15 research outputs found
An efficient one-pot synthesis of carbazole fused benzoquinolines and pyridocarbazoles
CobaltĀ(II),
in the presence of acetate and nitrate, quantitatively
adds to the manganeseācobalt oxido cubane Mn<sup>IV</sup>Co<sup>III</sup><sub>3</sub>O<sub>4</sub>(OAc)<sub>5</sub>(py)<sub>3</sub> (<b>1</b>) to furnish the pentametallic dangler complex Mn<sup>IV</sup>Co<sup>III</sup><sub>3</sub>Co<sup>II</sup>O<sub>4</sub>(OAc)<sub>6</sub>(NO<sub>3</sub>)Ā(py)<sub>3</sub> (<b>2</b>). Complex <b>2</b> is structurally reminiscent of photosystem IIās oxygen-evolving
center, and is a rare example of a transition-metal ādanglerā
complex. Superconducting quantum interference device magnetometry
and density functional theory calculations characterize <b>2</b> as having an <i>S</i> = 0 ground state arising from antiferromagnetic
coupling between the Co<sup>II</sup> and Mn<sup>IV</sup> ions. At
higher temperatures, an uncoupled state dominates. The voltammogram
of <b>2</b> has four electrochemical events, two more than that
of its parent cubane <b>1</b>, suggesting that addition of the
dangler increases available redox states. Structural, electrochemical,
and magnetic comparisons of complexes <b>1</b> and <b>2</b> allow a better understanding of the danglerās influence on
a cubane
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Synthesis and O<sub>2</sub> Reactivity of a Titanium(III) MetalāOrganic Framework
Metalāorganic frameworks featuring
pores lined with exposed metal cations have received attention for
a wide range of adsorption-related applications. While many frameworks
with coordinatively unsaturated M<sup>II</sup> centers have been reported,
there are relatively few examples of porous materials with coordinatively
unsaturated M<sup>III</sup> centers. Here, we report the synthesis
and characterization of Ti<sub>3</sub>OĀ(OEt)Ā(bdc)<sub>3</sub>(solv)<sub>2</sub> (Ti-MIL-101; bdc<sup>2ā</sup> = 1,4-benzenedicarboxylate;
solv = <i>N</i>,<i>N</i>-dimethylformamide, tetrahydrofuran),
the first metalāorganic framework containing exclusively Ti<sup>III</sup> centers. Through a combination of gas adsorption, X-ray
diffraction, magnetic susceptibility, and electronic and vibrational
spectroscopy measurements, this high-surface-area framework is shown
to contain five-coordinate Ti<sup>III</sup> centers upon desolvation,
which irreversibly bind O<sub>2</sub> to form titaniumĀ(IV) superoxo
and peroxo species. Electronic absorption spectra suggest that the
five-coordinate Ti<sup>III</sup> sites adopt a distorted trigonal-bipyramidal
geometry that effectively shields nuclear charge and inhibits strong
adsorption of nonredox-active gases
Utility of Lithium in Rare-Earth Metal Reduction Reactions to Form Nontraditional Ln<sup>2+</sup> Complexes and Unusual [Li(2.2.2-cryptand)]<sup>1+</sup> Cations
The
utility of lithium compared to other alkali metals in generating Ln<sup>2+</sup> rare-earth metal complexes via reduction of Ln<sup>3+</sup> precursors in reactions abbreviated as LnA<sub>3</sub>/M (Ln = rare-earth
metal; A = anionic ligand; M = alkali metal) is described. Lithium
reduction of Cpā²<sub>3</sub>Ln (Cpā² = C<sub>5</sub>H<sub>4</sub>SiMe<sub>3</sub>; Ln = Y, Tb, Dy, Ho) under Ar in the presence
of 2.2.2-cryptand (crypt) forms new examples of crystallographically
characterizable Ln<sup>2+</sup> complexes of these metals, [LiĀ(crypt)]Ā[Cpā²<sub>3</sub>Ln]. In each complex, lithium is found in an N<sub>2</sub>O<sub>4</sub> donor atom coordination geometry that is unusual for
the cryptand ligand. Magnetic susceptibility data on these new examples
of nontraditional divalent lanthanide complexes are consistent with
4f<sup><i>n</i></sup>5d<sup>1</sup> electronic configurations.
