5 research outputs found
Experimental and Theoretical Investigation of a Series of Novel Dimanganese(III) μ‑Hydroxo Bisporphyrins: Magneto–Structural Correlation and Effect of Metal Spin on Porphyrin Core Deformation
The synthesis, structure, and properties
of a new family of five ethane-bridged dimanganeseÂ(III) μ-hydroxo
bisporphyrins with the same core structure but different counteranions
are reported here. Additions of 10% Brønsted acids such as HI,
HBF<sub>4</sub>, HSbF<sub>6</sub>, HPF<sub>6</sub>, and HClO<sub>4</sub> to a dichloromethane solution of the dichloro dimanganeseÂ(III) bisporphyrin
produces complexes having a remarkably bent μ-hydroxo group
with I<sub>3</sub><sup>–</sup>, BF<sub>4</sub><sup>–</sup>, SbF<sub>6</sub><sup>–</sup>, PF<sub>6</sub><sup>–</sup>, and ClO<sub>4</sub><sup>–</sup> as counteranions, respectively.
The X-ray structures of all complexes have been determined, which
have revealed the presence of two equivalent high-spin manganeseÂ(III)
centers with equally distorted porphyrin rings in the complexes, in
sharp contrast with the case for the diironÂ(III) μ-hydroxo bisporphyrin
analogues. <sup>1</sup>H NMR spectra have shown highly deshielded <i>meso</i> resonances, unlike the case for the diironÂ(III) analogues,
where the <i>meso</i> resonances are highly shielded. The
variable-temperature magnetic data have been subjected to a least-squares
fit which provides a moderate antiferromagnetic coupling through the
hydroxo bridge between two zero-field split MnÂ(III) centers with coupling
constant (<i>J</i>) values ranging from −29.5 to
−38.6 cm<sup>–1</sup>. Fairly good correlations are
observed for <i>J</i> with Mn–OÂ(H) distances and
Mn–OÂ(H)–Mn angles for all the complexes except for that
having an I<sub>3</sub><sup>–</sup> counteranion. DFT calculations
support the stabilization of two equivalent high-spin MnÂ(III) porphyrin
cores in the complexes and have also explored the role of metal spin
in controlling porphyrin ring deformation. Unlike diironÂ(III) μ-hydroxo
bisporphyrin complexes, the dimanganeseÂ(III) analogues do not have
easily accessible spin states of the metal attainable by subtle environmental
perturbations and, therefore, can only stabilize the high-spin state
with a variety of counteranions
Experimental and Theoretical Investigation of a Series of Novel Dimanganese(III) μ‑Hydroxo Bisporphyrins: Magneto–Structural Correlation and Effect of Metal Spin on Porphyrin Core Deformation
The synthesis, structure, and properties
of a new family of five ethane-bridged dimanganeseÂ(III) μ-hydroxo
bisporphyrins with the same core structure but different counteranions
are reported here. Additions of 10% Brønsted acids such as HI,
HBF<sub>4</sub>, HSbF<sub>6</sub>, HPF<sub>6</sub>, and HClO<sub>4</sub> to a dichloromethane solution of the dichloro dimanganeseÂ(III) bisporphyrin
produces complexes having a remarkably bent μ-hydroxo group
with I<sub>3</sub><sup>–</sup>, BF<sub>4</sub><sup>–</sup>, SbF<sub>6</sub><sup>–</sup>, PF<sub>6</sub><sup>–</sup>, and ClO<sub>4</sub><sup>–</sup> as counteranions, respectively.
