15 research outputs found
One-Dimensional and Two-Dimensional Anilate-Based Magnets with Inserted Spin-Crossover Complexes
The syntheses, structures, and magnetic
properties of a family
of bimetallic anilate-based compounds with inserted spin-crossover
cationic complexes are reported. The structures of <b>1</b>ā<b>4</b> present a two-dimensional anionic network formed by MnĀ(II)
and CrĀ(III) ions linked through anilate ligands with inserted [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]<sup>+</sup> (<b>1</b>), [Fe<sup>III</sup>(4-OH-sal<sub>2</sub>-trien)]<sup>+</sup> (<b>2</b>), [Fe<sup>III</sup>(sal<sub>2</sub>-epe)]<sup>+</sup> (<b>3</b>), or [Fe<sup>III</sup>(5-Cl-sal<sub>2</sub>-trien)]<sup>+</sup> (<b>4</b>) complexes. The structure of <b>5</b> is formed by
anionic [Mn<sup>II</sup>Cl<sub>2</sub>Cr<sup>III</sup>(Cl<sub>2</sub>An)<sub>3</sub>]<sup>3ā</sup> chains surrounded by [Fe<sup>II</sup>(trenĀ(imid)<sub>3</sub>)]<sup>2+</sup>, Cl<sup>ā</sup>, and solvent molecules. The magnetic properties indicate that <b>1</b>ā<b>4</b> undergo a long-range ferrimagnetic
ordering at ca. 10 K. On the other hand, the inserted FeĀ(III) cations
remain in the low-spin (in <b>4</b>) or high-spin state (in <b>1</b>, <b>2</b>, and <b>3</b>). In the case of <b>5</b>, half of the inserted FeĀ(II) cations undergo a complete
and gradual spin crossover from 280 to 90 K that coexists with a magnetic
ordering below 2.5 K
Patterning of Magnetic Bimetallic Coordination Nanoparticles of Prussian Blue Derivatives by the LangmuirāBlodgett Technique
We report a novel method to prepare patterns of nanoparticles
over
large areas of the substrate. This method is based on the adsorption
of the negatively charged nanoparticles dispersed in an aqueous subphase
onto a monolayer of the phospholipid dipalmitoyl-l-Ī±-phosphatidylcholine
(DPPC) at the airāwater interface. It has been used to prepare
patterns of nanoparticles of Prussian blue analogues (PBA) of different
size (K<sub>0.25</sub>NiĀ[FeĀ(CN)<sub>6</sub>]<sub>0.75</sub> (NiFe),
K<sub>0.25</sub>NiĀ[CrĀ(CN)<sub>6</sub>]<sub>0.75</sub> (NiCr), K<sub>0.25</sub>NiĀ[CoĀ(CN)<sub>6</sub>]<sub>0.75</sub> (NiCo), Cs<sub>0.4</sub>CoĀ[CrĀ(CN)<sub>6</sub>]<sub>0.8</sub> (CsCoCr), and Cs<sub>0.4</sub>CoĀ[FeĀ(CN)<sub>6</sub>]<sub>0.9</sub> (CsCoFe)). The behavior of DPPC
monolayer at the airāwater interface in the presence of the
subphase of PBA nanoparticles has been studied by the compression
isotherms and Brewster angle microscopy (BAM) images. Atomic force
microscopy (AFM) of the transferred films on mica substrates shows
that patterns of the nanoparticles are observed for a 10<sup>ā4</sup> M concentration of the subphase, based on the nanoparticle precursors,
at surface pressures between 1 and 6 mN/m and transfer velocities
from 10 to 80 mm/min. Vertical, horizontal, or tilted fringes of the
nanoparticles with respect to the transfer direction can be obtained
depending on the transfer velocity and surface pressure
Nonanuclear Spin-Crossover Complex Containing Iron(II) and Iron(III) Based on a 2,6-Bis(pyrazol-1-yl)pyridine Ligand Functionalized with a Carboxylate Group
The synthesis and
magnetostructural characterization of [Fe<sup>III</sup><sub>3</sub>(Ī¼<sub>3</sub>-O)Ā(H<sub>2</sub>O)<sub>3</sub>[Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sub>6</sub>]Ā(ClO<sub>4</sub>)<sub>13</sub>Ā·(CH<sub>3</sub>)<sub>2</sub>CO)<sub>6</sub>Ā·(solvate) (<b>2</b>) are reported. This compound is obtained as a secondary product
during synthesis of the mononuclear complex [Fe<sup>II</sup>(bppCOOH)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>2</sub> (<b>1</b>). The single-crystal
X-ray diffraction structure of <b>2</b> shows that it contains
the nonanuclear cluster of the formula [Fe<sup>III</sup><sub>3</sub>(Ī¼<sub>3</sub>-O)Ā(H<sub>2</sub>O)<sub>3</sub>[Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sub>6</sub>]<sup>13+</sup>, which is formed by
a central Fe<sup>III</sup><sub>3</sub>O core coordinated to six partially
deprotonated [Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sup>+</sup> complexes.