The Dy and Ho complexes have exceptionally high single-ion magnetic
moments, 11.35 and 11.67 Ī¼<sub>B</sub>, respectively. Lithium
reduction of Cpā²<sub>3</sub>Y under N<sub>2</sub> at ā35
Ā°C forms the Y<sup>2+</sup> complex (Cpā²<sub>3</sub>Y)<sup>1ā</sup>, which reduces dinitrogen upon warming to room temperature
to generate the (N<sub>2</sub>)<sup>2ā</sup> complex [Cpā²<sub>2</sub>YĀ(THF)]<sub>2</sub>(Ī¼-Ī·<sup>2</sup>:Ī·<sup>2</sup>-N<sub>2</sub>). These results provide insight on the factors
that lead to reduced dinitrogen complexes and/or stable divalent lanthanide
complexes as a function of the specific reducing agent and conditions
Trimethylsilyl versus Bis(trimethylsilyl) Substitution in Tris(cyclopentadienyl) Complexes of La, Ce, and Pr: Comparison of Structure, Magnetic Properties, and Reactivity
To
evaluate the effect of cyclopentadienyl ligand substitution
in complexes of new +2 ions of the lanthanides, comparisons in reactivity
and spectroscopic and magnetic properties have been made between [KĀ(crypt)]Ā[Cpā²<sub>3</sub>Ln], <b>1-Ln</b> (Cpā² = C<sub>5</sub>H<sub>4</sub>SiMe<sub>3</sub>; crypt = 2.2.2-cryptand; Ln = La, Ce, Pr, and Nd),
and [KĀ(crypt)]Ā[Cpā²ā²<sub>3</sub>Ln], <b>2-Ln</b> [Cpā²ā² = C<sub>5</sub>H<sub>3</sub>(SiMe<sub>3</sub>)<sub>2</sub>]. The <b>2-Ln</b> complexes (Ce, Pr, and Nd)
were synthesized by reduction of Cpā²ā²<sub>3</sub>Ln
with potassium graphite in the presence of crypt and crystallographically
characterized. The structures and UVāvisible spectra of <b>2-Ln</b> are similar to those of <b>1-Ln</b>, as expected,
but greater thermal stability for <b>2-Ln</b>, expected from
comparisons of <b>2-U</b> and <b>1-U</b>, was not observed.
The magnetic susceptibilities of <b>2-Ce</b> and <b>2-Pr</b> were investigated because those of <b>1-Ce</b> and <b>1-Pr</b> did not match simple coupling models for 4f<sup><i>n</i></sup>5d<sup>1</sup> electron configurations. The magnetic data of
the <b>2-Ln</b> complexes are similar to those of <b>1-Ln</b>, which suggests that Ce<sup>2+</sup> and Pr<sup>2+</sup> complexes
with 4f<sup><i>n</i></sup>5d<sup>1</sup> electron configurations
may have more complex electronic structures compared to nontraditional
divalent complexes of the later lanthanides. Reactivity studies of
isolated samples of <b>1-Ln</b> and <b>2-Ln</b> with 1,2-dimethoxyethane
(DME) were conducted to determine if methoxide products, found in
previous <i>in situ</i> studies of the synthesis of <b>2-Ln</b> by Lappert and co-workers, would form. Methoxide products
were not observed, which shows that the chemistry of the isolated
complexes differs from that of the <i>in situ</i> reduction
reactions
Electronic Conductivity, Ferrimagnetic Ordering, and Reductive Insertion Mediated by Organic Mixed-Valence in a Ferric Semiquinoid MetalāOrganic Framework
A three-dimensional
network solid composed of Fe<sup>III</sup> centers
and paraĀmagnetic semiĀquinoid linkers, (NBu<sub>4</sub>)<sub>2</sub>ĀFe<sup>III</sup><sub>2</sub>Ā(dhbq)<sub>3</sub> (dhbq<sup>2ā/3ā</sup> = 2,5-dioxidoĀbenzoĀquinone/ā1,2-dioxido-4,5-semiĀquinone),
is shown to exhibit a conductivity of 0.16 Ā± 0.01 S/cm at 298
K, one of the highest values yet observed for a metalāorganic
framework (MOF). The origin of this electronic conductivity is determined
to be ligand mixed-valency, which is characterized using a suite of
spectroĀscopic techniques, slow-scan cyclic voltammetry, and
variable-temperature conductivity and magnetic susceptibility measurements.
