17 research outputs found
Iodine Release and Recovery, Influence of Polyiodide Anions on Electrical Conductivity and Nonlinear Optical Activity in an Interdigitated and Interpenetrated Bipillared-Bilayer Metal–Organic Framework
{[Cu<sub>6</sub>(pybz)<sub>8</sub>(OH)<sub>2</sub>]·I<sub>5</sub><sup>–</sup>·I<sub>7</sub><sup>–</sup>}<sub><i>n</i></sub> (<b>1</b>), obtained hydrothermally by using
iodine molecules as a versatile precursor template, consists of a
cationic framework with two types of zigzag channels, which segregate
I<sub>5</sub><sup>–</sup> and I<sub>7</sub><sup>–</sup> anions. The framework exhibits the first observed bipillared-bilayer
structure featuring both interdigitation and interpenetration. <b>1</b> displays high framework stability in both acidic (HCl) and
alkaline (NaOH) solutions. <b>1</b> slowly releases iodine in
dry methanol to give [Cu<sub>6</sub>(pybz)<sub>8</sub>(OH)<sub>2</sub>]Â(I<sup>–</sup>)<sub>2</sub>·3.5CH<sub>3</sub>OH (<b>1</b>′) and partially recovers iodine from cyclohexane
to form [Cu<sub>6</sub>(pybz)<sub>8</sub>(OH)<sub>2</sub>]Â(I<sup>–</sup>)<sub>2</sub>·<i>x</i>I<sub>2</sub> (<b>1</b>″). Differences of up to 100 times in electrical conductivity
and of 4 times in nonlinear optical activity (NLO) have been measured
between <b>1</b> and <b>1</b>′. This compound is
one of few displaying multifunctionality, electrical conductivity,
NLO, and crystal–crystal stability upon release and recovery
of iodine. It is also unique in the iodine release from polyiodide
anions in a metal–organic framework
Iodine Release and Recovery, Influence of Polyiodide Anions on Electrical Conductivity and Nonlinear Optical Activity in an Interdigitated and Interpenetrated Bipillared-Bilayer Metal–Organic Framework
{[Cu<sub>6</sub>(pybz)<sub>8</sub>(OH)<sub>2</sub>]·I<sub>5</sub><sup>–</sup>·I<sub>7</sub><sup>–</sup>}<sub><i>n</i></sub> (<b>1</b>), obtained hydrothermally by using
iodine molecules as a versatile precursor template, consists of a
cationic framework with two types of zigzag channels, which segregate
I<sub>5</sub><sup>–</sup> and I<sub>7</sub><sup>–</sup> anions. The framework exhibits the first observed bipillared-bilayer
structure featuring both interdigitation and interpenetration. <b>1</b> displays high framework stability in both acidic (HCl) and
alkaline (NaOH) solutions. <b>1</b> slowly releases iodine in
dry methanol to give [Cu<sub>6</sub>(pybz)<sub>8</sub>(OH)<sub>2</sub>]Â(I<sup>–</sup>)<sub>2</sub>·3.5CH<sub>3</sub>OH (<b>1</b>′) and partially recovers iodine from cyclohexane
to form [Cu<sub>6</sub>(pybz)<sub>8</sub>(OH)<sub>2</sub>]Â(I<sup>–</sup>)<sub>2</sub>·<i>x</i>I<sub>2</sub> (<b>1</b>″). Differences of up to 100 times in electrical conductivity
and of 4 times in nonlinear optical activity (NLO) have been measured
between <b>1</b> and <b>1</b>′. This compound is
one of few displaying multifunctionality, electrical conductivity,