The X-ray structures of all complexes have been determined, which
have revealed the presence of two equivalent high-spin manganeseÂ(III)
centers with equally distorted porphyrin rings in the complexes, in
sharp contrast with the case for the diironÂ(III) μ-hydroxo bisporphyrin
analogues. <sup>1</sup>H NMR spectra have shown highly deshielded <i>meso</i> resonances, unlike the case for the diironÂ(III) analogues,
where the <i>meso</i> resonances are highly shielded. The
variable-temperature magnetic data have been subjected to a least-squares
fit which provides a moderate antiferromagnetic coupling through the
hydroxo bridge between two zero-field split MnÂ(III) centers with coupling
constant (<i>J</i>) values ranging from −29.5 to
−38.6 cm<sup>–1</sup>. Fairly good correlations are
observed for <i>J</i> with Mn–OÂ(H) distances and
Mn–OÂ(H)–Mn angles for all the complexes except for that
having an I<sub>3</sub><sup>–</sup> counteranion. DFT calculations
support the stabilization of two equivalent high-spin MnÂ(III) porphyrin
cores in the complexes and have also explored the role of metal spin
in controlling porphyrin ring deformation. Unlike diironÂ(III) μ-hydroxo
bisporphyrin complexes, the dimanganeseÂ(III) analogues do not have
easily accessible spin states of the metal attainable by subtle environmental
perturbations and, therefore, can only stabilize the high-spin state
with a variety of counteranions
Experimental and Theoretical Investigation of a Series of Novel Dimanganese(III) μ‑Hydroxo Bisporphyrins: Magneto–Structural Correlation and Effect of Metal Spin on Porphyrin Core Deformation
The synthesis, structure, and properties
of a new family of five ethane-bridged dimanganeseÂ(III) μ-hydroxo
bisporphyrins with the same core structure but different counteranions
are reported here. Additions of 10% Brønsted acids such as HI,
HBF<sub>4</sub>, HSbF<sub>6</sub>, HPF<sub>6</sub>, and HClO<sub>4</sub> to a dichloromethane solution of the dichloro dimanganeseÂ(III) bisporphyrin
produces complexes having a remarkably bent μ-hydroxo group
with I<sub>3</sub><sup>–</sup>, BF<sub>4</sub><sup>–</sup>, SbF<sub>6</sub><sup>–</sup>, PF<sub>6</sub><sup>–</sup>, and ClO<sub>4</sub><sup>–</sup> as counteranions, respectively.
The X-ray structures of all complexes have been determined, which
have revealed the presence of two equivalent high-spin manganeseÂ(III)
centers with equally distorted porphyrin rings in the complexes, in
sharp contrast with the case for the diironÂ(III) μ-hydroxo bisporphyrin
analogues. <sup>1</sup>H NMR spectra have shown highly deshielded <i>meso</i> resonances, unlike the case for the diironÂ(III) analogues,
where the <i>meso</i> resonances are highly shielded. The
variable-temperature magnetic data have been subjected to a least-squares
fit which provides a moderate antiferromagnetic coupling through the
hydroxo bridge between two zero-field split MnÂ(III) centers with coupling
constant (<i>J</i>) values ranging from −29.5 to
−38.6 cm<sup>–1</sup>. Fairly good correlations are
observed for <i>J</i> with Mn–OÂ(H) distances and
Mn–OÂ(H)–Mn angles for all the complexes except for that
having an I<sub>3</sub><sup>–</sup> counteranion. DFT calculations
support the stabilization of two equivalent high-spin MnÂ(III) porphyrin
cores in the complexes and have also explored the role of metal spin
in controlling porphyrin ring deformation. Unlike diironÂ(III) μ-hydroxo
bisporphyrin complexes, the dimanganeseÂ(III) analogues do not have
easily accessible spin states of the metal attainable by subtle environmental
perturbations and, therefore, can only stabilize the high-spin state
with a variety of counteranions
Experimental and Theoretical Investigation of a Series of Novel Dimanganese(III) μ‑Hydroxo Bisporphyrins: Magneto–Structural Correlation and Effect of Metal Spin on Porphyrin Core Deformation
The synthesis, structure, and properties
of a new family of five ethane-bridged dimanganeseÂ(III) μ-hydroxo
bisporphyrins with the same core structure but different counteranions
are reported here. Additions of 10% Brønsted acids such as HI,
HBF<sub>4</sub>, HSbF<sub>6</sub>, HPF<sub>6</sub>, and HClO<sub>4</sub> to a dichloromethane solution of the dichloro dimanganeseÂ(III) bisporphyrin
produces complexes having a remarkably bent μ-hydroxo group
with I<sub>3</sub><sup>–</sup>, BF<sub>4</sub><sup>–</sup>, SbF<sub>6</sub><sup>–</sup>, PF<sub>6</sub><sup>–</sup>, and ClO<sub>4</sub><sup>–</sup> as counteranions, respectively.