Importantly, UVāvisāNIR diffuse reflectance measurements
reveal the first observation of RobināDay Class II/III mixed
valency in a MOF. Pursuit of stoichioĀmetric control over the
ligand redox states resulted in synthesis of the reduced frameĀwork
material Na<sub>0.9</sub>Ā(NBu<sub>4</sub>)<sub>1.8</sub>Fe<sup>III</sup><sub>2</sub>(dhbq)<sub>3</sub>. Differences in electronic
conductivity and magnetic ordering temperature between the two compounds
are investigated and correlated to the relative ratio of the two different
ligand redox states. Overall, the transition metalāsemiĀquinoid
system is established as a particularly promising scaffold for achieving
tunable long-range electronic communication in MOFs
Electronic Conductivity, Ferrimagnetic Ordering, and Reductive Insertion Mediated by Organic Mixed-Valence in a Ferric Semiquinoid MetalāOrganic Framework
A three-dimensional
network solid composed of Fe<sup>III</sup> centers
and paraĀmagnetic semiĀquinoid linkers, (NBu<sub>4</sub>)<sub>2</sub>ĀFe<sup>III</sup><sub>2</sub>Ā(dhbq)<sub>3</sub> (dhbq<sup>2ā/3ā</sup> = 2,5-dioxidoĀbenzoĀquinone/ā1,2-dioxido-4,5-semiĀquinone),
is shown to exhibit a conductivity of 0.16 Ā± 0.01 S/cm at 298
K, one of the highest values yet observed for a metalāorganic
framework (MOF). The origin of this electronic conductivity is determined
to be ligand mixed-valency, which is characterized using a suite of
spectroĀscopic techniques, slow-scan cyclic voltammetry, and
variable-temperature conductivity and magnetic susceptibility measurements.
Importantly, UVāvisāNIR diffuse reflectance measurements
reveal the first observation of RobināDay Class II/III mixed
valency in a MOF. Pursuit of stoichioĀmetric control over the
ligand redox states resulted in synthesis of the reduced frameĀwork
material Na<sub>0.9</sub>Ā(NBu<sub>4</sub>)<sub>1.8</sub>Fe<sup>III</sup><sub>2</sub>(dhbq)<sub>3</sub>. Differences in electronic
conductivity and magnetic ordering temperature between the two compounds
are investigated and correlated to the relative ratio of the two different
ligand redox states. Overall, the transition metalāsemiĀquinoid
system is established as a particularly promising scaffold for achieving
tunable long-range electronic communication in MOFs
Reversible CO Scavenging via Adsorbate-Dependent Spin State Transitions in an Iron(II)āTriazolate MetalāOrganic Framework
A new
metalāorganic framework, Fe-BTTri (Fe<sub>3</sub>[(Fe<sub>4</sub>Cl)<sub>3</sub>(BTTri)<sub>8</sub>]<sub>2</sub>Ā·18CH<sub>3</sub>OH, H<sub>3</sub>BTTri =1,3,5-trisĀ(1<i>H</i>-1,2,3-triazol-5-yl)Ābenzene)),
is found to be highly selective in the adsorption of CO over a variety
of other gas molecules, making it extremely effective, for example,
in the removal of trace CO from mixtures with H<sub>2</sub>, N<sub>2</sub>, and CH<sub>4</sub>. This framework not only displays significant
CO adsorption capacity at very low pressures (1.45 mmol/g at just
100 Ī¼bar), but, importantly, also exhibits readily reversible
CO binding. Fe-BTTri utilizes a unique spin state change mechanism
to bind CO in which the coordinatively unsaturated, high-spin Fe<sup>II</sup> centers of the framework convert to octahedral, low-spin
Fe<sup>II</sup> centers upon CO coordination. Desorption of CO converts
the Fe<sup>II</sup> sites back to a high-spin ground state, enabling
the facile regeneration and recyclability of the material. This spin
state change is supported by characterization via infrared spectroscopy,
single crystal X-ray analysis, MoĢssbauer spectroscopy, and
magnetic susceptibility measurements. Importantly, the spin state
change is selective for CO and is not observed in the presence of
