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Magnetic Sponge with Neutral–Ionic Phase Transitions
Phase transitions caused by the charge instability between the neutral and ionic phases of compounds, i.e., N–I phase transitions, provide avenues for switching the intrinsic properties of compounds related to electron/spin correlation and dipole generation as well as charge distribution. However, i...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5827013/ https://www.ncbi.nlm.nih.gov/pubmed/29619302 http://dx.doi.org/10.1002/advs.201700526 |
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author | Kosaka, Wataru Takahashi, Yusuke Nishio, Masaki Narushima, Keisuke Fukunaga, Hiroki Miyasaka, Hitoshi |
author_facet | Kosaka, Wataru Takahashi, Yusuke Nishio, Masaki Narushima, Keisuke Fukunaga, Hiroki Miyasaka, Hitoshi |
author_sort | Kosaka, Wataru |
collection | PubMed |
description | Phase transitions caused by the charge instability between the neutral and ionic phases of compounds, i.e., N–I phase transitions, provide avenues for switching the intrinsic properties of compounds related to electron/spin correlation and dipole generation as well as charge distribution. However, it is extremely difficult to control the transition temperature (T (c)) for the N–I phase transition, and only chemical modification based on the original material have been investigated. Here, a design overview of the tuning of N–I phase transition by interstitial guest molecules is presented. This study reports a new chain coordination‐polymer [Ru(2)(3,4‐Cl(2)PhCO(2))(4)TCNQ(EtO)(2)]∙DCE (1‐DCE; 3,4‐Cl(2)PhCO(2) (−) = 3,4‐dichlorobenzoate; TCNQ(EtO)(2) 2,5‐diethoxy‐7,7,8,8‐tetracyanoquinodimethane; and DCE = 1,2‐dichloroethane) that exhibits a one‐step N–I transition at 230 K (= T (c)) with the N‐ and I‐states possessing a simple paramagnetic state and a ferrimagnetically correlated state for the high‐ and low‐temperature phases, respectively. The T (c) continuously decreases depending on the content of DCE, which eventually disappears with the complete evacuation of DCE, affording solvent‐free compound 1 with the N‐state in the entire temperature range (this behavior is reversible). This is an example of tuning the in situ T (c) for the N–I phase transition via the control of the interstitial guest molecules. |
format | Online Article Text |
id | pubmed-5827013 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-58270132018-04-04 Magnetic Sponge with Neutral–Ionic Phase Transitions Kosaka, Wataru Takahashi, Yusuke Nishio, Masaki Narushima, Keisuke Fukunaga, Hiroki Miyasaka, Hitoshi Adv Sci (Weinh) Full Papers Phase transitions caused by the charge instability between the neutral and ionic phases of compounds, i.e., N–I phase transitions, provide avenues for switching the intrinsic properties of compounds related to electron/spin correlation and dipole generation as well as charge distribution. However, it is extremely difficult to control the transition temperature (T (c)) for the N–I phase transition, and only chemical modification based on the original material have been investigated. Here, a design overview of the tuning of N–I phase transition by interstitial guest molecules is presented. This study reports a new chain coordination‐polymer [Ru(2)(3,4‐Cl(2)PhCO(2))(4)TCNQ(EtO)(2)]∙DCE (1‐DCE; 3,4‐Cl(2)PhCO(2) (−) = 3,4‐dichlorobenzoate; TCNQ(EtO)(2) 2,5‐diethoxy‐7,7,8,8‐tetracyanoquinodimethane; and DCE = 1,2‐dichloroethane) that exhibits a one‐step N–I transition at 230 K (= T (c)) with the N‐ and I‐states possessing a simple paramagnetic state and a ferrimagnetically correlated state for the high‐ and low‐temperature phases, respectively. The T (c) continuously decreases depending on the content of DCE, which eventually disappears with the complete evacuation of DCE, affording solvent‐free compound 1 with the N‐state in the entire temperature range (this behavior is reversible). This is an example of tuning the in situ T (c) for the N–I phase transition via the control of the interstitial guest molecules. John Wiley and Sons Inc. 2017-12-04 /pmc/articles/PMC5827013/ /pubmed/29619302 http://dx.doi.org/10.1002/advs.201700526 Text en © 2017 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 Kosaka, Wataru Takahashi, Yusuke Nishio, Masaki Narushima, Keisuke Fukunaga, Hiroki Miyasaka, Hitoshi Magnetic Sponge with Neutral–Ionic Phase Transitions |
title | Magnetic Sponge with Neutral–Ionic Phase Transitions |
title_full | Magnetic Sponge with Neutral–Ionic Phase Transitions |
title_fullStr | Magnetic Sponge with Neutral–Ionic Phase Transitions |
title_full_unstemmed | Magnetic Sponge with Neutral–Ionic Phase Transitions |
title_short | Magnetic Sponge with Neutral–Ionic Phase Transitions |
title_sort | magnetic sponge with neutral–ionic phase transitions |
topic | Full Papers |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5827013/ https://www.ncbi.nlm.nih.gov/pubmed/29619302 http://dx.doi.org/10.1002/advs.201700526 |
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