9 research outputs found
Guanidinate Rare-Earth Tetraphenylborate Complexes and Their Prospects in Single-Molecule Magnetism
The pursuit of higher-nuclearity rare-earth-metal clusters
necessitates
adequate ancillary ligand scaffolds as well as easily dissociable
counterions. To this end, guanidinate anions are advantageous owing
to their highly customizable, sterically encumbering, anionic charged
framework. Here, we present the two mononuclear guanidinate rare-earth
complexes [{(Me3Si)2NC(NiPr)2}2RE][(μ-η6-Ph)(BPh3)], (RE = Y (1), Dy (2)), featuring
inner-sphere tetraphenylborate anions. Each complex is sterically
congested and comprises a metal ion that is ligated by two ancillary
guanidinate ions and one tetraphenylborate ligand. The isostructural
compounds, 1 and 2, were synthesized from
a protonolysis reaction between guanidinate alkyl complexes and [HNEt3][BPh4]. The isolated molecules were characterized
by X-ray crystallography and IR, NMR, and UV–vis spectroscopy.
The crowded coordination sphere around each metal ion implemented
by the ancillary guanidinate ligands causes the tetraphenylborate
ion to adopt a rare η6-binding mode where the metal
center interacts asymmetrically with the carbon atoms of one phenyl
ring. DFT and NBO calculations carried out on 1 provide
insight into a complicated bonding picture between one of the phenyl
rings of the BPh4– moiety and the rare-earth
ion. Furthermore, the dysprosium congener, 2, is a single-molecule
magnet displaying slow magnetic relaxation under the application of
a static dc field
Exchange Coupling and Magnetic Blocking in Bipyrimidyl Radical-Bridged Dilanthanide Complexes
The synthesis and magnetic properties of three new bipyrimidyl
radical-bridged dilanthanide complexes, [(Cp*<sub>2</sub>Ln)<sub>2</sub>(μ-bpym<sup>•</sup>)]<sup>+</sup> (Ln = Gd, Tb, Dy),
are reported. Strong Ln<sup>III</sup>-bpym<sup>•–</sup> exchange coupling is observed for all species, as indicated by the
increases in χ<sub>M</sub><i>T</i> at low temperatures.
For the Gd<sup>III</sup>-containing complex, a fit to the data reveals
antiferromagnetic coupling with <i>J</i> = −10 cm<sup>–1</sup> to give an <i>S</i> = <sup>13</sup>/<sub>2</sub> ground state. The Tb<sup>III</sup> and Dy<sup>III</sup> congeners
show single-molecule magnet behavior with relaxation barriers of <i>U</i><sub>eff</sub> = 44(2) and 87.8(3) cm<sup>–1</sup>, respectively, a consequence of the large magnetic anisotropies
imparted by these ions. Significantly, the latter complex exhibits
a divergence of the field-cooled and zero-field-cooled dc susceptibility
data at 6.5 K and magnetic hysteresis below this temperature
Exchange Coupling and Magnetic Blocking in Bipyrimidyl Radical-Bridged Dilanthanide Complexes
The synthesis and magnetic properties of three new bipyrimidyl
radical-bridged dilanthanide complexes, [(Cp*<sub>2</sub>Ln)<sub>2</sub>(μ-bpym<sup>•</sup>)]<sup>+</sup> (Ln = Gd, Tb, Dy),
are reported. Strong Ln<sup>III</sup>-bpym<sup>•–</sup> exchange coupling is observed for all species, as indicated by the
increases in χ<sub>M</sub><i>T</i> at low temperatures.
For the Gd<sup>III</sup>-containing complex, a fit to the data reveals
antiferromagnetic coupling with <i>J</i> = −10 cm<sup>–1</sup> to give an <i>S</i> = <sup>13</sup>/<sub>2</sub> ground state. The Tb<sup>III</sup> and Dy<sup>III</sup> congeners
show single-molecule magnet behavior with relaxation barriers of <i>U</i><sub>eff</sub> = 44(2) and 87.8(3) cm<sup>–1</sup>, respectively, a consequence of the large magnetic anisotropies
imparted by these ions. Significantly, the latter complex exhibits
a divergence of the field-cooled and zero-field-cooled dc susceptibility
data at 6.5 K and magnetic hysteresis below this temperature
Exchange Coupling and Magnetic Blocking in Bipyrimidyl Radical-Bridged Dilanthanide Complexes
The synthesis and magnetic properties of three new bipyrimidyl
radical-bridged dilanthanide complexes, [(Cp*<sub>2</sub>Ln)<sub>2</sub>(μ-bpym<sup>•</sup>)]<sup>+</sup> (Ln = Gd, Tb, Dy),
are reported. Strong Ln<sup>III</sup>-bpym<sup>•–</sup> exchange coupling is observed for all species, as indicated by the
increases in χ<sub>M</sub><i>T</i> at low temperatures.
