Cargando…

Change in the Electronic Structure of the Cobalt(II) Ion in a One-Dimensional Polymer with Flexible Linkers Induced by a Structural Phase Transition †

A new 1D-coordination polymer [Co(Piv)(2)(NH(2)(CH(2))(6)NH(2))](n) (1, Piv is Me(3)CCO(2)(−) anion) was obtained, the mononuclear fragments {Co(O(2)CR)(2)} within which are linked by μ-bridged molecules of hexamethylenediamine (NH(2)(CH(2))(6)NH(2)). For this compound, two different monoclinic C2/c...

Descripción completa

Detalles Bibliográficos
Autores principales: Yambulatov, Dmitriy S., Voronina, Julia K., Goloveshkin, Alexander S., Svetogorov, Roman D., Veber, Sergey L., Efimov, Nikolay N., Matyukhina, Anna K., Nikolaevskii, Stanislav A., Eremenko, Igor L., Kiskin, Mikhail A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9820815/
https://www.ncbi.nlm.nih.gov/pubmed/36613658
http://dx.doi.org/10.3390/ijms24010215
Descripción
Sumario:A new 1D-coordination polymer [Co(Piv)(2)(NH(2)(CH(2))(6)NH(2))](n) (1, Piv is Me(3)CCO(2)(−) anion) was obtained, the mononuclear fragments {Co(O(2)CR)(2)} within which are linked by μ-bridged molecules of hexamethylenediamine (NH(2)(CH(2))(6)NH(2)). For this compound, two different monoclinic C2/c (α-1) and P2/n (β-1) phases were found at room temperature by single-crystal X-ray diffraction analysis, with a similar structure of chains and their packages in unit cells. The low-temperature phase (γ-1) of crystal 1 at 150 K corresponds to the triclinic space group P-1. As the temperature decreases, the structural phase transition (SPT) in the α-1 and β-1 crystals is accompanied by an increase in the crystal packing density caused by the rearrangements of both H-bonds and the nearest ligand environment of the cobalt atom (“octahedral CoN(2)O(4) around the metal center at room temperature” → “pseudo-tetrahedral CoN(2)O(2) at 150 K”). The SPT was confirmed by DSC in the temperature range 210–150 K; when heated above 220 K, anomalies in the behavior of the heat flow are observed, which may be associated with the reversibility of SPT; endo effects are observed up to 300 K. The SPT starts below 200 K. At 100 K, a mixture of phases was found in sample 1: 27% α-1 phase, 61% γ-1 phase. In addition, at 100 K, 12% of the new δ-1 phase was detected, which was identified from the diffraction pattern at 260 K upon subsequent heating: the a,b,c-parameters and unit cell volume are close to the structure parameters of γ-1, and the values of the α,β,γ-angles are significantly different. Further heating leads to a phase transition from δ-1 to α-1, which both coexist at room temperature. According to the DC magnetometry data, during cooling and heating, the χ(M)T(T) curves for 1 form a hysteresis loop with ~110 K, in which the difference in the χ(M)T values reaches 9%. Ab initio calculations of the electronic structure of cobalt(II) in α-1 and γ-1 have been performed. Based on the EPR data at 10 K and the ab initio calculations, the behavior of the χ(M)T(T) curve for 1 was simulated in the temperature range of 2–150 K. It was found that 1 exhibits slow magnetic relaxation in a field of 1000 Oe.