The X-ray structures of all complexes have been determined, which
have revealed the presence of two equivalent high-spin manganeseÂ(III)
centers with equally distorted porphyrin rings in the complexes, in
sharp contrast with the case for the diironÂ(III) μ-hydroxo bisporphyrin
analogues. <sup>1</sup>H NMR spectra have shown highly deshielded <i>meso</i> resonances, unlike the case for the diironÂ(III) analogues,
where the <i>meso</i> resonances are highly shielded. The
variable-temperature magnetic data have been subjected to a least-squares
fit which provides a moderate antiferromagnetic coupling through the
hydroxo bridge between two zero-field split MnÂ(III) centers with coupling
constant (<i>J</i>) values ranging from −29.5 to
−38.6 cm<sup>–1</sup>. Fairly good correlations are
observed for <i>J</i> with Mn–OÂ(H) distances and
Mn–OÂ(H)–Mn angles for all the complexes except for that
having an I<sub>3</sub><sup>–</sup> counteranion. DFT calculations
support the stabilization of two equivalent high-spin MnÂ(III) porphyrin
cores in the complexes and have also explored the role of metal spin
in controlling porphyrin ring deformation. Unlike diironÂ(III) μ-hydroxo
bisporphyrin complexes, the dimanganeseÂ(III) analogues do not have
easily accessible spin states of the metal attainable by subtle environmental
perturbations and, therefore, can only stabilize the high-spin state
with a variety of counteranions
The Planar Cyclooctatetraene Bridge in Bis-Metallic Macrocycles: Isolating or Conjugating?
A minor modification of the reported
procedure for the synthesis
of a corrole dimer that is fused by the cyclooctatetraene (COT) unit,
(H<sub>3</sub>tpfc)<sub>2</sub>COT, allowed for its isolation in 18%
yield. Of the two redox isomers that this interesting macrocycle does
form, the current focus is on the reduced form, in which each subunit
resembles that of monomeric corroles with a trianionic N<sub>4</sub> coordination core. The corresponding bis-galliumÂ(III) complex was
prepared as an entry into the potentially rich coordination chemistry
of (H<sub>3</sub>tpfc)<sub>2</sub>COT. Both X-ray crystallography
and DFT calculations disclosed that the COT moiety is essentially
planar with very unusual nonalternating C–C bonds. The same
holds true for the bis-galliumÂ(III) complexes [(Ga-tpfc)<sub>2</sub>]ÂCOTÂ(py)<sub>2</sub> and [(Ga-tpfc)<sub>2</sub>]ÂCOTÂ(py)<sub>4</sub>, obtained with one and two pyridine molecules coordinated to each
metal ion, respectively. The electronic spectra of both the free base
and the galliumÂ(III) complexes display an extremely low energy band
(λ<sub>max</sub> at 720–724 nm), which points toward
extensive π delocalization through the COT bridge. This aspect
was fully addressed by examining the interactions between the two
corrole subunits in terms of electrochemistry and DFT calculations
of the oxidized and reduced macrocycle. The new near-IR bands that
appear upon both oxidation (λ<sub>max</sub> 1250 nm) and reduction
(λ<sub>max</sub> 1780 nm) serve as additional supporting evidence
for this conclusion