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dc.contributor.authorZabala Lekuona, Andoni
dc.contributor.authorLandart Gereka, Aritz
dc.contributor.authorQuesada Moreno, María Mar
dc.contributor.authorMota Ávila, Antonio José
dc.contributor.authorDíaz Ortega, Ismael F.
dc.contributor.authorNojiri, Hyroyuki
dc.contributor.authorKrzystek, Jurek
dc.contributor.authorSeco Botana, José Manuel ORCID
dc.contributor.authorColacio, Enrique
dc.date.accessioned2024-01-19T16:19:13Z
dc.date.available2024-01-19T16:19:13Z
dc.date.issued2023-11-22
dc.identifier.citationInorganic Chemistry 62(49) : 20030–20041 (2023)es_ES
dc.identifier.issn0020-1669
dc.identifier.issn1520-510X
dc.identifier.urihttp://hdl.handle.net/10810/64130
dc.description.abstractA new linear trinuclear Co(II)3 complex with a formula of [{Co(μ-L)}2Co] has been prepared by self-assembly of Co(II) ions and the N3O3-tripodal Schiff base ligand H3L, which is obtained from the condensation of 1,1,1-tris(aminomethyl)ethane and salicylaldehyde. Single X-ray diffraction shows that this compound is centrosymmetric with triple-phenolate bridging groups connecting neighboring Co(II) ions, leading to a paddle-wheel-like structure with a pseudo-C3 axis lying in the Co−Co−Co direction. The Co(II) ions at both ends of the Co(II)3 molecule exhibit distorted trigonal prismatic CoN3O3 geometry, whereas the Co(II) at the middle presents an elongated trigonal antiprismatic CoO6 geometry. The combined analysis of the magnetic data and theoretical calculations reveal strong easy-axis agnetic anisotropy for both types of Co(II) ions (|D| values higher than 115 cm−1) with the local anisotropic axes lying on the pseudo-C3 axis of the molecule. The magnetic exchange interaction between the middle and ends Co(II) ions, extracted by using either a Hamiltonian accounting for the isotropic magnetic coupling and ZFS or the Lines’ model, was found to be medium to strong and antiferromagnetic in nature, whereas the interaction between the external Co(II) ions is weak antiferromagnetic. Interestingly, the compound exhibits slow relaxation of magnetization and open hysteresis at zero field and therefore SMM behavior. The significant magnetic exchange coupling found for [{Co(μ-L)}2Co] is mainly responsible for the quenching of QTM, which combined with the easy-axis local anisotropy of the CoII ions and the ollinearity of their local anisotropy axes with the pseudo-C3 axis favors the observation of SMM behavior at zero field.es_ES
dc.language.isoenges_ES
dc.publisherACSes_ES
dc.rightsinfo:eu-repo/semantics/openAccesses_ES
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectzero-fieldes_ES
dc.subjectSMMes_ES
dc.subjecttrinuclear Co(II)3es_ES
dc.subjectmagnetismes_ES
dc.titleZero-Field SMM Behavior Triggered by Magnetic Exchange Interactions and a Collinear Arrangement of Local Anisotropy Axes in a Linear Co3 II Complexes_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.rights.holderAtribución 4.0es_ES
dc.relation.publisherversionhttps://pubs.acs.org/doi/10.1021/acs.inorgchem.3c02817es_ES
dc.identifier.doi10.1021/acs.inorgchem.3c02817
dc.departamentoesQuímica aplicadaes_ES
dc.departamentoeuKimika aplikatuaes_ES


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