Double Interpenetration in a Chiral Three-Dimensional Magnet with a (10,3)-a Structure

Study of the Counter Cation Effects on the Supramolecular Structure and Electronic Properties of a Dianionic Oxamate-Based {NiII2} Helicate

Herein, we describe the synthesis, crystal structure, and electronic properties of {[K₂(dmso)(H₂O)₅][Ni₂(H₂mpba)₃]·dmso·2H₂O}_n (1) and [Ni(H₂O)₆][Ni₂(H₂mpba)₃]·3CH₃OH·4H₂O (2) [dmso = dimethyl sulfoxide; CH₃OH = methanol; and H₄mpba = 1,3-phenylenebis(oxamic acid)] bearing the [Ni₂(H₂mpba)₃]^2- helicate, hereafter referred to as {Ni^II₂}. SHAPE software calculations indicate that the coordination geometry of all the Ni^II atoms in 1 and 2 is a distorted octahedron (O_h) whereas the coordination environments for K1 and K2 atoms in 1 are Snub disphenoid J84 (D_2d) and distorted octahedron (O_h), respectively. The {Ni^II₂} helicate in 1 is connected by K⁺ counter cations yielding a 2D coordination network with sql topology. In contrast to 1, the electroneutrality of the triple-stranded [Ni₂(H₂mpba)₃] ^2- dinuclear motif in 2 is achieved by a [Ni(H₂O)₆]²⁺ complex cation, where the three neighboring {Ni^II₂} units interact in a supramolecular fashion through four R₂²(10) homosynthons yielding a 2D array. Voltammetric measurements reveal that both compounds are redox active (with the Ni^II/Ni^I pair being mediated by OH^- ions) but with differences in formal potentials that reflect changes in the energy levels of molecular orbitals. The Ni^II ions from the helicate and the counter-ion (complex cation) in 2 can be reversibly reduced, resulting in the highest faradaic current intensities. The redox reactions in 1 also occur in an alkaline medium but at higher formal potentials. The connection of the helicate with the K⁺ counter cation has an impact on the energy levels of the molecular orbitals; this experimental behavior was further supported by X-ray absorption near-edge spectroscopy (XANES) experiments and computational calculations.

Metal-Organic Frameworks as Playgrounds for Reticulate Single-Molecule Magnets

Achieving fine control on the structure of metal-organic frameworks (MOFs) is mandatory to obtain target physical properties. Herein, we present how the combination of a metalloligand approach and a postsynthetic method is a suitable and highly useful synthetic strategy to success on this extremely difficult task. First, a novel oxamato-based tetranuclear cobalt(III) compound with a tetrahedron-shaped geometry is used, for the first time, as the metalloligand toward calcium(II) metal ions to lead to a diamagnetic Ca^II-Co^III three-dimensional (3D) MOF (1). In a second stage, in a single-crystal-to-single-crystal manner, the calcium(II) ions are replaced by terbium(III), dysprosium(III), holmium(III), and erbium(III) ions to yield four isostructural novel Ln^III-Co^III [Ln = Tb (2), Dy (3), Ho (4), and Er (5)] 3D MOFs. Direct-current magnetic properties for 2-5 show typical performances for the ground-state terms of the lanthanoid cations [⁷F₆ (Tb^III), ⁶H_15/2 (Dy^III), ⁵I₈ (Ho^III), and ⁴I_15/2 (Er^III)]. Analysis of the χ_MT data indicates that the ground state is the lowest M_J value, that is, M_J = 0 (2 and 4) and ±¹/₂ (3 and 5). Kramers' ions (3 and 5) exhibit field-induced emergent frequency-dependent alternating-current magnetic susceptibility signals, which is indicative of the presence of slow magnetic relaxation typical of single-molecule magnets.

