10 research outputs found
Thermal Hysteresis in a Spin-Crossover Fe<sup>III</sup> Quinolylsalicylaldimine Complex, Fe<sup>III</sup>(5-Br-qsal)<sub>2</sub>Ni(dmit)<sub>2</sub>·solv: Solvent Effects
The
Fe<sup>III</sup> complexes Fe(5-Br-qsal)<sub>2</sub>Ni(dmit)<sub>2</sub>·solv with solv = CH<sub>2</sub>Cl<sub>2</sub> (<b>1</b>) and (CH<sub>3</sub>)<sub>2</sub>CO (<b>2</b>) were synthesized,
and their structural and magnetic properties were studied. While magnetization
and Mössbauer spectroscopy data of <b>1</b> showed a
gradual spin transition, compound <b>2</b> evidenced an abrupt
transition with a thermal hysteresis of 13 K close to room temperature
(<i>T</i><sub>1/2</sub> ↓ ∼273 K and <i>T</i><sub>1/2</sub> ↑ ∼286 K). A similar packing
arrangement of segregated layers of cations and anions was found for <b>1</b> and <b>2</b>. In both low-spin, LS, structures there
are a large number of short intra- and interchain contacts. This number
is lower in the high-spin, HS, phases, particularly in the case of <b>1</b>. The significant loss of strong π–π interactions
in the cationic chains and short contacts in the anionic chains in
the HS structure of <b>1</b> leads to alternating strong and
weak bonds between cations along the cationic chains and the formation
of unconnected dimers along the anionic chains. This is consistent
with a significant weakening of the extended interactions in <b>1</b>. On the other hand, in the HS phase of <b>2</b> the
3D dimensionality of the short contacts observed in the LS phases
is preserved. The effect of distinct solvent molecules on the intermolecular
spacings explains the different spin crossover behaviors of the title
compounds
[Fe(nsal<sub>2</sub>trien)]SCN, a New Two-Step Iron(III) Spin Crossover Compound, with Symmetry Breaking Spin-State Transition and an Intermediate Ordered State
We report the synthesis of the iron(III)
complex of the hexadentate Schiff base ligand nsal<sub>2</sub>trien
obtained from the condensation of triethylenetetramine and 2 equiv.
of 2-hydroxy-1-naphthaldehyde. The study of the salt [Fe(nsal<sub>2</sub>trien)]SCN (<b>1</b>) by magnetic susceptibility measurements
and Mössbauer spectroscopy reveals a rather unique behavior
that displays thermally induced spin crossover (SCO) with two well-separated
steps at 250 (gradual transition) and 142 K (steep transition). Single
crystal X-ray structures were obtained at 294, 150, and 50 K, for
the high spin (HS), intermediate (Int), and low spin (LS) phases.
The HS and LS phases are isostructural, and based on a single Fe<sup>III</sup> site (either HS or LS) an unusual symmetry break occurs
in the transition to the Int ordered phase, where the unit cell includes
two distinct Fe<sup>III</sup> sites and is based on a repetition of
the [HS–LS] motif. The two-step SCO behavior of <b>1</b> must result from the existence of structural constraints preventing
the full conversion HS ↔ LS in a single step
Hybrid Magnetic Superconductors Formed by TaS<sub>2</sub> Layers and Spin Crossover Complexes
The restacking of charged TaS<sub>2</sub> nanosheets with molecular counterparts has so far allowed
for the combination of superconductivity with a manifold of other
molecule-intrinsic properties. Yet, a hybrid compound that blends
superconductivity with spin crossover switching has still not been
reported. Here we continue to exploit the solid-state/molecule-based
hybrid approach for the synthesis of a layered TaS<sub>2</sub>-based
material that hosts Fe<sup>2+</sup> complexes with a spin switching
behavior. The chemical design and synthetic aspects of the exfoliation/restacking
approach are discussed, highlighting how the material can be conveniently
obtained in the form of highly oriented easy-to-handle flakes. Finally,
proof of the presence of both phenomena is provided by the use of
a variety of physical characterization techniques. The likely sensitivity
of the intercalated Fe<sup>2+</sup> complexes to external stimuli
such as light opens the door for the study of synergistic effects
between the superconductivity and the spin crossover switching at
low temperatures
Selective Carbon Dioxide Hydrogenation Driven by Ferromagnetic RuFe Nanoparticles in Ionic Liquids
CO<sub>2</sub> is selectively hydrogenated to HCO<sub>2</sub>H
