2 research outputs found
Cavitands Incorporating a Lewis Acid Dinickel Chelate Function as Receptors for Halide Anions
The halide binding properties of
the cavitand [Ni<sub>2</sub>(L<sup>Me2H4</sup>)]<sup>2+</sup> (<b>4</b>) are reported. Cavitand <b>4</b> exhibits a chelating
N<sub>3</sub>NiÂ(μ-S)<sub>2</sub>NiN<sub>3</sub> moiety with
two square-pyramidal Ni<sup>II</sup>N<sub>3</sub>S<sub>2</sub> units
situated in an anion binding pocket of ∼4 Å diameter formed
by the organic backbone of the (L<sup>Me2H4</sup>)<sup>2–</sup> macrocycle. The receptor reacts with fluoride, chloride (in MeCN/MeOH),
and bromide (in MeCN) ions to afford an isostructural series of halogenido-bridged
complexes [Ni<sub>2</sub>(L<sup>Me2H4</sup>)Â(μ-Hal)]<sup>+</sup> (Hal = F<sup>–</sup> (<b>5</b>), Cl<sup>–</sup> (<b>6</b>), and Br<sup>–</sup> (<b>7</b>)) featuring
a N<sub>3</sub>NiÂ(μ-S)<sub>2</sub>(μ-Hal)ÂNiN<sub>3</sub> core structure. No reaction occurs with iodide or other polyatomic
anions (ClO<sub>4</sub><sup>–</sup>, NO<sub>3</sub><sup>–</sup>, HCO<sub>3</sub><sup>–</sup>, H<sub>2</sub>PO<sub>4</sub><sup>–</sup>, HSO<sub>4</sub><sup>–</sup>, SO<sub>4</sub><sup>2–</sup>). The binding events are accompanied by discrete
UV–vis spectral changes, due to a switch of the coordination
geometry from square-pyramidal (N<sub>3</sub>S<sub>2</sub> donor set
in <b>4</b>) to octahedral in the halogenido-bridged complexes
(N<sub>3</sub>S<sub>2</sub>Hal donor environment in <b>5</b>–<b>7</b>). In MeCN/MeOH (1/1 v/v) the log <i>K</i><sub>11</sub> values for the 1:1 complexes are 7.77(9) (F<sup>–</sup>), 4.06(7) (Cl<sup>–</sup>), and 2.0(1) (Br<sup>–</sup>). X-ray crystallographic analyses for <b>4</b>(ClO<sub>4</sub>)<sub>2</sub>, <b>4</b>(I)<sub>2</sub>, <b>5</b>(F), <b>6</b>(ClO<sub>4</sub>), and <b>7</b>(Br) and computational
studies reveal a significant increase of the intramolecular distance
between two propylene groups at the cavity entrance upon going from
F<sup>–</sup> to I<sup>–</sup> (for the DFT computed
structure). In case of the receptor <b>4</b> and fluorido-bridged
complex <b>5</b>, the corresponding distances are nearly identical.
This indicates a high degree of preorganization of the [Ni<sub>2</sub>(L<sup>Me2H4</sup>)]<sup>2+</sup> receptor and a size fit mismatch
of the receptor binding cavity for anions larger than F<sup>–</sup>
Structure, Magnetic Behavior, and Anisotropy of Homoleptic Trinuclear Lanthanoid 8‑Quinolinolate Complexes
Three
complexes of the form [Ln<sup>III</sup><sub>3</sub>(OQ)<sub>9</sub>] (Ln = Gd, Tb, Dy; OQ = 8-quinolinolate) have been synthesized and
their magnetic properties studied. The trinuclear complexes adopt
V-shaped geometries with three bridging 8-quinolinolate oxygen atoms
between the central and peripheral eight-coordinate metal atoms. The
magnetic properties of these three complexes differ greatly. Variable-temperature
direct-current (dc) magnetic susceptibility measurements reveal that
the gadolinium and terbium complexes display weak antiferromagnetic
nearest-neighbor magnetic exchange interactions. This was quantified
in the isotropic gadolinium case with an exchangecoupling parameter
of <i>J</i> = −0.068(2) cm<sup>–1</sup>. The
dysprosium compound displays weak ferromagnetic exchange. Variable-frequency
and -temperature alternating-current magnetic susceptibility measurements
on the anisotropic cases reveal that the dysprosium complex displays
single-molecule-magnet behavior, in zero dc field, with two distinct
relaxation modes of differing time scales within the same molecule.
Analysis of the data revealed anisotropy barriers of <i>U</i><sub>eff</sub> = 92 and 48 K for the two processes. The terbium complex,
on the other hand, displays no such behavior in zero dc field, but
upon application of a static dc field, slow magnetic relaxation can
be observed. Ab initio and electrostatic calculations were used in
an attempt to explain the origin of the experimentally observed slow
relaxation of the magnetization for the dysprosium complex