Open and closed forms of the interpenetrated [Cu2(Tae)(Bpa)2](NO3)2·nH2O: magnetic properties and high pressure CO2/CH4 gas sorption

Two closed and one open structural forms of the interpenetrated [Cu₂(Tae)(Bpa)₂](NO₃)₂·nH₂O (H₂Tae = 1,1,2,2-tetraacetylethane, Bpa = 1,2-bis(4-pyridyl)ethane) cationic coordination polymer have been synthesized. Three crystallographically related interpenetrated "ths" cationic nets encapsulate water molecules and nitrate anions giving rise to the closed structural forms of [Cu₂(Tae)(Bpa)₂](NO₃)₂·nH₂O. Depending on the location of water molecules and nitrate groups, two different closed forms with 5.5 and 3.6 crystallization water molecules have been obtained. The thermal activation of the closed structures gives rise to a 29% expansion of the unit cell. This closed to open transformation is reversible, and is triggered by the loss or uptake of solvent. The high pressure gas adsorption experiments show similar selectivity values towards CO₂ for CO₂/CH₄ mixtures to that showed by some metal organic frameworks without unsaturated metal sites, and isosteric heats for CO₂ adsorption similar to that for the HKUST-1 compound.

2D and 3D mixed MII/CuIImetal–organic frameworks (M = Ca and Sr) withN,N′-2,6-pyridinebis(oxamate) and oxalate: preparation and magneto-structural study

Heterobimetallic coordination polymers with either antiferro- of ferromagnetic interactions are described herein.

Synthetic ability of dinuclear mesocates containing 1,3-bis(diazinecarboxamide)benzene bridging ligands to form complexes of increased nuclearity. Crystal structures, magnetic properties and theoretical studies

Triple stranded Ni-metallacyclic complexes Na_2.5[Ni₂(bpcb)₃]·0.5OH·18.5H₂O (1) and Na₂[Ni₂(bpzcb)₃]·16H₂O (2), and double stranded Cu-metallacyclic complexes [Cu₂(bpcb)₂(H₂O)₂]·8H₂O (3) and [Cu₂(bpzcb)₂(H₂O)₂]·4H₂O (4) have been assembled from the tailored bisbidentate bridging ligands, 1,3-bis(pyrimidine-2-carboxamide)benzene (H₂bpcb) and 1,3-bis(pyrazine-2-carboxamide)benzene (H₂bpzcb), and the corresponding nitrate salts of the metal ions. Following the "complex as ligand" strategy, 1 can be assembled with either Ni²⁺, Co²⁺ ions or the [Mn(acen)Cl] complex to afford unique, neutral, bent trinuclear molecules [M^IINi(bpcb)₃]·xH₂O (5 and 6) and the 2D honeycomb-like complex (PPh₄){[Ni₂(bpcb)₃]₂[Mn(acen)]₃} (7), respectively. In these cases, the Ni₂ units are linked to the corresponding metal ions through amidate oxygen atoms and the outward nitrogen atom of one of the pyrimidine rings of the bcpb ligand. The assembly of 2 with Ln³⁺ ions (Ln³⁺ = Tb, Gd) leads to one dimensional complexes of formula [{[Ni₂(bpzcb)₃]Tb(H₂O)₅}(CF₃SO₃)·THF·5H₂O]_n (8) and [{[Ni₂(bpzcb)₃]Ln(H₂O)₄(NO₃)}·2THF·nH₂O]_n (9 and 10) (Ln³⁺ = Gd and Tb), where the dinuclear Ni₂ units are joined to two Ln³⁺ ions exclusively through amidate oxygen atoms of two different ligands. The analyses of the magnetic data indicate that 1-4 exhibit intradinuclear ferromagnetic interactions between the metal ions through a spin polarisation mechanism, as supported by DFT calculations. Trinuclear complexes 5 and 6 show predominant antiferromagnetic coupling, which is a result of an antiferromagnetic interaction between one of the Ni²⁺ ions of the Ni₂ unit and the M²⁺ ion through the pyrimidine bridging fragment that is stronger than the polarised ferromagnetic interaction between the Ni²⁺ ions through the bpcb ligand in the dinuclear [Ni₂(bpcb)₃]^2- moiety. Complex 7 shows a dominant antiferromagnetic interaction between the Ni²⁺ and Mn²⁺, whereas the Ni₂Ln (Ln³⁺ = Gd, Tb) chain complexes present ferromagnetic interactions inside the Ni₂ mesocate unit as well as between the Ni²⁺ ions of the Ni₂ unit and the Ln³⁺ ions. The magnetic exchange interactions in these new materials have been experimentally analysed and supported by theoretical DFT studies.