Field-assisted slow relaxation of magnetization in Cu( ii ) complexes with pentaheterocyclic triphenodioxazine ligands: the quasi-one-dimensional versus the binuclear case
Two new copper( ii ) complexes have been obtained by the reaction of sterically crowded triphenodioxazine ligands with Cu( ii ) hexafluoroacetylacetonate. Compound 1 is a co-crystal of Cu(hfac) 2 moieties and triphenodioxazine molecules within a quasi-one-dimensional crystal structure with only weak...
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Veröffentlicht in: | New journal of chemistry 2023-11, Vol.47 (46), p.21353-21360 |
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creator | Korchagin, D. V. Ivakhnenko, E. P. Demidov, O. P. Knyazev, P. A. Efimov, N. N. Morgunov, R. B. Starikov, A. G. Palii, A. V. Minkin, V. I. Aldoshin, S. M. |
description | Two new copper(
ii
) complexes have been obtained by the reaction of sterically crowded triphenodioxazine ligands with Cu(
ii
) hexafluoroacetylacetonate. Compound 1 is a co-crystal of Cu(hfac)
2
moieties and triphenodioxazine molecules within a quasi-one-dimensional crystal structure with only weak Cu⋯N short intermolecular interactions (Cu⋯N distances are equal to 2.69(1) and 2.75(1) Å). In contrast, complex 2 has a binuclear structure with two Cu(hfac)
2
units bridged through triphenodioxazine ligand with the covalent Cu–N bond length of 2.335(2) Å. The magnetic AC susceptibility data show that in spite of the absence of zero-field splitting in the Cu(
ii
) ion having the ground state with spin
S
= 1/2, both compounds demonstrate slow magnetic relaxation at the applied magnetic field. For a quasi-one-dimensional complex 1, the optimal field for observing slow magnetic relaxation is 400 Oe, while for the binuclear complex it is 2500 Oe. The observed temperature dependence of the relaxation time in 1 is well described by the combination of Raman and direct mechanisms of relaxation, while for complex 2 the inclusion of Raman mechanism and quantum tunneling of magnetization is required to describe the relaxation behavior. |
doi_str_mv | 10.1039/D3NJ04614A |
format | Article |
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ii
) complexes have been obtained by the reaction of sterically crowded triphenodioxazine ligands with Cu(
ii
) hexafluoroacetylacetonate. Compound 1 is a co-crystal of Cu(hfac)
2
moieties and triphenodioxazine molecules within a quasi-one-dimensional crystal structure with only weak Cu⋯N short intermolecular interactions (Cu⋯N distances are equal to 2.69(1) and 2.75(1) Å). In contrast, complex 2 has a binuclear structure with two Cu(hfac)
2
units bridged through triphenodioxazine ligand with the covalent Cu–N bond length of 2.335(2) Å. The magnetic AC susceptibility data show that in spite of the absence of zero-field splitting in the Cu(
ii
) ion having the ground state with spin
S
= 1/2, both compounds demonstrate slow magnetic relaxation at the applied magnetic field. For a quasi-one-dimensional complex 1, the optimal field for observing slow magnetic relaxation is 400 Oe, while for the binuclear complex it is 2500 Oe. The observed temperature dependence of the relaxation time in 1 is well described by the combination of Raman and direct mechanisms of relaxation, while for complex 2 the inclusion of Raman mechanism and quantum tunneling of magnetization is required to describe the relaxation behavior.</description><identifier>ISSN: 1144-0546</identifier><identifier>EISSN: 1369-9261</identifier><identifier>DOI: 10.1039/D3NJ04614A</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Copper ; Crystal structure ; Ligands ; Magnetic induction ; Magnetic relaxation ; Magnetization ; Molecular structure ; Quantum tunnelling ; Relaxation time ; Temperature dependence</subject><ispartof>New journal of chemistry, 2023-11, Vol.47 (46), p.21353-21360</ispartof><rights>Copyright Royal Society of Chemistry 2023</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c218t-894a6dc4520b4b0331ff2e2a168e01da960a9189eab741e0aeb77f6493c1438b3</cites><orcidid>0000-0001-6096-503X ; 0000-0002-1682-2362 ; 0000-0003-3555-7442 ; 0000-0002-0199-1382 ; 0000-0003-0338-6466 ; 0000-0001-6627-8329</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Korchagin, D. V.