6 research outputs found
Triple-Stranded Helicates of Zinc(II) and Cadmium(II) Involving a New Redox-Active Multiring Nitrogenous Heterocyclic Ligand: Synthesis, Structure, and Electrochemical and Photophysical Properties
The protonated form [H<sub>2</sub>(L)]Ā(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub> (<b>1</b>) of a new redox-active
bis-bidentate
nitrogenous heterocyclic ligand, viz., 3,3ā²-dipyridin-2-ylĀ[1,1ā²]ĀbiĀ[imidazoĀ[1,5-<i>a</i>]Āpyridinyl] (L), and its zincĀ(II) and cadmiumĀ(II) complexes
(<b>2</b> and <b>3</b>) have been synthesized and characterized
by single-crystal X-ray diffraction analysis. In the solid state,
both <b>2</b> and <b>3</b> have triple-stranded helical
structures involving ligands that experience twisting and bending
to the extent needed by the stereoelectronic demand of the central
metal ion. The metal centers in the zincĀ(II) complex [Zn<sub>2</sub>(L)<sub>3</sub>]Ā(ClO<sub>4</sub>)<sub>4</sub> (<b>2</b>) are
equivalent, each having a distorted octahedral geometry, flattened
along the <i>C</i><sub>3</sub> axis with a Zn1Ā·Ā·Ā·Zn1#
separation of 4.8655(13) Ć
. The cadmium complex [Cd<sub>2</sub>(L)<sub>3</sub>(H<sub>2</sub>O)]Ā(ClO<sub>4</sub>)<sub>4</sub> (<b>3</b>), on the other hand, has a rare type of helical structure,
showing coordination asymmetry around the metal centers with a drastically
reduced Cd1Ā·Ā·Ā·Cd2 separation of 4.070 Ć
. The coordination
environment around Cd1 is a distorted pentagonal bipyramid involving
a N<sub>6</sub>O donor set with the oxygen atom coming from a coordinated
water, leaving the remaining metal center Cd2 with a distorted octahedral
geometry. The structures of <b>2</b> and <b>3</b> also
involve anionāĻ- and CHāĻ-type noncovalent
interactions that play dominant roles in shaping the extended structures
of these molecules in the solid state. In solution, these compounds
exhibit strong fluxional behavior, making the individual ligand strands
indistinguishable from one another, as revealed from their <sup>1</sup>H NMR spectra, which also provide indications about these molecules
retaining their helical structures in solution. Electrochemically,
these compounds are quite interesting, undergoing ligand-based oxidations
in two successive one-electron steps at <i>E</i><sub>1/2</sub> of ca. 0.65 and 0.90 V versus a Ag/AgCl (3 M NaCl) reference. These
molecules are all efficient emitters in the red and blue regions because
of ligand-based Ļ*āĻ fluorescent emissions, tuned
appropriately by the attached Lewis acid centers
Triple-Stranded Helicates of Zinc(II) and Cadmium(II) Involving a New Redox-Active Multiring Nitrogenous Heterocyclic Ligand: Synthesis, Structure, and Electrochemical and Photophysical Properties
The protonated form [H<sub>2</sub>(L)]Ā(CF<sub>3</sub>SO<sub>3</sub>)<sub>2</sub> (<b>1</b>) of a new redox-active
bis-bidentate
nitrogenous heterocyclic ligand, viz., 3,3ā²-dipyridin-2-ylĀ[1,1ā²]ĀbiĀ[imidazoĀ[1,5-<i>a</i>]Āpyridinyl] (L), and its zincĀ(II) and cadmiumĀ(II) complexes
(<b>2</b> and <b>3</b>) have been synthesized and characterized
by single-crystal X-ray diffraction analysis. In the solid state,
both <b>2</b> and <b>3</b> have triple-stranded helical
structures involving ligands that experience twisting and bending
to the extent needed by the stereoelectronic demand of the central
metal ion. The metal centers in the zincĀ(II) complex [Zn<sub>2</sub>(L)<sub>3</sub>]Ā(ClO<sub>4</sub>)<sub>4</sub> (<b>2</b>) are
equivalent, each having a distorted octahedral geometry, flattened
along the <i>C</i><sub>3</sub> axis with a Zn1Ā·Ā·Ā·Zn1#
separation of 4.8655(13) Ć
