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Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)

[Image: see text] A new reduced phase derived from the excitonic insulator candidate Ta(2)NiSe(5) has been synthesized via the intercalation of lithium. LiTa(2)NiSe(5) crystallizes in the orthorhombic space group Pmnb (no. 62) with lattice parameters a = 3.50247(3) Å, b = 13.4053(4) Å, c = 15.7396(2...

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Autores principales: Hyde, P. A., Cen, J., Cassidy, S. J., Rees, N. H., Holdship, P., Smith, R. I., Zhu, B., Scanlon, D. O., Clarke, S. J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10394660/
https://www.ncbi.nlm.nih.gov/pubmed/37466301
http://dx.doi.org/10.1021/acs.inorgchem.3c01510
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author Hyde, P. A.
Cen, J.
Cassidy, S. J.
Rees, N. H.
Holdship, P.
Smith, R. I.
Zhu, B.
Scanlon, D. O.
Clarke, S. J.
author_facet Hyde, P. A.
Cen, J.
Cassidy, S. J.
Rees, N. H.
Holdship, P.
Smith, R. I.
Zhu, B.
Scanlon, D. O.
Clarke, S. J.
author_sort Hyde, P. A.
collection PubMed
description [Image: see text] A new reduced phase derived from the excitonic insulator candidate Ta(2)NiSe(5) has been synthesized via the intercalation of lithium. LiTa(2)NiSe(5) crystallizes in the orthorhombic space group Pmnb (no. 62) with lattice parameters a = 3.50247(3) Å, b = 13.4053(4) Å, c = 15.7396(2) Å, and Z = 4, with an increase of the unit cell volume by 5.44(1)% compared with Ta(2)NiSe(5). Significant rearrangement of the Ta-Ni-Se layers is observed, in particular a very significant relative displacement of the layers compared to the parent phase, similar to that which occurs under hydrostatic pressure. Neutron powder diffraction experiments and computational analysis confirm that Li occupies a distorted triangular prismatic site formed by Se atoms of adjacent Ta(2)NiSe(5) layers with an average Li–Se bond length of 2.724(2) Å. Li-NMR experiments show a single Li environment at ambient temperature. Intercalation suppresses the distortion to monoclinic symmetry that occurs in Ta(2)NiSe(5) at 328 K and that is believed to be driven by the formation of an excitonic insulating state. Magnetometry data show that the reduced phase has a smaller net diamagnetic susceptibility than Ta(2)NiSe(5) due to the enhancement of the temperature-independent Pauli paramagnetism caused by the increased density of states at the Fermi level evident also from the calculations, consistent with the injection of electrons during intercalation and formation of a metallic phase.
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spelling pubmed-103946602023-08-03 Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5) Hyde, P. A. Cen, J. Cassidy, S. J. Rees, N. H. Holdship, P. Smith, R. I. Zhu, B. Scanlon, D. O. Clarke, S. J. Inorg Chem [Image: see text] A new reduced phase derived from the excitonic insulator candidate Ta(2)NiSe(5) has been synthesized via the intercalation of lithium. LiTa(2)NiSe(5) crystallizes in the orthorhombic space group Pmnb (no. 62) with lattice parameters a = 3.50247(3) Å, b = 13.4053(4) Å, c = 15.7396(2) Å, and Z = 4, with an increase of the unit cell volume by 5.44(1)% compared with Ta(2)NiSe(5). Significant rearrangement of the Ta-Ni-Se layers is observed, in particular a very significant relative displacement of the layers compared to the parent phase, similar to that which occurs under hydrostatic pressure. Neutron powder diffraction experiments and computational analysis confirm that Li occupies a distorted triangular prismatic site formed by Se atoms of adjacent Ta(2)NiSe(5) layers with an average Li–Se bond length of 2.724(2) Å. Li-NMR experiments show a single Li environment at ambient temperature. Intercalation suppresses the distortion to monoclinic symmetry that occurs in Ta(2)NiSe(5) at 328 K and that is believed to be driven by the formation of an excitonic insulating state. Magnetometry data show that the reduced phase has a smaller net diamagnetic susceptibility than Ta(2)NiSe(5) due to the enhancement of the temperature-independent Pauli paramagnetism caused by the increased density of states at the Fermi level evident also from the calculations, consistent with the injection of electrons during intercalation and formation of a metallic phase. American Chemical Society 2023-07-19 /pmc/articles/PMC10394660/ /pubmed/37466301 http://dx.doi.org/10.1021/acs.inorgchem.3c01510 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Hyde, P. A.
Cen, J.
Cassidy, S. J.
Rees, N. H.
Holdship, P.
Smith, R. I.
Zhu, B.
Scanlon, D. O.
Clarke, S. J.
Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)
title Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)
title_full Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)
title_fullStr Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)
title_full_unstemmed Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)
title_short Lithium Intercalation into the Excitonic Insulator Candidate Ta(2)NiSe(5)
title_sort lithium intercalation into the excitonic insulator candidate ta(2)nise(5)
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10394660/
https://www.ncbi.nlm.nih.gov/pubmed/37466301
http://dx.doi.org/10.1021/acs.inorgchem.3c01510
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