For the Gd<sup>III</sup>-containing complex, a fit to the data reveals
antiferromagnetic coupling with <i>J</i> = −10 cm<sup>–1</sup> to give an <i>S</i> = <sup>13</sup>/<sub>2</sub> ground state. The Tb<sup>III</sup> and Dy<sup>III</sup> congeners
show single-molecule magnet behavior with relaxation barriers of <i>U</i><sub>eff</sub> = 44(2) and 87.8(3) cm<sup>–1</sup>, respectively, a consequence of the large magnetic anisotropies
imparted by these ions. Significantly, the latter complex exhibits
a divergence of the field-cooled and zero-field-cooled dc susceptibility
data at 6.5 K and magnetic hysteresis below this temperature
Exchange Coupling and Magnetic Blocking in Bipyrimidyl Radical-Bridged Dilanthanide Complexes
The synthesis and magnetic properties of three new bipyrimidyl
radical-bridged dilanthanide complexes, [(Cp*<sub>2</sub>Ln)<sub>2</sub>(μ-bpym<sup>•</sup>)]<sup>+</sup> (Ln = Gd, Tb, Dy),
are reported. Strong Ln<sup>III</sup>-bpym<sup>•–</sup> exchange coupling is observed for all species, as indicated by the
increases in χ<sub>M</sub><i>T</i> at low temperatures.
For the Gd<sup>III</sup>-containing complex, a fit to the data reveals
antiferromagnetic coupling with <i>J</i> = −10 cm<sup>–1</sup> to give an <i>S</i> = <sup>13</sup>/<sub>2</sub> ground state. The Tb<sup>III</sup> and Dy<sup>III</sup> congeners
show single-molecule magnet behavior with relaxation barriers of <i>U</i><sub>eff</sub> = 44(2) and 87.8(3) cm<sup>–1</sup>, respectively, a consequence of the large magnetic anisotropies
imparted by these ions. Significantly, the latter complex exhibits
a divergence of the field-cooled and zero-field-cooled dc susceptibility
data at 6.5 K and magnetic hysteresis below this temperature
Taming Super-Reduced Bi<sub>2</sub><sup>3–</sup> Radicals with Rare Earth Cations
Here, we report the synthesis of two new sets of dibismuth-bridged
rare earth molecules. The first series contains a bridging diamagnetic
Bi22– anion, (Cp*2RE)2(μ-η2:η2-Bi2), 1-RE (where Cp* = pentamethylcyclopentadienyl; RE
= Gd (1-Gd), Tb (1-Tb), Dy (1-Dy), Y (1-Y)), while the second series comprises the first
Bi23– radical-containing complexes for
any d- or f-block metal ions, [K(crypt-222)][(Cp*2RE)2(μ-η2:η2-Bi2•)]·2THF (2-RE, RE = Gd (2-Gd), Tb (2-Tb), Dy (2-Dy), Y (2-Y); crypt-222 = 2.2.2-cryptand), which were obtained from
one-electron reduction of 1-RE with KC8. The
Bi23– radical-bridged terbium and dysprosium
congeners, 2-Tb and 2-Dy, are single-molecule
magnets with magnetic hysteresis. We investigate the nature of the
unprecedented lanthanide–bismuth and bismuth–bismuth
bonding and their roles in magnetic communication between paramagnetic
metal centers, through single-crystal X-ray diffraction, ultraviolet–visible/near-infrared
(UV–vis/NIR) spectroscopy, SQUID magnetometry, DFT and multiconfigurational
ab initio calculations. We find a πz* ground SOMO for Bi23–, which has isotropic spin–spin
exchange coupling with neighboring metal ions of ca. −20 cm–1; however, the exchange coupling is strongly augmented
by orbitally dependent terms in the anisotropic cases of 2-Tb and 2-Dy. As the first examples of p-block radicals
beneath the second row bridging any metal ions, these studies have
important ramifications for single-molecule magnetism, main group
element, rare earth metal, and coordination chemistry at large
Slow Magnetic Relaxation in a Dysprosium Ammonia Metallocene Complex
We report the serendipitous
discovery and magnetic characterization of a dysprosium bisÂ(ammonia)
metallocene complex, [(C<sub>5</sub>Me<sub>5</sub>)<sub>2</sub>DyÂ(NH<sub>3</sub>)<sub>2</sub>]Â(BPh<sub>4</sub>) (<b>1</b>), isolated
in the course of performing a well-established synthesis of the unsolvated
cationic complex [(C<sub>5</sub>Me<sub>5</sub>)<sub>2</sub>Dy]Â[(μ-Ph)<sub>2</sub>BPh<sub>2</sub>]. While side reactivity studies suggest that
this bisÂ(ammonia) species owes its initial incidence to impurities