NLO, and crystal–crystal stability upon release and recovery
of iodine. It is also unique in the iodine release from polyiodide
anions in a metal–organic framework
Ligand Effect on the Single-Molecule Magnetism of Tetranuclear Co(II) Cubane
A clear dependence
on the ligand has been observed for the magnetic properties of a closely
related series of CoÂ(II) cubane structures, viz. [Co<sub>4</sub>(<i>mbm</i> or <i>bm</i>)<sub>4</sub>(ROH)<sub>4</sub>Br<sub>4</sub>] (<b>1-MeOH</b>, <b>1-EtOH</b>, <b>2-MeOH</b>, and <b>2-EtOH</b>, where <b>1</b> = [Co<sub>4</sub>(<i>mbm</i>)<sub>4</sub>Br<sub>4</sub>], <b>2</b> = [Co<sub>4</sub>(<i>bm</i>)<sub>4</sub>Br<sub>4</sub>], <i>bm</i> = (1<i>H</i>-benzoÂ[<i>d</i>]Âimidazol-2-yl)Âmethanolate. and <i>mbm</i> = 1-Me-<i>bm</i>.) The [Co<sub>4</sub>(OR)<sub>4</sub>] cubane core consists
of an octahedral Co<sup>II</sup> center chelated by the alkoxide oxygen
and imidazole nitrogen atoms from monoanionic <i>bm</i> or <i>mbm</i> and coordinated by methanol/alcohol and bromine. Interestingly,
electrospray ionization mass spectrometry (ESI-MS) indicates that <b>1-MeOH</b> and <b>2-MeOH</b> are unstable in methanol and
transformed to the butterfly [Co<sub>4</sub>L<sub>6</sub>]<sup>2+</sup> but that <b>1-EtOH</b> and <b>2-EtOH</b> are stable
in ethanol. Their magnetic susceptibilities suggest ferromagnetic
coupling between the nearest cobalt centers to give a theoretical <i>S</i> = 4 × 3/2 ground state with considerable magneto-crystalline
behavior. The packing and intermolecular interactions appear to influence
the geometry of the cubes and thus the anisotropy of cobalt, which
leads to different blocking temperatures (<i>T</i><sub>B</sub>). Consequently, the compounds with <i>mbm</i>, <b>1-MeOH</b> and <b>1-EtOH</b>, exhibit <i>T</i><sub>B</sub> >
2 K as shown by the relaxation of magnetization in zero applied dc
field where the barriers <i>U</i><sub>eff</sub>/<i>k</i><sub>B</sub> are respectively 27 and 21 K and relaxation
times are τ<sub>0</sub> = 1.3 × 10<sup>–9</sup> and
9.7 × 10<sup>–9</sup> s. However, the compounds with <i>bm</i>, <b>2-MeOH</b> and <b>2-EtOH</b>, remain
paramagnetic above 2 K and do not show nonlinear response of the ac
susceptibilities. These findings reaffirm the subtle dependence of
single-molecule magnetism on coordination geometry and intermolecular
interaction
A Porous 4‑Fold-Interpenetrated Chiral Framework Exhibiting Vapochromism, Single-Crystal-to-Single-Crystal Solvent Exchange, Gas Sorption, and a Poisoning Effect
The synthesis and characterization of a 4-fold-interpenetrated
pseudodiamond
metal–organic framework (MOF), Co<sup>II</sup>(pybz)<sub>2</sub>·2DMF [pybz = 4-(4-pyridyl)Âbenzoate], are reported. <i>N</i>,<i>N</i>-Dimethylformamide
(DMF) of the channels can be removed to give the porous framework,
and it can also be exchanged for methanol, ethanol, benzene, and cyclohexane.