or hydrocarbons (HCs) by RuFe nanoparticles (NPs) in ionic liquids
(ILs) under mild reaction conditions. The generation of HCO<sub>2</sub>H occurs in ILs containing basic anions, whereas heavy HCs (up to
C<sub>21</sub> at 150 °C) are formed in the presence of ILs containing
nonbasic anions. Remarkably, high values of TONs (400) and a TOF value
of 23.52 h<sup>–1</sup> for formic acid with a molar ratio
of 2.03 per BMI·OAc IL were obtained. Moreover, these NPs exhibited
outstanding abilities in the formation of long-chain HCs with efficient
catalytic activity (12% conversion) in a BMI·NTf<sub>2</sub> hydrophobic
IL. The IL forms a cage around the NPs that controls the diffusion/residence
time of the substrates, intermediates, and products. The distinct
CO<sub>2</sub> hydrogenation pathways (HCO<sub>2</sub>H or FT via
RWGS) catalyzed by the RuFe alloy are directly related to the basicity
and hydrophobicity of the IL ion pair (mainly imposed by the anion)
and the composition of the metal alloy. The presence of Fe in the
RuFe alloy provides enhanced catalytic performance via a metal dilution
effect for the formation of HCO<sub>2</sub>H and via a synergistic
effect for the generation of heavy HCs
Comparison of the performance of Skin Prick, ImmunoCAP, and ISAC tests in the diagnosis of patients with allergy
Background: Allergy is diagnosed from typical symptoms, and tests are performed to incriminate the suspected precipitant. Skin prick tests (SPTs) are commonly performed, inexpensive, and give immediate results. Laboratory tests (ImmunoCAP) for serum allergen-specific IgE antibodies are usually performed more selectively. The immuno-solid phase allergen chip (ISAC) enables testing for specific IgE against multiple allergen components in a multiplex assay. Methods: We retrospectively analysed clinic letters, case notes, and laboratory results of 118 patients attending the National Adult Allergy Service at the University Hospital of Wales who presented diagnostic difficulty, to evaluate which testing strategy (SPT, ImmunoCAP, or ISAC) was the most appropriate to use to confirm the diagnosis in these complex patients, evaluated in a “real-life” clinical service setting. Results: In patients with nut allergy, the detection rates of SPTs (56%) and ISAC (65%) were lower than those of ImmunoCAP (71%). ISAC had a higher detection rate (88%) than ImmunoCAP (69%) or SPT (33%) in the diagnosis of oral allergy syndrome. ImmunoCAP test results identified all 9 patients with anaphylaxis due to wheat allergy (100%), whereas ISAC was positive in only 6 of these 9 (67%). Conclusions: In this difficult diagnostic group, the ImmunoCAP test should be the preferred single test for possible allergy to nuts, wheat, other specific foods, and anaphylaxis of any cause. In these conditions, SPT and ISAC tests give comparable results. The most useful single test for oral allergy syndrome is ISAC, and SPT should be the preferred test for latex allergy
Stimuli Responsive Hybrid Magnets: Tuning the Photoinduced Spin-Crossover in Fe(III) Complexes Inserted into Layered Magnets
The
insertion of a [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complex
cation into a 2D oxalate network in the presence of different solvents
results in a family of hybrid magnets with coexistence of magnetic
ordering and photoinduced spin-crossover (LIESST effect) in compounds
[Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHCl<sub>3</sub> (<b>1·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHBr<sub>3</sub> (<b>1·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Br<sub>2</sub> (<b>1·CH</b><sub><b>2</b></sub><b>Br</b><sub><b>2</b></sub>). The three compounds crystallize in a 2D honeycomb anionic layer
formed by Mn<sup>II</sup> and Cr<sup>III</sup> ions linked through
oxalate ligands and a layer of [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes and solvent molecules (CHCl<sub>3</sub>, CHBr<sub>3</sub>, or CH<sub>2</sub>Br<sub>2</sub>) intercalated between the 2D oxalate
network. The magnetic properties and Mössbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes at different temperatures <i>T</i><sub>1/2</sub>. The three compounds present a LIESST effect with a relaxation