</creatorcontrib><creatorcontrib>Ivakhnenko, E. P.</creatorcontrib><creatorcontrib>Demidov, O. P.</creatorcontrib><creatorcontrib>Knyazev, P. A.</creatorcontrib><creatorcontrib>Efimov, N. N.</creatorcontrib><creatorcontrib>Morgunov, R. B.</creatorcontrib><creatorcontrib>Starikov, A. G.</creatorcontrib><creatorcontrib>Palii, A. V.</creatorcontrib><creatorcontrib>Minkin, V. I.</creatorcontrib><creatorcontrib>Aldoshin, S. M.</creatorcontrib><title>Field-assisted slow relaxation of magnetization in Cu( ii ) complexes with pentaheterocyclic triphenodioxazine ligands: the quasi-one-dimensional versus the binuclear case</title><title>New journal of chemistry</title><description>Two new copper(
ii
) complexes have been obtained by the reaction of sterically crowded triphenodioxazine ligands with Cu(
ii
) hexafluoroacetylacetonate. Compound 1 is a co-crystal of Cu(hfac)
2
moieties and triphenodioxazine molecules within a quasi-one-dimensional crystal structure with only weak Cu⋯N short intermolecular interactions (Cu⋯N distances are equal to 2.69(1) and 2.75(1) Å). In contrast, complex 2 has a binuclear structure with two Cu(hfac)
2
units bridged through triphenodioxazine ligand with the covalent Cu–N bond length of 2.335(2) Å. The magnetic AC susceptibility data show that in spite of the absence of zero-field splitting in the Cu(
ii
) ion having the ground state with spin
S
= 1/2, both compounds demonstrate slow magnetic relaxation at the applied magnetic field. For a quasi-one-dimensional complex 1, the optimal field for observing slow magnetic relaxation is 400 Oe, while for the binuclear complex it is 2500 Oe. The observed temperature dependence of the relaxation time in 1 is well described by the combination of Raman and direct mechanisms of relaxation, while for complex 2 the inclusion of Raman mechanism and quantum tunneling of magnetization is required to describe the relaxation behavior.</description><subject>Copper</subject><subject>Crystal structure</subject><subject>Ligands</subject><subject>Magnetic induction</subject><subject>Magnetic relaxation</subject><subject>Magnetization</subject><subject>Molecular structure</subject><subject>Quantum tunnelling</subject><subject>Relaxation time</subject><subject>Temperature dependence</subject><issn>1144-0546</issn><issn>1369-9261</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNpFkU9v1DAUxCNEJUrhwiewxAWQAn6x14m5VUv_gKpygXP04rx0XXnt1M-h236lfkkWFonTjEY_jUaaqnoD8iNIZT99UdffpDagT59Vx6CMrW1j4Pneg9a1XGnzonrJfCslQGvguHo69xTGGpk9FxoFh3QvMgXcYfEpijSJLd5EKv7xEPgo1ss74b14L1zazoF2xOLel42YKRbcUKGc3IML3omS_byhmEafdvjoI4ngbzCO_FmUDYm7BdnXKVI9-i1F3vdjEL8o88J_gcHHxQXCLBwyvaqOJgxMr__pSfXz_OzH-rK--n7xdX16VbsGulJ3VqMZnV41ctCDVAqmqaEGwXQkYURrJFroLOHQaiCJNLTtZLRVDrTqBnVSvT30zjndLcSlv01L3k_jvumsao3Wq3ZPfThQLifmTFM_Z7_F_NCD7P-c0f8_Q_0GInKAMw</recordid><startdate>20231127</startdate><enddate>20231127</enddate><creator>Korchagin, D. V.</creator><creator>Ivakhnenko, E. P.</creator><creator>Demidov, O. P.</creator><creator>Knyazev, P. A.</creator><creator>Efimov, N. N.</creator><creator>Morgunov, R. B.</creator><creator>Starikov, A. G.</creator><creator>Palii, A. V.</creator><creator>Minkin, V. I.</creator><creator>Aldoshin, S. M.</creator><general>Royal Society of Chemistry</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>H9R</scope><scope>JG9</scope><scope>KA0</scope><orcidid>https://orcid.org/0000-0001-6096-503X</orcidid><orcidid>https://orcid.org/0000-0002-1682-2362</orcidid><orcidid>https://orcid.org/0000-0003-3555-7442</orcidid><orcidid>https://orcid.org/0000-0002-0199-1382</orcidid><orcidid>https://orcid.org/0000-0003-0338-6466</orcidid><orcidid>https://orcid.org/0000-0001-6627-8329</orcidid></search><sort><creationdate>20231127</creationdate><title>Field-assisted slow relaxation of magnetization in Cu( ii ) complexes with pentaheterocyclic triphenodioxazine ligands: the quasi-one-dimensional versus the binuclear case</title><author>Korchagin, D. V. ; Ivakhnenko, E. P. ; Demidov, O. P. ; Knyazev, P. A. ; Efimov, N. N. ; Morgunov, R. B. ; Starikov, A. G. ; Palii, A. V. ; Minkin, V. I. ; Aldoshin, S. M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c218t-894a6dc4520b4b0331ff2e2a168e01da960a9189eab741e0aeb77f6493c1438b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Copper</topic><topic>Crystal structure</topic><topic>Ligands</topic><topic>Magnetic induction</topic><topic>Magnetic relaxation</topic><topic>Magnetization</topic><topic>Molecular structure</topic><topic>Quantum tunnelling</topic><topic>Relaxation time</topic><topic>Temperature dependence</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Korchagin, D. V.