It is a rare example of a stable MOF based on a single octahedral
building unit. The single-crystal structures of Co<sup>II</sup>(pybz)<sub>2</sub>·2DMF, Co<sup>II</sup>(pybz)<sub>2</sub>, Co<sup>II</sup>(pybz)<sub>2</sub>·4MeOH, and Co<sup>II</sup>(pybz)<sub>2</sub>·2.5EtOH have been successfully determined. In all of them,
the framework is marginally modified and contains a highly distorted
and strained octahedral node of cobalt with two pyridine nitrogen
atoms and two chelate carboxylate groups. In air, the crystals of
Co<sup>II</sup>(pybz)<sub>2</sub>·2DMF readily change color from
claret red to light pink. Thermogravimetric analysis and Raman spectroscopy
indicate a change in coordination, where the carboxylate becomes monodentate
and an additional two water molecules are coordinated to each cobalt
atom. In a dry solvent, this transformation does not take place. Tests
show that Co<sup>II</sup>(pybz)<sub>2</sub> may be a more efficient
drying agent than silica gel and anhydrous CuSO<sub>4</sub>. The desolvated
Co<sup>II</sup>(pybz)<sub>2</sub> can absorb several gases such as
CO<sub>2</sub>, N<sub>2</sub>, H<sub>2</sub>, and CH<sub>4</sub> and
also vapors of methanol, ethanol, benzene, and cyclohexane. If Co<sup>II</sup>(pybz)<sub>2</sub> is exposed to air and followed by reactivation,
its sorption capacity is considerably reduced, which we associate
with a poisoning effect. Because of the long distance between the
cobalt atoms in the structure, the magnetic properties are those of
a paramagnet
Porous Supramolecular Networks Constructed of One-Dimensional Metal–Organic Chains: Carbon Dioxide and Iodine Capture
In
search of porous materials for selective sorption and iodine inclusion,
we have found two networks made of chains with a kink at the metal
nodes held together by supramolecular interactions (H-bond and π···π
stacking). The solvent can be removed and replaced reversibly without
loss of crystallinity, as demonstrated by single-crystal-to-single-crystal
crystallography. In contrast, iodine uptake degrades the crystallinity
to amorphous, and it regains its crystalline state after removal of
the iodine at 200 °C. Slight differences in behavior of the sorption
and inclusion properties between the tetrahedral metal nodes, Zn and
Co, are associated with the size of the nodes. An important feature
is the extent of iodine that can be included between the chains that
is doubled with temperature from 30 to 100 °C and exceeds the
weight in mass of the compounds
Tracking the Formation of a Polynuclear Co<sub>16</sub> Complex and Its Elimination and Substitution Reactions by Mass Spectroscopy and Crystallography
We present the syntheses and structures
of the biggest chiral cobalt
coordination cluster, [Co<sub>16</sub>(L)<sub>4</sub>Â(H<sub>3</sub>L)<sub>8</sub>Â(N<sub>3</sub>)<sub>6</sub>]Â(NO<sub>3</sub>)<sub>2</sub>·​16H<sub>2</sub>O·​2CH<sub>3</sub>OH (<b>1</b>, where H<sub>4</sub>L = <i>S,S</i>-1,2-bisÂ(1<i>H</i>-benzÂimidazol-2-yl)-1,2-ethaneÂdiol). <b>1</b> consists of two Co<sub>4</sub>O<sub>4</sub> cubes (Co<sub>4</sub>(L)<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>) alternating
with Co<sub>2</sub>(EO-N<sub>3</sub>)<sub>2</sub>Co<sub>2</sub> (Co<sub>4</sub>(L)<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>Â(N<sub>3</sub>)<sub>2</sub>), bridged by the benzimidazole and azide nitrogen
atoms to form a twisted ring. The ligand adopts both <i>cis</i> and <i>trans</i> forms, and all the rings have the same
chiralilty. ESI-MS of <b>1</b> from a methanol solution of crystals
reveals the fragment [Co<sub>16</sub>(L)<sub>4</sub>Â(H<sub>3</sub>L)<sub>8</sub>Â(N<sub>3</sub>)<sub>6</sub>+2H]<sup>4+</sup>,
suggesting the polynuclear core is stable in solution. ESI-MS measurements
from the reaction solution found smaller fragments, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>–H]<sup>3+</sup>, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>–2H]<sup>2+</sup>, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>Â(N<sub>3</sub>)<sub>2</sub>]<sup>2+</sup>, and [Co<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>]<sup>2+</sup>, and ESI-MS from a methanol solution
of the solid deposit found in addition the Co<sub>16</sub> core. These
results and the dependence on the synthesis time allow us to propose
the process for the formation of <b>1</b>, which opens up a