temperature <i>T</i><sub>LIESST</sub> inversely proportional
to <i>T</i><sub>1/2</sub>. The isostructural paramagnetic
compound, [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>2·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) was also prepared. This compound presents a
partial spin crossover of the inserted Fe<sup>III</sup> complex as
well as a LIESST effect. Finally, spectroscopic characterization of
the Fe<sup>III</sup> doped compound [Ga<sub>0.99</sub>Fe<sub>0.01</sub>(sal<sub>2</sub>trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>3·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) shows a gradual
and complete thermal spin crossover and a LIESST effect on the isolated
Fe<sup>III</sup> complexes. This result confirms that cooperativity
is not a necessary condition to observe the LIESST effect in an Fe<sup>III</sup> compound
Stimuli Responsive Hybrid Magnets: Tuning the Photoinduced Spin-Crossover in Fe(III) Complexes Inserted into Layered Magnets
The
insertion of a [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complex
cation into a 2D oxalate network in the presence of different solvents
results in a family of hybrid magnets with coexistence of magnetic
ordering and photoinduced spin-crossover (LIESST effect) in compounds
[Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHCl<sub>3</sub> (<b>1·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHBr<sub>3</sub> (<b>1·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Br<sub>2</sub> (<b>1·CH</b><sub><b>2</b></sub><b>Br</b><sub><b>2</b></sub>). The three compounds crystallize in a 2D honeycomb anionic layer
formed by Mn<sup>II</sup> and Cr<sup>III</sup> ions linked through
oxalate ligands and a layer of [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes and solvent molecules (CHCl<sub>3</sub>, CHBr<sub>3</sub>, or CH<sub>2</sub>Br<sub>2</sub>) intercalated between the 2D oxalate
network. The magnetic properties and Mössbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes at different temperatures <i>T</i><sub>1/2</sub>. The three compounds present a LIESST effect with a relaxation
temperature <i>T</i><sub>LIESST</sub> inversely proportional
to <i>T</i><sub>1/2</sub>. The isostructural paramagnetic
compound, [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>2·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) was also prepared. This compound presents a
partial spin crossover of the inserted Fe<sup>III</sup> complex as
well as a LIESST effect. Finally, spectroscopic characterization of
the Fe<sup>III</sup> doped compound [Ga<sub>0.99</sub>Fe<sub>0.01</sub>(sal<sub>2</sub>trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>3·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) shows a gradual
and complete thermal spin crossover and a LIESST effect on the isolated
Fe<sup>III</sup> complexes. This result confirms that cooperativity
is not a necessary condition to observe the LIESST effect in an Fe<sup>III</sup> compound
Stimuli Responsive Hybrid Magnets: Tuning the Photoinduced Spin-Crossover in Fe(III) Complexes Inserted into Layered Magnets
The
insertion of a [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complex
cation into a 2D oxalate network in the presence of different solvents
results in a family of hybrid magnets with coexistence of magnetic
ordering and photoinduced spin-crossover (LIESST effect) in compounds
[Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHCl<sub>3</sub> (<b>1·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHBr<sub>3</sub> (<b>1·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Br<sub>2</sub> (<b>1·CH</b><sub><b>2</b></sub><b>Br</b><sub><b>2</b></sub>). The three compounds crystallize in a 2D honeycomb anionic layer
formed by Mn<sup>II</sup> and Cr<sup>III</sup> ions linked through
oxalate ligands and a layer of [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes and solvent molecules (CHCl<sub>3</sub>, CHBr<sub>3</sub>, or CH<sub>2</sub>Br<sub>2</sub>) intercalated between the 2D oxalate
network. The magnetic properties and Mössbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes at different temperatures <i>T</i><sub>1/2</sub>. The three compounds present a LIESST effect with a relaxation
temperature <i>T</i><sub>LIESST</sub> inversely proportional
