16 research outputs found
A PolyoxometalateāCyanometalate Multilayered Coordination Network
The reaction of the Īµ-Keggin polyoxometalate (POM)
[PMo<sub>12</sub>O<sub>36</sub>(OH)<sub>4</sub>{LaĀ(H<sub>2</sub>O)<sub>4</sub>}<sub>4</sub>]<sup>5+</sup> with Fe<sup>II</sup>(CN)<sub>6</sub><sup>4ā</sup> under typical bench conditions at room temperature
and ambient pressure has afforded the novel [Īµ-PMo<sub>12</sub>O<sub>37</sub>(OH)<sub>3</sub>{LaĀ(H<sub>2</sub>O)<sub>5</sub>(FeĀ(CN)<sub>6</sub>)<sub>0.25</sub>}<sub>4</sub>] network, which exhibits a three-dimensional
multilayered structure. The compound has been fully characterized
by synchrotron-radiation X-ray crystallography, IR spectroscopy, elemental
analysis, and thermogravimetric analysis. This coordination network
constitutes the first example of a cyanometalate bonded to a POM unit
High Thermal Durability of Water-Free Copper-Octacyanotungsten-Based Magnets Containing Halogen Bonds
Two-dimensional (2-D) cyano-bridged CuāW bimetallic assemblies that include halogen-substituted pyridine molecules, [Cu<sup>II</sup>(3-iodopyridine)<sub>4</sub>][Cu<sup>II</sup>(3-iodopyridine)<sub>2</sub>]<sub>2</sub>[W<sup>V</sup>(CN)<sub>8</sub>]<sub>2</sub> (<b>1</b>) (triclinic crystal structure, <i>P</i>1Ģ
space group), [Cu<sup>II</sup>(3-bromopyridine)<sub>4</sub>][Cu<sup>II</sup>(3-bromopyridine)<sub>2</sub>]<sub>2</sub>[W<sup>V</sup>(CN)<sub>8</sub>]<sub>2</sub> (<b>2</b>) (triclinic, <i>P</i>1Ģ
), and [Cu<sup>II</sup>(3-chloropyridine)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>][Cu<sup>II</sup>(3-chloropyridine)<sub>2</sub>]<sub>2</sub>[W<sup>V</sup>(CN)<sub>8</sub>]<sub>2</sub>Ā·4H<sub>2</sub>O (<b>3</b>) (monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i>), were synthesized. Thermogravimetric measurements demonstrate that <b>1</b> and <b>2</b> have high thermal durability up to ca. 150 Ā°C (423 K) due to the lack of water molecules in the crystal and the stacked CuāW 2-D layers with halogen bonding between halogen-substituted pyridine and the cyano nitrogen of octacyanotungstate. In contrast, <b>3</b> exhibits weight loss above ca. 50 Ā°C (323 K) as the water molecules between the 2-D layers are removed upon heating. Magnetic measurements show that <b>1</b>ā<b>3</b> are ferromagnets due to parallel ordering of the magnetic spins on Cu<sup>II</sup> (<i>S</i> = 1/2) and W<sup>V</sup> (<i>S</i> = 1/2) with Curie temperatures (<i>T</i><sub>C</sub>) of 4.7 K (<b>1</b>), 5.2 K (<b>2</b>), and 7.2 K (<b>3</b>)
Green to Red Luminescence Switchable by Excitation Light in Cyanido-Bridged Tb<sup>III</sup>āW<sup>V</sup> Ferromagnet
Green to Red Luminescence Switchable by Excitation
Light in Cyanido-Bridged Tb<sup>III</sup>āW<sup>V</sup> Ferromagne
Chiral Ln<sup>III</sup>(tetramethylurea)ā[W<sup>V</sup>(CN)<sub>8</sub>] Coordination Chains Showing Slow Magnetic Relaxation
We
prepared a series of isostructural chiral cyanido-bridged zigzag
chains [LnĀ(tmu)<sub>5</sub>]Ā[WĀ(CN)<sub>8</sub>] (Ln = Gd, <b>1</b>; Tb, <b>2</b>; Dy, <b>3</b>; Ho, <b>4</b>; Er, <b>5</b>; Tm, <b>6</b>) using achiral tmu = tetramethylurea.