other gases, such as H<sub>2</sub>, N<sub>2</sub>, CO<sub>2</sub>,
CH<sub>4</sub>, or other hydrocarbons, resulting in unprecedentedly
high selectivities for CO adsorption for use in CO/H<sub>2</sub>,
CO/N<sub>2</sub>, and CO/CH<sub>4</sub> separations and in preferential
CO adsorption over typical strongly adsorbing gases like CO<sub>2</sub> and ethylene. While adsorbate-induced spin state transitions are
well-known in molecular chemistry, particularly for CO, to our knowledge
this is the first time such behavior has been observed in a porous
material suitable for use in a gas separation process. Potentially,
this effect can be extended to selective separations involving other
Ļ-acids
Selective, Tunable O<sub>2</sub> Binding in Cobalt(II)āTriazolate/Pyrazolate MetalāOrganic Frameworks
The air-free reaction of CoCl<sub>2</sub> with 1,3,5-triĀ(1<i>H</i>-1,2,3-triazol-5-yl)Ābenzene
(H<sub>3</sub>BTTri) in <i>N</i>,<i>N</i>-dimethylformamide
(DMF) and methanol
leads to the formation of Co-BTTri (Co<sub>3</sub>[(Co<sub>4</sub>Cl)<sub>3</sub>(BTTri)<sub>8</sub>]<sub>2</sub>Ā·DMF), a sodalite-type
metalāorganic framework. Desolvation of this material generates
coordinatively unsaturated low-spin cobaltĀ(II) centers that exhibit
a strong preference for binding O<sub>2</sub> over N<sub>2</sub>,
with isosteric heats of adsorption (<i>Q</i><sub>st</sub>) of ā34(1) and ā12(1) kJ/mol, respectively. The low-spin
(<i>S</i> = 1/2) electronic configuration of the metal centers
in the desolvated framework is supported by structural, magnetic susceptibility,
and computational studies. A single-crystal X-ray structure determination
reveals that O<sub>2</sub> binds end-on to each framework cobalt center
in a 1:1 ratio with a CoāO<sub>2</sub> bond distance of 1.973(6)
Ć
. Replacement of one of the triazolate linkers with a more electron-donating
pyrazolate group leads to the isostructural framework Co-BDTriP (Co<sub>3</sub>[(Co<sub>4</sub>Cl)<sub>3</sub>(BDTriP)<sub>8</sub>]<sub>2</sub>Ā·DMF; H<sub>3</sub>BDTriP = 5,5ā²-(5-(1<i>H</i>-pyrazol-4-yl)-1,3-phenylene)ĀbisĀ(1<i>H</i>-1,2,3-triazole)),
which demonstrates markedly higher yet still fully reversible O<sub>2</sub> affinities (<i>Q</i><sub>st</sub> = ā47(1)
kJ/mol at low loadings). Electronic structure calculations suggest
that the O<sub>2</sub> adducts in Co-BTTri are best described as cobaltĀ(II)ādioxygen
species with partial electron transfer, while the stronger binding
sites in Co-BDTriP form cobaltĀ(III)āsuperoxo moieties. The
stability, selectivity, and high O<sub>2</sub> adsorption capacity
of these materials render them promising new adsorbents for air separation
processes
Structural and Electronic Effects on the Properties of Fe<sub>2</sub>(dobdc) upon Oxidation with N<sub>2</sub>O
We report electronic,
vibrational, and magnetic properties, together with their structural
dependences, for the metalāorganic framework Fe<sub>2</sub>(dobdc) (dobdc<sup>4ā</sup> = 2,5-dioxido-1,4-benzenedicarboxylate)
and its derivatives, Fe<sub>2</sub>(O)<sub>2</sub>(dobdc) and Fe<sub>2</sub>(OH)<sub>2</sub>(dobdc)īøspecies arising in the previously
proposed mechanism for the oxidation of ethane to ethanol using N<sub>2</sub>O as an oxidant. Magnetic susceptibility measurements reported
for Fe<sub>2</sub>(dobdc) in an earlier study and reported in the
current study for Fe<sup>II</sup><sub>0.26</sub>[Fe<sup>III</sup>(OH)]<sub>1.74</sub>(dobdc)Ā(DMF)<sub>0.15</sub>(THF)<sub>0.22</sub>, which
is more simply referred to as Fe<sub>2</sub>(OH)<sub>2</sub>(dobdc),
were used to confirm the computational results. Theory was also compared
to experiment for infrared spectra and powder X-ray diffraction structures.
