TY - JOUR
T1 - Large easy-axis magnetic anisotropy in a series of trigonal prismatic mononuclear cobalt(ii) complexes with zero-field hidden single-molecule magnet behaviour
T2 - the important role of the distortion of the coordination sphere and intermolecular interactions in the slow relaxation
AU - Landart-Gereka, Aritz
AU - Quesada-Moreno, María Mar
AU - Díaz-Ortega, Ismael F.
AU - Nojiri, Hiroyuki
AU - Ozerov, Mykhaylo
AU - Krzystek, J.
AU - Palacios, María A.
AU - Colacio, Enrique
N1 - Funding Information:
Financial support from the Spanish Ministerio de Ciencia e Innovación project (PGC2018 102052-B-C21) MCIN/AEI/10.13039/501100011033/FEDER “Una manera de hacer Europa”, to Junta de Andalucía (FQM-195) and the project I +D+i (P20_00692) and the University of Granada. Part of this work was performed at the NHMFL, which is funded by the National Science Foundation (Cooperative Agreement DMR 1644779) and the State of Florida. HN and IFDO acknowledge GIMRT and ICC-IMR. M. M. Q. M. thanks Junta de Andalucía for a postdoctoral fellowship (DOC_01282) and Ministerio de Ciencia, Innovación y Universidades for a Juan de la Cierva formación contract (grant FJC2018-035709-I supported by MCIN/AEI/10.13039/501100011033). We acknowledge Gloria Pelayo for her help in the synthesis of compound 2 and Silvia Gómez Coca for insightful discussions and help with the quantum-chemical calculations.
Publisher Copyright:
© 2022 The Royal Society of Chemistry.
PY - 2022/3/31
Y1 - 2022/3/31
N2 - The complexes [Co(L)]X·S (X = CoCl42−, S = CH3CN (1); X = ZnCl42−, S = CH3OH (2)), [Co(L)]X2·S (X = ClO4−, S = 2CH3OH (3) and X = BF4− (4)) and [Co(L)(NCS)2] (5), where L = the N6-tripodal ligand tris(pyridylhydrazonyl)phosphorylsulfide, were prepared and studied by X-ray crystallography, ac and dc magnetic data, FIRMS and HFEPR spectra, and theoretical calculations. On passing from 1 to 4, the change of the counteranion decreases slightly the distortion of the CoN6 coordination polyhedron from trigonal prismatic to octahedral, with a parallel increase of the easy-axis magnetic anisotropy. Compound 1 does not show slow magnetic relaxation, even in the presence of a dc magnetic field, due to fast QTM triggered by dipolar interactions. Although the complexes 2-4 show a weak frequency and temperature dependence of the ac susceptibility below 10 K at zero field, they exhibit slow relaxation and single-molecule magnet (SMM) behaviour under the corresponding optimal field. The relaxation of the magnetization takes place mainly through a Raman relaxation process above 4 K, whereas below this temperature QTM and/or direct processes dominate. The relaxation time increases with the parallel increase of the uniaxial anisotropy on passing from 1 to 4. The width of the hysteresis for the trigonal prismatic complexes at 0.4 K decreases in the order 3 > 2 > 4 > 1, which is due to combined effects of QTM relaxation and axial anisotropy. Magnetic dilution of complexes 3 and 4 with ZnII triggers the slow relaxation of the magnetization at zero-field, so that these complexes can be considered as “hidden mononuclear SMMs”. Compound 5, with a compressed octahedral geometry, exhibits easy-plane magnetic anisotropy (D = +34.7 cm−1), and it is a field-induced mononuclear SMM with magnetization relaxation faster than compounds 2-4 and a smaller hysteresis loop.
AB - The complexes [Co(L)]X·S (X = CoCl42−, S = CH3CN (1); X = ZnCl42−, S = CH3OH (2)), [Co(L)]X2·S (X = ClO4−, S = 2CH3OH (3) and X = BF4− (4)) and [Co(L)(NCS)2] (5), where L = the N6-tripodal ligand tris(pyridylhydrazonyl)phosphorylsulfide, were prepared and studied by X-ray crystallography, ac and dc magnetic data, FIRMS and HFEPR spectra, and theoretical calculations. On passing from 1 to 4, the change of the counteranion decreases slightly the distortion of the CoN6 coordination polyhedron from trigonal prismatic to octahedral, with a parallel increase of the easy-axis magnetic anisotropy. Compound 1 does not show slow magnetic relaxation, even in the presence of a dc magnetic field, due to fast QTM triggered by dipolar interactions. Although the complexes 2-4 show a weak frequency and temperature dependence of the ac susceptibility below 10 K at zero field, they exhibit slow relaxation and single-molecule magnet (SMM) behaviour under the corresponding optimal field. The relaxation of the magnetization takes place mainly through a Raman relaxation process above 4 K, whereas below this temperature QTM and/or direct processes dominate. The relaxation time increases with the parallel increase of the uniaxial anisotropy on passing from 1 to 4. The width of the hysteresis for the trigonal prismatic complexes at 0.4 K decreases in the order 3 > 2 > 4 > 1, which is due to combined effects of QTM relaxation and axial anisotropy. Magnetic dilution of complexes 3 and 4 with ZnII triggers the slow relaxation of the magnetization at zero-field, so that these complexes can be considered as “hidden mononuclear SMMs”. Compound 5, with a compressed octahedral geometry, exhibits easy-plane magnetic anisotropy (D = +34.7 cm−1), and it is a field-induced mononuclear SMM with magnetization relaxation faster than compounds 2-4 and a smaller hysteresis loop.
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U2 - 10.1039/d2qi00275b
DO - 10.1039/d2qi00275b
M3 - Article
AN - SCOPUS:85129138379
SN - 2052-1545
VL - 9
SP - 2810
EP - 2831
JO - Inorganic Chemistry Frontiers
JF - Inorganic Chemistry Frontiers
IS - 12
ER -