to <i>T</i><sub>1/2</sub>. The isostructural paramagnetic
compound, [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>2·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) was also prepared. This compound presents a
partial spin crossover of the inserted Fe<sup>III</sup> complex as
well as a LIESST effect. Finally, spectroscopic characterization of
the Fe<sup>III</sup> doped compound [Ga<sub>0.99</sub>Fe<sub>0.01</sub>(sal<sub>2</sub>trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>3·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) shows a gradual
and complete thermal spin crossover and a LIESST effect on the isolated
Fe<sup>III</sup> complexes. This result confirms that cooperativity
is not a necessary condition to observe the LIESST effect in an Fe<sup>III</sup> compound
Investigation of Charge-Ordered Barium Iron Fluorides with One-Dimensional Structural Diversity and Complex Magnetic Interactions
Three mixed-valence barium iron fluorides, Ba7Fe7F34, Ba2Fe2F9,
and BaFe2F7, were prepared through hydrothermal
redox reactions. The characteristic structures of these compounds
feature diverse distributions of FeIIF6 octahedra
and FeIIIF6 groups. Ba7Fe7F34 contained one-dimensional infinite ∞[FeIIFeIII6F34]14– double chains, comprising cis corner-sharing octahedra
along the b direction; Ba2Fe2F9 contained one-dimensional ∞[Fe2F9]4– double chains, consisting
of cis corner-sharing octahedra along the chain (a-axis direction) and trans corner-sharing
octahedra vertical to the chain, while BaFe2F7 revealed three-dimensional (3D) frameworks that consist of isolated
edge-sharing dinuclear FeII2F10 units
linked via corners by FeIIIF6 octahedra. Magnetization
and Mössbauer spectroscopy measurements revealed that Ba7Fe7F34 exhibits an antiferromagnetic
phase transition at ∼11 K, where ferrimagnetic ∞[FeIIFeIII6F34]14– double chains are arranged in a paralleling manner, while Ba2Fe2F9 shows canted antiferromagnetic
ordering at ∼32.5 K, leading to noncollinear spin ordering
Stimuli Responsive Hybrid Magnets: Tuning the Photoinduced Spin-Crossover in Fe(III) Complexes Inserted into Layered Magnets
The
insertion of a [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complex
cation into a 2D oxalate network in the presence of different solvents
results in a family of hybrid magnets with coexistence of magnetic
ordering and photoinduced spin-crossover (LIESST effect) in compounds
[Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHCl<sub>3</sub> (<b>1·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CHBr<sub>3</sub> (<b>1·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Br<sub>2</sub> (<b>1·CH</b><sub><b>2</b></sub><b>Br</b><sub><b>2</b></sub>). The three compounds crystallize in a 2D honeycomb anionic layer
formed by Mn<sup>II</sup> and Cr<sup>III</sup> ions linked through
oxalate ligands and a layer of [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes and solvent molecules (CHCl<sub>3</sub>, CHBr<sub>3</sub>, or CH<sub>2</sub>Br<sub>2</sub>) intercalated between the 2D oxalate
network. The magnetic properties and Mössbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [Fe(sal<sub>2</sub>-trien)]<sup>+</sup> complexes at different temperatures <i>T</i><sub>1/2</sub>. The three compounds present a LIESST effect with a relaxation
temperature <i>T</i><sub>LIESST</sub> inversely proportional
to <i>T</i><sub>1/2</sub>. The isostructural paramagnetic
compound, [Fe<sup>III</sup>(sal<sub>2</sub>-trien)][Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>2·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) was also prepared. This compound presents a
partial spin crossover of the inserted Fe<sup>III</sup> complex as
well as a LIESST effect. Finally, spectroscopic characterization of
the Fe<sup>III</sup> doped compound [Ga<sub>0.99</sub>Fe<sub>0.01</sub>(sal<sub>2</sub>trien)][Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]·CH<sub>2</sub>Cl<sub>2</sub> (<b>3·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>) shows a gradual
and complete thermal spin crossover and a LIESST effect on the isolated
Fe<sup>III</sup> complexes. This result confirms that cooperativity
is not a necessary condition to observe the LIESST effect in an Fe<sup>III</sup> compound