new way for the direct observation of the ligand-controlled assembly
of clusters. In addition, the isolation of [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>]Â(NO<sub>3</sub>)<sub>4</sub>·​4H<sub>2</sub>O (<b>2</b>) consisting of separate Co<sub>4</sub>O<sub>4</sub> cubes with the ligands being only <i>cis</i> in
crystalline form supports the proposal. Interestingly, N<sub>3</sub><sup></sup> is replaced by either CH<sub>3</sub>O<sup>–</sup> or OH<sup>–</sup>, and this is the first time that high-resolution
ESI-MS is successfully utilized to examine both the step-by-step elimination
and substitution of inner bridging ligands in such a high nuclear
complex. Increasing the voltage results in stepwise elimination of
azide from the parent cluster. The preliminary magnetic susceptibility
of <b>1</b> indicates ferromagnetic cubes antiferromagnetically
coupled to the squares within the cluster, though in a field of 2.5
kOe, weak and slow relaxation is observed below 4 K
Tracking the Formation of a Polynuclear Co<sub>16</sub> Complex and Its Elimination and Substitution Reactions by Mass Spectroscopy and Crystallography
We present the syntheses and structures
of the biggest chiral cobalt
coordination cluster, [Co<sub>16</sub>(L)<sub>4</sub>Â(H<sub>3</sub>L)<sub>8</sub>Â(N<sub>3</sub>)<sub>6</sub>]Â(NO<sub>3</sub>)<sub>2</sub>·​16H<sub>2</sub>O·​2CH<sub>3</sub>OH (<b>1</b>, where H<sub>4</sub>L = <i>S,S</i>-1,2-bisÂ(1<i>H</i>-benzÂimidazol-2-yl)-1,2-ethaneÂdiol). <b>1</b> consists of two Co<sub>4</sub>O<sub>4</sub> cubes (Co<sub>4</sub>(L)<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>) alternating
with Co<sub>2</sub>(EO-N<sub>3</sub>)<sub>2</sub>Co<sub>2</sub> (Co<sub>4</sub>(L)<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>Â(N<sub>3</sub>)<sub>2</sub>), bridged by the benzimidazole and azide nitrogen
atoms to form a twisted ring. The ligand adopts both <i>cis</i> and <i>trans</i> forms, and all the rings have the same
chiralilty. ESI-MS of <b>1</b> from a methanol solution of crystals
reveals the fragment [Co<sub>16</sub>(L)<sub>4</sub>Â(H<sub>3</sub>L)<sub>8</sub>Â(N<sub>3</sub>)<sub>6</sub>+2H]<sup>4+</sup>,
suggesting the polynuclear core is stable in solution. ESI-MS measurements
from the reaction solution found smaller fragments, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>–H]<sup>3+</sup>, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>–2H]<sup>2+</sup>, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>Â(N<sub>3</sub>)<sub>2</sub>]<sup>2+</sup>, and [Co<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>]<sup>2+</sup>, and ESI-MS from a methanol solution
of the solid deposit found in addition the Co<sub>16</sub> core. These
results and the dependence on the synthesis time allow us to propose
the process for the formation of <b>1</b>, which opens up a
new way for the direct observation of the ligand-controlled assembly
of clusters. In addition, the isolation of [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>]Â(NO<sub>3</sub>)<sub>4</sub>·​4H<sub>2</sub>O (<b>2</b>) consisting of separate Co<sub>4</sub>O<sub>4</sub> cubes with the ligands being only <i>cis</i> in
crystalline form supports the proposal. Interestingly, N<sub>3</sub><sup></sup> is replaced by either CH<sub>3</sub>O<sup>–</sup> or OH<sup>–</sup>, and this is the first time that high-resolution
ESI-MS is successfully utilized to examine both the step-by-step elimination
and substitution of inner bridging ligands in such a high nuclear
complex. Increasing the voltage results in stepwise elimination of
azide from the parent cluster. The preliminary magnetic susceptibility
of <b>1</b> indicates ferromagnetic cubes antiferromagnetically
coupled to the squares within the cluster, though in a field of 2.5
kOe, weak and slow relaxation is observed below 4 K
A Porous 4‑Fold-Interpenetrated Chiral Framework Exhibiting Vapochromism, Single-Crystal-to-Single-Crystal Solvent Exchange, Gas Sorption, and a Poisoning Effect
The synthesis and characterization of a 4-fold-interpenetrated
pseudodiamond
metal–organic framework (MOF), Co<sup>II</sup>(pybz)<sub>2</sub>·2DMF [pybz = 4-(4-pyridyl)Âbenzoate], are reported. <i>N</i>,<i>N</i>-Dimethylformamide
(DMF) of the channels can be removed to give the porous framework,
and it can also be exchanged for methanol, ethanol, benzene, and cyclohexane.