Their chiral character was confirmed with single crystal X-ray diffraction
and circular dichroism measurements. Magnetic studies show antiferromagnetic
interactions within cyanido-bridged Ln<sup>III</sup>āW<sup>V</sup> pairs, and interchain ordering of net spins in <b>1</b>, <b>4</b>, and <b>5</b>. It is worth to emphasize that
Dy-, Er-, and Tm-based systems combine magnetic field-induced slow
magnetic relaxation and chirality. Analysis of AC magnetic data with
two relaxation processes for <b>5</b> gives energy barrier Ī<sub>Ļ</sub>/<i>k</i><sub>B</sub> = 1.2(3) K and relaxation
time Ļ<sub>0</sub> = 2.63(8) Ć 10<sup>ā2</sup> s,
and Ī<sub>Ļ</sub>/<i>k</i><sub>B</sub> = 22(2)
K and Ļ<sub>0</sub> = 1.21(3) Ć 10<sup>ā8</sup> s.
ColeāCole function fits for <b>3</b> and <b>6</b> result in Ī<sub>Ļ</sub>/<i>k</i><sub>B</sub> = 17(1) K, Ļ<sub>0</sub> = 1.68(3) Ć 10<sup>ā6</sup> s and Ī<sub>Ļ</sub>/<i>k</i><sub>B</sub> =
5.7(3) K, Ļ<sub>0</sub> = 1.53(4) Ć 10<sup>ā2</sup> s, respectively. Slower relaxation processes have been assigned
to dipoleādipole interactions while faster ones to single ion
magnet behavior of LnĀ(III) ions
Supramolecular Two-Dimensional Network Mediated via Sulfurās ĻāHoles in a Conducting Molecular Crystal: Effects of Its Rigidity on Physical Properties and Structural Transition
This study reveals
that noncovalent intermolecular interactions
mediated by Ļ-holes on sulfur atoms can function as an efficient
tool to design and construct a novel supramolecular motif, and that
these noncovalent bonds are rigid enough to regulate the displacement
of molecules at the structural transition. A novel two-dimensional
cationĀ·Ā·Ā·anion supramolecular structure via sulfurās
Ļ-holes was constructed in a functional molecular crystal, (ethyl-4-bromothiazolium)<sub>2</sub>[PtĀ(mnt)<sub>2</sub>]<sub>3</sub> (mnt = maleonitriledithiolato).
The unit cell contained two crystallographically independent anions <b>A</b> and <b>B</b>. Electrostatic Ļ-hole bonds were
detected between Ļ-holes on sulfur in the cation and lone pairs
of āCN moieties in <b>B</b>, while <b>A</b> did
not form such SĀ·Ā·Ā·N Ļ-hole bonds. This salt exhibited
a structural transition at ca. 150 K, in which <b>B</b> did
not show apparent displacement, while <b>A</b> shifted along
the anionās stacking direction. This shift enhanced trimerization
of the anion in the low-temperature phase, leading to the enhanced
antiferromagnetic exchange interaction and the increased activation
energy in the electrical conduction. We showed that sulfur-based Ļ-hole
bonds are rigid enough to contribute to modulating the physical properties
through regulating the displacement of molecules in molecular materials
Synthesis and Characterization of BāHeterocyclic ĻāRadical and Its Reactivity as a Boryl Radical
The first isolation and full characterization of the
stable, persistent
diazaboracyclic neutral radical <b>3</b> is reported. Reduction
of base-stabilized difluororoborane <b>2</b> provided radical <b>3</b> as a neutral molecule having a planar sp<sup>2</sup> boron
atom attached to one fluorine and two nitrogen atoms. ESR spectroscopy
and DFT calculations indicated that the unpaired electron is delocalized
over the six-membered ring. Because of an electronic transition related
to the singly occupied molecular orbital, <b>3</b> has a characteristic
red color, as UVāvis spectroscopy showed an absorption maximum
at 498 nm. Although DFT calculations suggested that radical <b>3</b> has relatively low spin density on the boron atom in comparison
with the nitrogen and carbon atoms in the six-membered ring, <b>3</b> reacted as a base-stabilized boryl radical when treated
with benzoquinone or benzoyl peroxide
Cesium Cyano-Bridged Co<sup>II</sup>āM<sup>V</sup> (M = Mo and W) Layered Frameworks Exhibiting High Thermal Durability and Metamagnetism
Two-dimensional cesium bimetal cyano-bridged
