Pentacoordinate and Hexacoordinate Mn(III) Complexes of Tetradentate Schiff-Base Ligands Containing Tetracyanidoplatinate(II) Bridges and Revealing Uniaxial Magnetic Anisotropy
Abstract:(2b), where H 2 L4B = N,N'-benzene-bis(4-aminodiethylene-salicylideneiminate), consists of two [{Mn(L4B)} moieties, involving pentacoordinate Mn III atoms, bridged through the tetracyanidoplatinate (II) bridges to which they are coordinated in a trans fashion. Both complexes possess uniaxial type of magnetic anisotropy, with D (the axial parameter of zero-field splitting) = −3.7(1) in 2a and −2.2(1) cm −1 in 2b. Furthermore, the parameters of magnetic anisotropy 2a and 2b were also thoroughly studied by theore… Show more
“…Single crystals of [Mn(salen)] 2 [Pt(CN) 4 ]·H 2 O ( 1·H 2 O ) were prepared by mixing methanol solutions of [Mn(salen)]Cl and K 2 [Pt(CN) 4 ]·3H 2 O in a 2:1 ratio. , At 150 K 1·H 2 O crystallizes in a tetragonal ( P 4/ ncc ). Undulating zigzag layers are constructed from two-connecting [Mn(salen)] + units linked through the nitrogen atoms of the cyanide groups of four-connecting [Pt(CN) 4 ] 2– units (Figure (a)).…”
The ability to tune physical properties is attractive for the development of new materials for myriad applications. Understanding and controlling the structural dynamics in complicated network structures like coordination polymers (CPs) is particularly challenging. We report a series of two-dimensional CPs [Mn(salen)][M(CN)]· xHO (M = Pt (1), PtI (2), and MnN (3)) incorporating zigzag cyano-network layers that display composition-dependent anisotropic thermal expansion properties. Variable-temperature single-crystal X-ray structural analyses demonstrated that the thermal expansion behavior is caused by double structural distortions involving [Mn(salen)] units incorporated into the zigzag layers. Thermal relaxations produce structural transformations resulting in positive thermal expansion for 2·HO and negative thermal expansion for 3. In the case of 1·HO, the relaxation does not occur and zero thermal expansion results in the plane between 200 to 380 K. The present study proposes a new strategy based on structural distortions in coordination networks to control thermal responsivities of frameworks.
“…Single crystals of [Mn(salen)] 2 [Pt(CN) 4 ]·H 2 O ( 1·H 2 O ) were prepared by mixing methanol solutions of [Mn(salen)]Cl and K 2 [Pt(CN) 4 ]·3H 2 O in a 2:1 ratio. , At 150 K 1·H 2 O crystallizes in a tetragonal ( P 4/ ncc ). Undulating zigzag layers are constructed from two-connecting [Mn(salen)] + units linked through the nitrogen atoms of the cyanide groups of four-connecting [Pt(CN) 4 ] 2– units (Figure (a)).…”
The ability to tune physical properties is attractive for the development of new materials for myriad applications. Understanding and controlling the structural dynamics in complicated network structures like coordination polymers (CPs) is particularly challenging. We report a series of two-dimensional CPs [Mn(salen)][M(CN)]· xHO (M = Pt (1), PtI (2), and MnN (3)) incorporating zigzag cyano-network layers that display composition-dependent anisotropic thermal expansion properties. Variable-temperature single-crystal X-ray structural analyses demonstrated that the thermal expansion behavior is caused by double structural distortions involving [Mn(salen)] units incorporated into the zigzag layers. Thermal relaxations produce structural transformations resulting in positive thermal expansion for 2·HO and negative thermal expansion for 3. In the case of 1·HO, the relaxation does not occur and zero thermal expansion results in the plane between 200 to 380 K. The present study proposes a new strategy based on structural distortions in coordination networks to control thermal responsivities of frameworks.
“…Nevertheless, if we consider a special category of SMMs with one paramagnetic center, so called single-ion magnets (SIMs), then the deliberate modulation of the magnetic anisotropy is easier and depends reasonably on the topology and donor atom constitution of the coordination polyhedron [ 2 ]. Up to now, several correlations on the relationship between a structure and anisotropy parameters have been reported, namely for tetracoordinate [ 8 , 9 ], pentacoordinate [ 10 , 11 ], hexacoordinate Ni II and Co II compounds [ 12 , 13 ], tetracoordinate Fe II compounds [ 14 ] and penta and hexacoordinate Mn III compounds [ 15 , 16 ]. From these, the largest number of complexes exhibiting slow-relaxation of magnetization belongs undoubtedly to the group of tetracoordinate Co II compounds, which we have chosen as an object of the present study.…”
Static and dynamic magnetic properties of the tetracoordinate CoII complex [Co(CH3-im)2Cl2], (1, CH3-im = N-methyl-imidazole), studied using thorough analyses of magnetometry, and High-Frequency and -Field EPR (HFEPR) measurements, are reported. The study was supported by ab initio complete active space self-consistent field (CASSCF) calculations. It has been revealed that 1 possesses a large magnetic anisotropy with a large rhombicity (magnetometry: D = −13.5 cm−1, E/D = 0.33; HFEPR: D = −14.5(1) cm−1, E/D = 0.16(1)). These experimental results agree well with the theoretical calculations (D = −11.2 cm−1, E/D = 0.18). Furthermore, it has been revealed that 1 behaves as a field-induced single-ion magnet with a relatively large spin-reversal barrier (Ueff = 33.5 K). The influence of the Cl–Co–Cl angle on magnetic anisotropy parameters was evaluated using the CASSCF calculations.
“…The crystal structures of the related heterometallic cyanido-bridged Mn-Pt-complexes [{Mn(salen)} 2 Pt(CN) 4 ] n (salen = N,N′-bis(salicylidene)ethylenediiminato) [5,6], [Mn(L)Pt(CN) 4 ] n (L = 2,13-dimethyl-3,12-diaza-6,9-dioxa-1(2,6)-pyridinacyclotridecaphane-2,12-diene) [7] and [Mn(phen) Pt(CN) 4 ] n (phen = 1,10-phenanthroline) [8] have been determined previously.…”
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