Raman spectroscopy studies on single crystals of <b>1</b> and <b>2</b> have been performed to elucidate the spin and oxidation
states of iron in <b>2</b>. These studies and magnetic characterization
indicate that most of the ironĀ(II) complexes of <b>2</b> remain
in the low-spin (LS) state and present a gradual and incomplete spin
crossover above 300 K. On the other hand, the Fe<sup>III</sup> trimer
shows the expected antiferromagnetic behavior. From the structural
point of view, <b>2</b> represents the first example in which
bppCOO<sup>ā</sup> acts as a bridging ligand, thus forming
a polynuclear magnetic complex
Nonanuclear Spin-Crossover Complex Containing Iron(II) and Iron(III) Based on a 2,6-Bis(pyrazol-1-yl)pyridine Ligand Functionalized with a Carboxylate Group
The synthesis and
magnetostructural characterization of [Fe<sup>III</sup><sub>3</sub>(Ī¼<sub>3</sub>-O)Ā(H<sub>2</sub>O)<sub>3</sub>[Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sub>6</sub>]Ā(ClO<sub>4</sub>)<sub>13</sub>Ā·(CH<sub>3</sub>)<sub>2</sub>CO)<sub>6</sub>Ā·(solvate) (<b>2</b>) are reported. This compound is obtained as a secondary product
during synthesis of the mononuclear complex [Fe<sup>II</sup>(bppCOOH)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>2</sub> (<b>1</b>). The single-crystal
X-ray diffraction structure of <b>2</b> shows that it contains
the nonanuclear cluster of the formula [Fe<sup>III</sup><sub>3</sub>(Ī¼<sub>3</sub>-O)Ā(H<sub>2</sub>O)<sub>3</sub>[Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sub>6</sub>]<sup>13+</sup>, which is formed by
a central Fe<sup>III</sup><sub>3</sub>O core coordinated to six partially
deprotonated [Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sup>+</sup> complexes.
Raman spectroscopy studies on single crystals of <b>1</b> and <b>2</b> have been performed to elucidate the spin and oxidation
states of iron in <b>2</b>. These studies and magnetic characterization
indicate that most of the ironĀ(II) complexes of <b>2</b> remain
in the low-spin (LS) state and present a gradual and incomplete spin
crossover above 300 K. On the other hand, the Fe<sup>III</sup> trimer
shows the expected antiferromagnetic behavior. From the structural
point of view, <b>2</b> represents the first example in which
bppCOO<sup>ā</sup> acts as a bridging ligand, thus forming
a polynuclear magnetic complex
Nonanuclear Spin-Crossover Complex Containing Iron(II) and Iron(III) Based on a 2,6-Bis(pyrazol-1-yl)pyridine Ligand Functionalized with a Carboxylate Group
The synthesis and
magnetostructural characterization of [Fe<sup>III</sup><sub>3</sub>(Ī¼<sub>3</sub>-O)Ā(H<sub>2</sub>O)<sub>3</sub>[Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sub>6</sub>]Ā(ClO<sub>4</sub>)<sub>13</sub>Ā·(CH<sub>3</sub>)<sub>2</sub>CO)<sub>6</sub>Ā·(solvate) (<b>2</b>) are reported. This compound is obtained as a secondary product
during synthesis of the mononuclear complex [Fe<sup>II</sup>(bppCOOH)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>2</sub> (<b>1</b>). The single-crystal
X-ray diffraction structure of <b>2</b> shows that it contains
the nonanuclear cluster of the formula [Fe<sup>III</sup><sub>3</sub>(Ī¼<sub>3</sub>-O)Ā(H<sub>2</sub>O)<sub>3</sub>[Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sub>6</sub>]<sup>13+</sup>, which is formed by
a central Fe<sup>III</sup><sub>3</sub>O core coordinated to six partially
deprotonated [Fe<sup>II</sup>(bppCOOH)Ā(bppCOO)]<sup>+</sup> complexes.
Raman spectroscopy studies on single crystals of <b>1</b> and <b>2</b> have been performed to elucidate the spin and oxidation
states of iron in <b>2</b>. These studies and magnetic characterization
indicate that most of the ironĀ(II) complexes of <b>2</b> remain
in the low-spin (LS) state and present a gradual and incomplete spin
crossover above 300 K. On the other hand, the Fe<sup>III</sup> trimer
shows the expected antiferromagnetic behavior. From the structural
point of view, <b>2</b> represents the first example in which
bppCOO<sup>ā</sup> acts as a bridging ligand, thus forming
a polynuclear magnetic complex
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 āreal-lifeā 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 [FeĀ(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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHCl<sub>3</sub> (<b>1Ā·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHBr<sub>3</sub> (<b>1Ā·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Br<sub>2</sub> (<b>1Ā·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 [FeĀ(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 MoĢssbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [FeĀ(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)]Ā[Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>2Ā·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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>3Ā·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 [FeĀ(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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHCl<sub>3</sub> (<b>1Ā·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHBr<sub>3</sub> (<b>1Ā·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Br<sub>2</sub> (<b>1Ā·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 [FeĀ(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 MoĢssbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [FeĀ(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)]Ā[Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>2Ā·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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>3Ā·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 [FeĀ(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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHCl<sub>3</sub> (<b>1Ā·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHBr<sub>3</sub> (<b>1Ā·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Br<sub>2</sub> (<b>1Ā·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 [FeĀ(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 MoĢssbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [FeĀ(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)]Ā[Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>2Ā·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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>3Ā·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 [FeĀ(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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHCl<sub>3</sub> (<b>1Ā·CHCl</b><sub><b>3</b></sub>), [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CHBr<sub>3</sub> (<b>1Ā·CHBr</b><sub><b>3</b></sub>), and [Fe<sup>III</sup>(sal<sub>2</sub>-trien)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Br<sub>2</sub> (<b>1Ā·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 [FeĀ(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 MoĢssbauer spectroscopy
indicate that they undergo long-range ferromagnetic ordering at 5.6
K and a spin crossover of the intercalated [FeĀ(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)]Ā[Zn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>2Ā·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)]Ā[Mn<sup>II</sup>Cr<sup>III</sup>(ox)<sub>3</sub>]Ā·CH<sub>2</sub>Cl<sub>2</sub> (<b>3Ā·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