. The cadmium complex [Cd<sub>2</sub>(L)<sub>3</sub>(H<sub>2</sub>O)]Ā(ClO<sub>4</sub>)<sub>4</sub> (<b>3</b>), on the other hand, has a rare type of helical structure,
showing coordination asymmetry around the metal centers with a drastically
reduced Cd1Ā·Ā·Ā·Cd2 separation of 4.070 Ć
. The coordination
environment around Cd1 is a distorted pentagonal bipyramid involving
a N<sub>6</sub>O donor set with the oxygen atom coming from a coordinated
water, leaving the remaining metal center Cd2 with a distorted octahedral
geometry. The structures of <b>2</b> and <b>3</b> also
involve anionāĻ- and CHāĻ-type noncovalent
interactions that play dominant roles in shaping the extended structures
of these molecules in the solid state. In solution, these compounds
exhibit strong fluxional behavior, making the individual ligand strands
indistinguishable from one another, as revealed from their <sup>1</sup>H NMR spectra, which also provide indications about these molecules
retaining their helical structures in solution. Electrochemically,
these compounds are quite interesting, undergoing ligand-based oxidations
in two successive one-electron steps at <i>E</i><sub>1/2</sub> of ca. 0.65 and 0.90 V versus a Ag/AgCl (3 M NaCl) reference. These
molecules are all efficient emitters in the red and blue regions because
of ligand-based Ļ*āĻ fluorescent emissions, tuned
appropriately by the attached Lewis acid centers
Ligand-Induced Tuning of the Oxidase Activity of Ī¼āHydroxidodimanganese(III) Complexes Using 3,5-Di-<i>tert</i>-butylcatechol as the Substrate: Isolation and Characterization of Products Involving an Oxidized Dioxolene Moiety
Oxidase activities
of a Ī¼-hydroxidodimanganeseĀ(III) system involving a series of
tetradentate capping ligands H<sub>2</sub>L<sup>R<sub>1</sub>,R<sub>2</sub></sup> with a pair of phenolate arms have been investigated
in the presence of 3,5-di-<i>tert</i>-butylcatechol (H<sub>2</sub>DBC) as a coligand cum-reductant. The reaction follows two
distinctly different paths, decided by the substituent combinations
(R<sub>1</sub> and R<sub>2</sub>) present in the capping ligand. With
the ligands H<sub>2</sub>L<sup><i>t</i>āBu,<i>t</i>āBu</sup> and H<sub>2</sub>L<sup><i>t</i>āBu,OMe</sup>, the products obtained are semiquinonato compounds
[Mn<sup>III</sup>(L<sup><i>t</i>āBu,<i>t</i>āBu</sup>)Ā(DBSQ)]Ā·2CH<sub>3</sub>OH (<b>1</b>)
and [Mn<sup>III</sup>(L<sup><i>t</i>āBu,OMe</sup>)Ā(DBSQ)]Ā·CH<sub>3</sub>OH (<b>2</b>), respectively. In
the process, molecular oxygen is reduced by two electrons to generate
H<sub>2</sub>O<sub>2</sub> in the solution, as confirmed by iodometric
detection. With the rest of the ligands, viz., H<sub>2</sub>L<sup>Me,Me</sup>, H<sub>2</sub>L<sup><i>t</i>āBu,Me</sup>, H<sub>2</sub>L<sup>Me,<i>t</i>āBu</sup>, and H<sub>2</sub>L<sup>Cl,Cl</sup>, the products initially obtained are believed
to be highly reactive quinonato compounds [Mn<sup>III</sup>(L<sup>R<sub>1</sub>,R<sub>2</sub></sup>)Ā(DBQ)]<sup>+</sup>, which undergo
a domino reaction with the solvent methanol to generate products of
composition [Mn<sup>III</sup>(L<sup>R<sub>1</sub>,R<sub>2</sub></sup>)Ā(BMOD)] (<b>3</b>ā<b>6</b>) involving a nonplanar
dioxolene moiety, viz., 3,5-di-<i>tert</i>-butyl-3-methoxy-6-oxocyclohexa-1,4-dienolate
(BMOD<sup>ā</sup>). This novel dioxolene derivative is formed
by a Michael-type nucleophilic 1,4-addition reaction of the methoxy
group to the coordinated quinone in [Mn<sup>III</sup>(L<sup>R<sub>1</sub>,R<sub>2</sub></sup>)Ā(DBQ)]<sup>+</sup>. During this reaction,
molecular oxygen is reduced by four electrons to generate water. The
products have been characterized by single-crystal X-ray diffraction
analysis as well as by spectroscopic methods and magnetic measurements.
