at 300 K. Additionally, ion exchange in KV<sub>6</sub>Sb<sub>6</sub> via a solvothermal route leads to a successful partial exchange of K<sup>+</sup> with <i>A</i><sup>+</sup> (<i>A</i> = Na, Rb, and Cs). This study highlights the tunability of the layered structure of the KV<sub>6</sub>Sb<sub>6</sub> compound, providing a rich playground for the realization of new 2D materials.

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Journal
Journal of the American Chemical Society
Published
2024-09-21
DOI
https://doi.org/10.1021/jacs.4c07285
Citations
6
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
2.03

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article

When van der Waals Met Kagome: A 2D Antimonide with a Vanadium-Kagome Network

Julia V. Zaikina, Shiya Chen, Shahnaz Mukta, Yaroslav Mudryk et al.
6 citations
Journal of the American Chemical Society
Topological Materials and Phenomena
2.03
article

When van der Waals Met Kagome: A 2D Antimonide with a Vanadium-Kagome Network

Julia V. Zaikina, Shiya Chen, Shahnaz Mukta, Yaroslav Mudryk, Yang Sun, Alexander Gundlach‐Graham, Arka Sarkar, Yao Abusa, Aishwarya Mantravadi, Oleg I. Lebedev, Bradyn C. Weaver, Kai‐Ming Ho
article en
6 citations

Abstract

2D materials showcase unconventional properties emerging from quantum confinement effects. In this work, a "soft chemical" route allows for the deintercalation of K<sup>+</sup> from the layered antimonide KV<sub>6</sub>Sb<sub>6</sub>, resulting in the discovery of a new metastable 2D-Kagome antimonide K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> with a van der Waals gap of 3.2 Å. The structure of K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> was determined via the synergistic techniques, including X-ray pair distribution function analysis, advanced transmission electron microscopy, and density functional theory calculations. The K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> compound crystallizes in the monoclinic space group <i>C</i>2/<i>m</i> (<i>a</i> = 9.57(2) Å, <i>b</i> = 5.502(8) Å, <i>c</i> = 10.23(2) Å, β = 97.6(2)°, <i>Z</i> = 2). The [V<sub>6</sub>Sb<sub>6</sub>] layers in K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> are retained upon deintercalation and closely resemble the layers in the parent compound, yet deintercalation results in a relative shift of the adjacent [V<sub>6</sub>Sb<sub>6</sub>] layers. The magnetic properties of the K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> phase in the 2-300 K range are comparable to those of KV<sub>6</sub>Sb<sub>6</sub> and another Kagome antimonide KV<sub>3</sub>Sb<sub>5</sub>, consistent with nearly temperature-independent paramagnetism. Electronic band structure calculation suggests a nontrivial band topology with flat bands and opening of band crossing afforded by deintercalation. Transport property measurements reveal a metallic nature for K<sub>0.1(1)</sub>V<sub>6</sub>Sb<sub>6</sub> and a low thermal conductivity of 0.6 W K<sup>-1</sup> m<sup>-1</sup> at 300 K. Additionally, ion exchange in KV<sub>6</sub>Sb<sub>6</sub> via a solvothermal route leads to a successful partial exchange of K<sup>+</sup> with <i>A</i><sup>+</sup> (<i>A</i> = Na, Rb, and Cs). This study highlights the tunability of the layered structure of the KV<sub>6</sub>Sb<sub>6</sub> compound, providing a rich playground for the realization of new 2D materials.

Journal of the American Chemical SocietyVol. 146(39)
Centre National de la Recherche Scientifique (FR), Iowa State University (US), Xiamen University (CN), École Nationale Supérieure d'Ingénieurs de Caen (FR), Société Nationale des Chemins de Fer Français (France) (FR), Ames National Laboratory (US), Laboratoire de Cristallographie et Sciences des Matériaux (FR)
Natural Science Foundation of Xiamen City, National Natural Science Foundation of China, Fundamental Research Funds for the Central Universities, Division of Materials Research, Basic Energy Sciences
Openalex Percentile: Top 13%
Topological Materials and Phenomena
2.03
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