It is a rare example of a stable MOF based on a single octahedral
building unit. The single-crystal structures of Co<sup>II</sup>(pybz)<sub>2</sub>·2DMF, Co<sup>II</sup>(pybz)<sub>2</sub>, Co<sup>II</sup>(pybz)<sub>2</sub>·4MeOH, and Co<sup>II</sup>(pybz)<sub>2</sub>·2.5EtOH have been successfully determined. In all of them,
the framework is marginally modified and contains a highly distorted
and strained octahedral node of cobalt with two pyridine nitrogen
atoms and two chelate carboxylate groups. In air, the crystals of
Co<sup>II</sup>(pybz)<sub>2</sub>·2DMF readily change color from
claret red to light pink. Thermogravimetric analysis and Raman spectroscopy
indicate a change in coordination, where the carboxylate becomes monodentate
and an additional two water molecules are coordinated to each cobalt
atom. In a dry solvent, this transformation does not take place. Tests
show that Co<sup>II</sup>(pybz)<sub>2</sub> may be a more efficient
drying agent than silica gel and anhydrous CuSO<sub>4</sub>. The desolvated
Co<sup>II</sup>(pybz)<sub>2</sub> can absorb several gases such as
CO<sub>2</sub>, N<sub>2</sub>, H<sub>2</sub>, and CH<sub>4</sub> and
also vapors of methanol, ethanol, benzene, and cyclohexane. If Co<sup>II</sup>(pybz)<sub>2</sub> is exposed to air and followed by reactivation,
its sorption capacity is considerably reduced, which we associate
with a poisoning effect. Because of the long distance between the
cobalt atoms in the structure, the magnetic properties are those of
a paramagnet
Tracking the Formation of a Polynuclear Co<sub>16</sub> Complex and Its Elimination and Substitution Reactions by Mass Spectroscopy and Crystallography
We present the syntheses and structures
of the biggest chiral cobalt
coordination cluster, [Co<sub>16</sub>(L)<sub>4</sub>Â(H<sub>3</sub>L)<sub>8</sub>Â(N<sub>3</sub>)<sub>6</sub>]Â(NO<sub>3</sub>)<sub>2</sub>·​16H<sub>2</sub>O·​2CH<sub>3</sub>OH (<b>1</b>, where H<sub>4</sub>L = <i>S,S</i>-1,2-bisÂ(1<i>H</i>-benzÂimidazol-2-yl)-1,2-ethaneÂdiol). <b>1</b> consists of two Co<sub>4</sub>O<sub>4</sub> cubes (Co<sub>4</sub>(L)<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>) alternating
with Co<sub>2</sub>(EO-N<sub>3</sub>)<sub>2</sub>Co<sub>2</sub> (Co<sub>4</sub>(L)<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>Â(N<sub>3</sub>)<sub>2</sub>), bridged by the benzimidazole and azide nitrogen
atoms to form a twisted ring. The ligand adopts both <i>cis</i> and <i>trans</i> forms, and all the rings have the same
chiralilty. ESI-MS of <b>1</b> from a methanol solution of crystals
reveals the fragment [Co<sub>16</sub>(L)<sub>4</sub>Â(H<sub>3</sub>L)<sub>8</sub>Â(N<sub>3</sub>)<sub>6</sub>+2H]<sup>4+</sup>,
suggesting the polynuclear core is stable in solution. ESI-MS measurements