assemblies Cs<sup>I</sup><sub>4</sub>Co<sup>II</sup>[Mo<sup>V</sup>(CN)<sub>8</sub>]ĀCl<sub>3</sub> (<b>CsCoMo</b>) and Cs<sup>I</sup><sub>4</sub>Co<sup>II</sup>[W<sup>V</sup>(CN)<sub>8</sub>]ĀCl<sub>3</sub> (<b>CsCoW</b>) were synthesized. The negatively charged
and solvent-free
{Co<sup>II</sup>[M<sup>V</sup>(CN)<sub>8</sub>]ĀCl<sub>3</sub>}<sup>4ā</sup> (M = Mo, W) coordination layers are separated by
Cs<sup>+</sup> ions. Themogravimetric measurements show that these
compounds reveal high thermal durability up to 523 K (250 Ā°C),
which is due to the absence of solvent molecules in their crystal
structures. The magnetic measurements show that <b>CsCoMo</b> and <b>CsCoW</b> are metamagnets showing the field-induced
transition from an antiferromagnetic phase with NeĢel temperature
of 25 K to a ferromagnetic phase, which is observed at high critical
magnetic field of 24 kOe at 1.8 K. These originate from antiferromagnetic
interactions between ferromagnetically coupled cyano-bridged Co<sup>II</sup>āM<sup>V</sup> layers, and the contribution from single-ion
anisotropy of Co<sup>II</sup>
Conjunction of Chirality and Slow Magnetic Relaxation in the Supramolecular Network Constructed of Crossed Cyano-Bridged Co<sup>II</sup>āW<sup>V</sup> Molecular Chains
The addition of chiral 2,2ā²-(2,6-pyridinediyl)ĀbisĀ(4-isopropyl-2-oxazoline)
(<i>i</i>Pr-Pybox) to a self-assembled Co<sup>II</sup>ā[W<sup>V</sup>(CN)<sub>8</sub>] magnetic system gives two enantiomorphic
cyano-bridged chains, {[Co<sup>II</sup>((<i>S</i>,<i>S</i>)-<i>i</i>Pr-Pybox)Ā(MeOH)]<sub>3</sub>[W<sup>V</sup>(CN)<sub>8</sub>]<sub>2</sub>Ā·ā5.5MeOHĀ·ā0.5H<sub>2</sub>O}<sub><i>n</i></sub> (<b>1</b>-<i>SS</i>) and {[Co<sup>II</sup>((<i>R</i>,<i>R</i>)-<i>i</i>Pr-Pybox) (MeOH)]<sub>3</sub>[W<sup>V</sup>(CN)<sub>8</sub>]<sub>2</sub>Ā·ā5.5MeOHĀ·ā0.5H<sub>2</sub>O}<sub><i>n</i></sub> (<b>1</b>-<i>RR</i>). Both
compounds crystallize with a structure containing a unique crossed
arrangement of one-dimensional chains that form a microporous supramolecular
network with large channels (14.9 Ć
Ć 15.1 Ć
Ć
15.3 Ć
) filled with methanol. The investigated materials exhibited
optical chirality, as confirmed by natural circular dichroism and
UVāvis absorption spectra. <b>1</b>-(<i>SS</i>) and <b>1</b>-(<i>RR</i>) are paramagnets with cyano-mediated
Co<sup>II</sup>āW<sup>V</sup> magnetic couplings that lead
to a specific spin arrangement with half of the W<sup>V</sup> ions
coupled ferromagnetically with their Co<sup>II</sup> neighbors and
the other half coupled antiferromagnetically. Significant magnetic
anisotropy with the easy axis along the [101] direction was confirmed
by single-crystal magnetic studies and can be explained by the single-ion
anisotropy of elongated octahedral Co<sup>II</sup> sites. Below 3
K, the frequency-dependent Ļ<sub>M</sub><sup>ā³</sup>(<i>T</i>) signal indicated
slow magnetic relaxation characteristic of single-chain magnets
Synthesis and Characterization of BāHeterocyclic ĻāRadical and Its Reactivity as a Boryl Radical
The first isolation and full characterization of the
stable, persistent
diazaboracyclic neutral radical <b>3</b> is reported. Reduction
of base-stabilized difluororoborane <b>2</b> provided radical <b>3</b> as a neutral molecule having a planar sp<sup>2</sup> boron
atom attached to one fluorine and two nitrogen atoms. ESR spectroscopy
and DFT calculations indicated that the unpaired electron is delocalized
over the six-membered ring. Because of an electronic transition related
to the singly occupied molecular orbital, <b>3</b> has a characteristic
red color, as UVāvis spectroscopy showed an absorption maximum
at 498 nm. Although DFT calculations suggested that radical <b>3</b> has relatively low spin density on the boron atom in comparison
with the nitrogen and carbon atoms in the six-membered ring, <b>3</b> reacted as a base-stabilized boryl radical when treated
with benzoquinone or benzoyl peroxide