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Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain
The cobalt(II) in [Co(NCS)(2)(4‐methoxypyridine)(2)](n) are linked by pairs of thiocyanate anions into linear chains. In contrast to a previous structure determination, two crystallographically independent cobalt(II) centers have been found to be present. In the antiferromagnetic state, below the cr...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7078958/ https://www.ncbi.nlm.nih.gov/pubmed/31702081 http://dx.doi.org/10.1002/chem.201903924 |
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author | Rams, Michał Jochim, Aleksej Böhme, Michael Lohmiller, Thomas Ceglarska, Magdalena Rams, Marek M. Schnegg, Alexander Plass, Winfried Näther, Christian |
author_facet | Rams, Michał Jochim, Aleksej Böhme, Michael Lohmiller, Thomas Ceglarska, Magdalena Rams, Marek M. Schnegg, Alexander Plass, Winfried Näther, Christian |
author_sort | Rams, Michał |
collection | PubMed |
description | The cobalt(II) in [Co(NCS)(2)(4‐methoxypyridine)(2)](n) are linked by pairs of thiocyanate anions into linear chains. In contrast to a previous structure determination, two crystallographically independent cobalt(II) centers have been found to be present. In the antiferromagnetic state, below the critical temperature (T (c)=3.94 K) and critical field (H (c)=290 Oe), slow relaxations of the ferromagnetic chains are observed. They originate mainly from defects in the magnetic structure, which has been elucidated by micromagnetic Monte Carlo simulations and ac measurements using pristine and defect samples. The energy barriers of the relaxations are Δ(τ1)=44.9(5) K and Δ(τ2)=26.0(7) K for long and short spin chains, respectively. The spin excitation energy, measured by using frequency‐domain EPR spectroscopy, is 19.1 cm(−1) and shifts 0.1 cm(−1) due to the magnetic ordering. Ab initio calculations revealed easy‐axis anisotropy for both Co(II) centers, and also an exchange anisotropy J(xx)/J(zz) of 0.21. The XXZ anisotropic Heisenberg model (solved by using the density renormalization matrix group technique) was used to reconcile the specific heat, susceptibility, and EPR data. |
format | Online Article Text |
id | pubmed-7078958 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-70789582020-03-19 Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain Rams, Michał Jochim, Aleksej Böhme, Michael Lohmiller, Thomas Ceglarska, Magdalena Rams, Marek M. Schnegg, Alexander Plass, Winfried Näther, Christian Chemistry Full Papers The cobalt(II) in [Co(NCS)(2)(4‐methoxypyridine)(2)](n) are linked by pairs of thiocyanate anions into linear chains. In contrast to a previous structure determination, two crystallographically independent cobalt(II) centers have been found to be present. In the antiferromagnetic state, below the critical temperature (T (c)=3.94 K) and critical field (H (c)=290 Oe), slow relaxations of the ferromagnetic chains are observed. They originate mainly from defects in the magnetic structure, which has been elucidated by micromagnetic Monte Carlo simulations and ac measurements using pristine and defect samples. The energy barriers of the relaxations are Δ(τ1)=44.9(5) K and Δ(τ2)=26.0(7) K for long and short spin chains, respectively. The spin excitation energy, measured by using frequency‐domain EPR spectroscopy, is 19.1 cm(−1) and shifts 0.1 cm(−1) due to the magnetic ordering. Ab initio calculations revealed easy‐axis anisotropy for both Co(II) centers, and also an exchange anisotropy J(xx)/J(zz) of 0.21. The XXZ anisotropic Heisenberg model (solved by using the density renormalization matrix group technique) was used to reconcile the specific heat, susceptibility, and EPR data. John Wiley and Sons Inc. 2020-01-09 2020-03-02 /pmc/articles/PMC7078958/ /pubmed/31702081 http://dx.doi.org/10.1002/chem.201903924 Text en © 2019 The Authors. Published by Wiley-VCH Verlag GmbH & Co. KGaA. This is an open access article under the terms of the http://creativecommons.org/licenses/by-nc-nd/4.0/ License, which permits use and distribution in any medium, provided the original work is properly cited, the use is non‐commercial and no modifications or adaptations are made. |
spellingShingle | Full Papers Rams, Michał Jochim, Aleksej Böhme, Michael Lohmiller, Thomas Ceglarska, Magdalena Rams, Marek M. Schnegg, Alexander Plass, Winfried Näther, Christian Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain |
title | Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain |
title_full | Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain |
title_fullStr | Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain |
title_full_unstemmed | Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain |
title_short | Single‐Chain Magnet Based on Cobalt(II) Thiocyanate as XXZ Spin Chain |
title_sort | single‐chain magnet based on cobalt(ii) thiocyanate as xxz spin chain |
topic | Full Papers |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7078958/ https://www.ncbi.nlm.nih.gov/pubmed/31702081 http://dx.doi.org/10.1002/chem.201903924 |
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