in the DyCl<sub>3</sub>(H<sub>2</sub>O)<sub><i>x</i></sub> starting material, we were able to independently prepare <b>1</b> and its tetrahydrofuran (THF) derivative, [(C<sub>5</sub>Me<sub>5</sub>)<sub>2</sub>DyÂ(NH<sub>3</sub>)Â(THF)]Â(BPh<sub>4</sub>) (<b>2</b>), from the reaction of [(C<sub>5</sub>Me<sub>5</sub>)<sub>2</sub>Dy]Â[(μ-Ph)<sub>2</sub>BPh<sub>2</sub>] with ammonia
in THF. The low-symmetry complex <b>1</b> exhibits slow magnetic
relaxation under zero applied direct-current (dc) field to temperatures
as high as 46 K and notably exhibits an effective barrier to magnetic
relaxation that is more than 150% greater than that previously reported
for the [(C<sub>5</sub>Me<sub>5</sub>)<sub>2</sub>Ln]Â[(μ-Ph)<sub>2</sub>BPh<sub>2</sub>] precursor. On the basis of fitting of the
temperature-dependent relaxation data, magnetic relaxation is found
to occur via Orbach, Raman, and quantum-tunneling relaxation processes,
and the latter process can be suppressed by the application of a 1400
Oe dc field. Field-cooled and zero-field-cooled dc magnetic susceptibility
measurements reveal a divergence at 4 K indicative of magnetic blocking,
and magnetic hysteresis was observed up to 5.2 K. These results illustrate
the surprises and advantages that the lanthanides continue to offer
for synthetic chemists and magnetochemists alike
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Solubility of Nanocrystalline Cerium Dioxide: Experimental Data and Thermodynamic Modeling
Ultrafine
5 nm ceria isotropic nanoparticles were prepared using
the rapid chemical precipitation approach from ceriumÂ(III) nitrate
and ammonium hydroxide aqueous solutions. The as-prepared nanoparticles
were shown to contain predominantly CeÂ(IV) species. The solubility
of nanocrystalline CeO<sub>2</sub> at several pH values was determined
using ICP-MS and radioactive tracer methods. Phase composition of
the ceria samples remained unchanged upon partial dissolution, while
the shape of the particles changed dramatically, yielding nanorods
under neutral pH conditions. According to X-ray absorption spectroscopy
investigation of the supernatant, CeÂ(III) was the main cerium species
in solution at pH < 4. Based on the results obtained, a reductive
dissolution model was used for data interpretation. According to this
model, the solubility product for ceria nanoparticles was determined
to be log <i>K</i><sub>sp</sub> = −59.3 ± 0.3
in 0.01 M NaClO<sub>4</sub>. Taken together, our results show that
the pH dependence of ceria anti- and pro-oxidant activity can be related
to the dissolution of CeO<sub>2</sub> in aqueous media
Extraction of Lanthanide and Actinide Ions from Aqueous Mixtures Using a Carboxylic Acid-Functionalized Porous Aromatic Framework
Porous aromatic frameworks
(PAFs) incorporating a high concentration
of acid functional groups possess characteristics that are promising
for use in separating lanthanide and actinide metal ions, as required
in the treatment of radioactive waste. These materials have been shown
to be indefinitely stable to concentrated acids and bases, potentially
allowing for multiple adsorption/stripping cycles. Additionally, the
PAFs combine exceptional features from MOFs and inorganic/activated
carbons giving rise to tunable pore surfaces and maximum chemical
stability. Herein, we present a study of the adsorption of selected
metal ions, Sr<sup>2+</sup>, Fe<sup>3+</sup>, Nd<sup>3+</sup>, and
Am<sup>3+</sup>, from aqueous solutions employing a carbon-based porous
aromatic framework, BPP-7 (Berkeley Porous Polymer-7). This material
displays high metal loading capacities together with excellent adsorption
selectivity for neodymium over strontium based on Langmuir adsorption
isotherms and ideal adsorbed solution theory (IAST) calculations.
Based in part upon X-ray absorption spectroscopy studies, the stronger
adsorption of neodymium is attributed to multiple metal ion and binding
site interactions resulting from the densely functionalized and highly
interpenetrated structure of BPP-7. Recyclability and combustibility
experiments demonstrate that multiple adsorption/stripping cycles
can be completed with minimal degradation of the polymer adsorption
capacity