</creatorcontrib><creatorcontrib>Ivakhnenko, E. P.</creatorcontrib><creatorcontrib>Demidov, O. P.</creatorcontrib><creatorcontrib>Knyazev, P. A.</creatorcontrib><creatorcontrib>Efimov, N. N.</creatorcontrib><creatorcontrib>Morgunov, R. B.</creatorcontrib><creatorcontrib>Starikov, A. G.</creatorcontrib><creatorcontrib>Palii, A. V.</creatorcontrib><creatorcontrib>Minkin, V. I.</creatorcontrib><creatorcontrib>Aldoshin, S. M.</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Illustrata: Natural Sciences</collection><collection>Materials Research Database</collection><collection>ProQuest Illustrata: Technology Collection</collection><jtitle>New journal of chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Korchagin, D. V.</au><au>Ivakhnenko, E. P.</au><au>Demidov, O. P.</au><au>Knyazev, P. A.</au><au>Efimov, N. N.</au><au>Morgunov, R. B.</au><au>Starikov, A. G.</au><au>Palii, A. V.</au><au>Minkin, V. I.</au><au>Aldoshin, S. M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Field-assisted slow relaxation of magnetization in Cu( ii ) complexes with pentaheterocyclic triphenodioxazine ligands: the quasi-one-dimensional versus the binuclear case</atitle><jtitle>New journal of chemistry</jtitle><date>2023-11-27</date><risdate>2023</risdate><volume>47</volume><issue>46</issue><spage>21353</spage><epage>21360</epage><pages>21353-21360</pages><issn>1144-0546</issn><eissn>1369-9261</eissn><abstract>Two new copper(
ii
) complexes have been obtained by the reaction of sterically crowded triphenodioxazine ligands with Cu(
ii
) hexafluoroacetylacetonate. Compound 1 is a co-crystal of Cu(hfac)
2
moieties and triphenodioxazine molecules within a quasi-one-dimensional crystal structure with only weak Cu⋯N short intermolecular interactions (Cu⋯N distances are equal to 2.69(1) and 2.75(1) Å). In contrast, complex 2 has a binuclear structure with two Cu(hfac)
2
units bridged through triphenodioxazine ligand with the covalent Cu–N bond length of 2.335(2) Å. The magnetic AC susceptibility data show that in spite of the absence of zero-field splitting in the Cu(
ii
) ion having the ground state with spin
S
= 1/2, both compounds demonstrate slow magnetic relaxation at the applied magnetic field. For a quasi-one-dimensional complex 1, the optimal field for observing slow magnetic relaxation is 400 Oe, while for the binuclear complex it is 2500 Oe. The observed temperature dependence of the relaxation time in 1 is well described by the combination of Raman and direct mechanisms of relaxation, while for complex 2 the inclusion of Raman mechanism and quantum tunneling of magnetization is required to describe the relaxation behavior.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/D3NJ04614A</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0001-6096-503X</orcidid><orcidid>https://orcid.org/0000-0002-1682-2362</orcidid><orcidid>https://orcid.org/0000-0003-3555-7442</orcidid><orcidid>https://orcid.org/0000-0002-0199-1382</orcidid><orcidid>https://orcid.org/0000-0003-0338-6466</orcidid><orcidid>https://orcid.org/0000-0001-6627-8329</orcidid></addata></record> |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Copper Crystal structure Ligands Magnetic induction Magnetic relaxation Magnetization Molecular structure Quantum tunnelling Relaxation time Temperature dependence |
title | Field-assisted slow relaxation of magnetization in Cu( ii ) complexes with pentaheterocyclic triphenodioxazine ligands: the quasi-one-dimensional versus the binuclear case |
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