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Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2

Quantum magnetic properties in a geometrically frustrated lattice of spin‐1/2 magnet, such as quantum spin liquid or solid and the associated spin fractionalization, are considered key in developing a new phase of matter. The feasibility of observing the quantum magnetic properties, usually found in...

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Autores principales: Gunasekera, Jagath, Dahal, Ashutosh, Chen, Yiyao, Rodriguez‐Rivera, Jose A., Harriger, Leland W., Thomas, Stefan, Heitmann, Thomas W., Dugaev, Vitalii, Ernst, Arthur, Singh, Deepak K.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5980209/
https://www.ncbi.nlm.nih.gov/pubmed/29876219
http://dx.doi.org/10.1002/advs.201700978
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author Gunasekera, Jagath
Dahal, Ashutosh
Chen, Yiyao
Rodriguez‐Rivera, Jose A.
Harriger, Leland W.
Thomas, Stefan
Heitmann, Thomas W.
Dugaev, Vitalii
Ernst, Arthur
Singh, Deepak K.
author_facet Gunasekera, Jagath
Dahal, Ashutosh
Chen, Yiyao
Rodriguez‐Rivera, Jose A.
Harriger, Leland W.
Thomas, Stefan
Heitmann, Thomas W.
Dugaev, Vitalii
Ernst, Arthur
Singh, Deepak K.
author_sort Gunasekera, Jagath
collection PubMed
description Quantum magnetic properties in a geometrically frustrated lattice of spin‐1/2 magnet, such as quantum spin liquid or solid and the associated spin fractionalization, are considered key in developing a new phase of matter. The feasibility of observing the quantum magnetic properties, usually found in geometrically frustrated lattice of spin‐1/2 magnet, in a perovskite material with controlled disorder is demonstrated. It is found that the controlled chemical disorder, due to the chemical substitution of Ru ions by Co‐ions, in a simple perovskite CaRuO(3) creates a random prototype configuration of artificial spin‐1/2 that forms dimer pairs between the nearest and further away ions. The localization of the Co impurity in the Ru matrix is analyzed using the Anderson localization formulation. The dimers of artificial spin‐1/2, due to the localization of Co impurities, exhibit singlet‐to‐triplet excitation at low temperature without any ordered spin correlation. The localized gapped excitation evolves into a gapless quasi‐continuum as dimer pairs break and create freely fluctuating fractionalized spins at high temperature. Together, these properties hint at a new quantum magnetic state with strong resemblance to the resonance valence bond system.
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spelling pubmed-59802092018-06-06 Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2 Gunasekera, Jagath Dahal, Ashutosh Chen, Yiyao Rodriguez‐Rivera, Jose A. Harriger, Leland W. Thomas, Stefan Heitmann, Thomas W. Dugaev, Vitalii Ernst, Arthur Singh, Deepak K. Adv Sci (Weinh) Full Papers Quantum magnetic properties in a geometrically frustrated lattice of spin‐1/2 magnet, such as quantum spin liquid or solid and the associated spin fractionalization, are considered key in developing a new phase of matter. The feasibility of observing the quantum magnetic properties, usually found in geometrically frustrated lattice of spin‐1/2 magnet, in a perovskite material with controlled disorder is demonstrated. It is found that the controlled chemical disorder, due to the chemical substitution of Ru ions by Co‐ions, in a simple perovskite CaRuO(3) creates a random prototype configuration of artificial spin‐1/2 that forms dimer pairs between the nearest and further away ions. The localization of the Co impurity in the Ru matrix is analyzed using the Anderson localization formulation. The dimers of artificial spin‐1/2, due to the localization of Co impurities, exhibit singlet‐to‐triplet excitation at low temperature without any ordered spin correlation. The localized gapped excitation evolves into a gapless quasi‐continuum as dimer pairs break and create freely fluctuating fractionalized spins at high temperature. Together, these properties hint at a new quantum magnetic state with strong resemblance to the resonance valence bond system. John Wiley and Sons Inc. 2018-03-02 /pmc/articles/PMC5980209/ /pubmed/29876219 http://dx.doi.org/10.1002/advs.201700978 Text en © 2018 The Authors. Published by WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Full Papers
Gunasekera, Jagath
Dahal, Ashutosh
Chen, Yiyao
Rodriguez‐Rivera, Jose A.
Harriger, Leland W.
Thomas, Stefan
Heitmann, Thomas W.
Dugaev, Vitalii
Ernst, Arthur
Singh, Deepak K.
Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2
title Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2
title_full Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2
title_fullStr Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2
title_full_unstemmed Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2
title_short Quantum Magnetic Properties in Perovskite with Anderson Localized Artificial Spin‐1/2
title_sort quantum magnetic properties in perovskite with anderson localized artificial spin‐1/2
topic Full Papers
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5980209/
https://www.ncbi.nlm.nih.gov/pubmed/29876219
http://dx.doi.org/10.1002/advs.201700978
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