Structural and magnetic properties were computed by using KohnāSham
density functional theory both with periodic boundary conditions and
with cluster models. In addition, we studied the effects of different
treatments of the exchange interactions on the magnetic coupling parameters
by comparing several approaches to the exchange-correlation functional:
generalized gradient approximation (GGA), GGA with empirical Coulomb
and exchange integrals for 3<i>d</i> electrons (GGA+U),
nonseparable gradient approximation (NGA) with empirical Coulomb and
exchange integrals for 3<i>d</i> electrons (NGA+U), hybrid
GGA, meta-GGA, and hybrid meta-GGA. We found the coupling between
the metal centers along a chain to be ferromagnetic in the case of
Fe<sub>2</sub>(dobdc) and antiferromagnetic in the cases of Fe<sub>2</sub>(O)<sub>2</sub>(dobdc) and Fe<sub>2</sub>(OH)<sub>2</sub>(dobdc).
The shift in magnetic coupling behavior correlates with the changing
electronic structure of the framework, which derives from both structural
and electronic changes that occur upon metal oxidation and addition
of the charge-balancing oxo and hydroxo ligands
Charge Delocalization and Bulk Electronic Conductivity in the Mixed-Valence MetalāOrganic Framework Fe(1,2,3-triazolate)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub>
Metalāorganic
frameworks are of interest for use in a variety
of electrochemical and electronic applications, although a detailed
understanding of their charge transport behavior, which is of critical
importance for enhancing electronic conductivities, remains limited.
Herein, we report isolation of the mixed-valence framework materials,
FeĀ(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> (tri<sup>ā</sup> = 1,2,3-triazolate; <i>x</i> = 0.09, 0.22,
and 0.33), obtained from the stoichiometric chemical oxidation of
the poorly conductive ironĀ(II) framework FeĀ(tri)<sub>2</sub>, and
find that the conductivity increases dramatically with iron oxidation
level. Notably, the most oxidized variant, FeĀ(tri)<sub>2</sub>(BF<sub>4</sub>)<sub>0.33</sub>, displays a room-temperature conductivity
of 0.3(1) S/cm, which represents an increase of 8 orders of magnitude
from that of the parent material and is one of the highest conductivity
values reported among three-dimensional metalāorganic frameworks.
Detailed characterization of FeĀ(tri)<sub>2</sub> and the FeĀ(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> materials via
powder X-ray diffraction, MoĢssbauer spectroscopy, and IR and
UVāvis-NIR diffuse reflectance spectroscopies reveals that
the high conductivity arises from intervalence charge transfer between
mixed-valence low-spin Fe<sup>II/III</sup> centers. Further, MoĢssbauer
spectroscopy indicates the presence of a valence-delocalized Fe<sup>II/III</sup> species in FeĀ(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> at 290 K, one of the first such observations for
a metalāorganic framework. The electronic structure of valence-pure
FeĀ(tri)<sub>2</sub> and the charge transport mechanism and electronic
structure of mixed-valence FeĀ(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> frameworks are discussed in detail