from the reaction solution found smaller fragments, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>–H]<sup>3+</sup>, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>–2H]<sup>2+</sup>, [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>Â(N<sub>3</sub>)<sub>2</sub>]<sup>2+</sup>, and [Co<sub>2</sub>Â(H<sub>3</sub>L)<sub>2</sub>]<sup>2+</sup>, and ESI-MS from a methanol solution
of the solid deposit found in addition the Co<sub>16</sub> core. These
results and the dependence on the synthesis time allow us to propose
the process for the formation of <b>1</b>, which opens up a
new way for the direct observation of the ligand-controlled assembly
of clusters. In addition, the isolation of [Co<sub>4</sub>Â(H<sub>3</sub>L)<sub>4</sub>]Â(NO<sub>3</sub>)<sub>4</sub>·​4H<sub>2</sub>O (<b>2</b>) consisting of separate Co<sub>4</sub>O<sub>4</sub> cubes with the ligands being only <i>cis</i> in
crystalline form supports the proposal. Interestingly, N<sub>3</sub><sup></sup> is replaced by either CH<sub>3</sub>O<sup>–</sup> or OH<sup>–</sup>, and this is the first time that high-resolution
ESI-MS is successfully utilized to examine both the step-by-step elimination
and substitution of inner bridging ligands in such a high nuclear
complex. Increasing the voltage results in stepwise elimination of
azide from the parent cluster. The preliminary magnetic susceptibility
of <b>1</b> indicates ferromagnetic cubes antiferromagnetically
coupled to the squares within the cluster, though in a field of 2.5
kOe, weak and slow relaxation is observed below 4 K
Mn(II)-Based Porous Metal–Organic Framework Showing Metamagnetic Properties and High Hydrogen Adsorption at Low Pressure
A MnÂ(II)-based homometallic porous metal–organic
framework,
Mn<sub>5</sub>(btac)<sub>4</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(EtOH)<sub>2</sub>·DMF·3EtOH·3H<sub>2</sub>O (<b>1</b>, btac <b>=</b> benzotriazole-5-carboxylate), has been
solvothermally synthesized and structurally characterized by elemental
analysis, thermogravimetric analysis, and X-ray crystallographic study. <b>1</b> is a 3D neutral framework featuring 1D porous channels constructed
by {Mn–OH–Mn}<sub><i>n</i></sub> chains and
btac linkers. Magnetic studies show that <b>1</b> is a 3D metamagnet
containing 1D {Mn–OH–Mn}<sub><i>n</i></sub> ferrimagnetic chains. High-pressure H<sub>2</sub> adsorption measurement
at 77 K reveals that activated <b>1</b> can absorb 0.99 wt %
H<sub>2</sub> at 0.5 atm and reaches a maximum of 1.03 wt % at 5.5
atm. The steep H<sub>2</sub> absorption at lower pressure (98.2% of
the storage capacity at 0.5 atm) is higher than the corresponding
values of some MOFs (MIL-100 (16.1%), MOF-177 (57.1%), and MOF-5 (22.2%)).
Furthermore, activated <b>1</b> can adsorb CO<sub>2</sub> at
room temperature and 275 K. The adsorption enthalpy is 22.0 kJ mol<sup>–1</sup>, which reveals the high binding ability for CO<sub>2</sub>. Detailed gas sorption implies that the exposed MnÂ(II) coordination
sites in the activated <b>1</b> play an important role to improve
its adsorption capacities