Density functional theory calculations have been made to address the
observed influence of the secondary coordination sphere in tuning
the two-electron versus four-electron reduction of dioxygen. The semiquinone
form of the dioxolene moiety is stabilized in compounds <b>1</b> and <b>2</b> because of extended electron delocalization via
participation of the appropriate metal orbital(s)
Nonoxido Vanadium(IV) Compounds Involving Dithiocarbazate-Based Tridentate ONS Ligands: Synthesis, Electronic and Molecular Structure, Spectroscopic and Redox Properties
A new series of nonoxido vanadiumĀ(IV)
compounds [VL<sub>2</sub>] (L = L<sup>1</sup>āL<sup>3</sup>) (<b>1</b>ā<b>3</b>) have been synthesized using
dithiocarbazate-based tridentate
Schiff-base ligands H<sub>2</sub>L<sup>1</sup>āH<sub>2</sub>L<sup>3</sup>, containing an appended phenol ring with a <i>tert</i>-butyl substitution at the 2-position. The compounds
are characterized by X-ray diffraction analysis (<b>1</b>, <b>3</b>), IR, UV-vis, EPR spectroscopy, and electrochemical methods.
These are nonoxido V<sup>IV</sup> complexes that reveal a rare distorted
trigonal prismatic arrangement around the ābareā vanadium
centers. Concerning the ligand isomerism, the structure of <b>1</b> and <b>3</b> can be described as intermediate between <i>mer</i> and <i>sym-fac</i> isomers. DFT methods were
used to predict the geometry, <b>g</b> and <sup>51</sup>V <b>A</b> tensors, electronic structure, and electronic absorption
spectrum of compounds <b>1</b>ā<b>3</b>. Hyperfine
coupling constants measured in the EPR spectra can be reproduced satisfactorily
at the level of theory PBE0/VTZ, whereas the wavelength and intensity
of the absorptions in the UV-vis spectra at the level CAM-B3LYP/gen,
where āgenā is a general basis set obtained using 6-31+gĀ(d)
for S and 6-31g for all the other elements. The results suggest that
the electronic structure of <b>1</b>ā<b>3</b> can
be described in terms of a mixing among V-<i>d</i><sub><i>xy</i></sub>, V-<i>d</i><sub><i>xz</i></sub>, and V-<i>d</i><sub><i>yz</i></sub> orbitals
in the singly occupied molecular orbital (SOMO), which causes a significant
lowering of the absolute value of the <sup>51</sup>V hyperfine coupling
constant along the <i>x</i>-axis. The cyclic voltammograms
of these compounds in dichloroethane solution display three one-electron
processes, two in the cathodic and one in the anodic potential range.
Process A (<i>E</i><sub>1/2</sub> = +1.06 V) is due to the
quasi-reversible VĀ(IV/V) oxidation while process B at <i>E</i><sub>1/2</sub> = ā0.085 V is due to the quasi-reversible VĀ(IV/III)
reduction, and the third one (process C) at a more negative potential <i>E</i><sub>1/2</sub> = ā1.66 V is due to a ligand centered
reduction, all potentials being measured vs Ag/AgCl reference
Pentanuclear 3dā4f Heterometal Complexes of M<sup>II</sup><sub>3</sub>Ln<sup>III</sup><sub>2</sub> (M = Ni, Cu, Zn and Ln = Nd, Gd, Tb) Combinations: Syntheses, Structures, Magnetism, and Photoluminescence Properties
A new family of pentanuclear 3dā4f
heterometal complexes of general composition [Ln<sup>III</sup><sub>2</sub>(M<sup>II</sup>L)<sub>3</sub>(Ī¼<sub>3</sub>-O)<sub>3</sub>H]Ā(ClO<sub>4</sub>)Ā·<i>x</i>H<sub>2</sub>O (<b>1</b>ā<b>5</b>) [Ln = Nd, M = Zn, <b>1</b>;
Nd, Ni, <b>2</b>; Nd, Cu, <b>3</b>; Gd, Cu, <b>4</b>; Tb, Cu, <b>5</b>] have been synthesized in moderate yields
(50ā60%) following a self-assembly reaction involving the hexadentate
phenol-based ligand, viz., <i>N</i>,<i>N</i>-bisĀ(2-hydroxy-3-methoxy-5-methylbenzyl)-<i>N</i><sup>ā²</sup>,<i>N</i><sup>ā²</sup>-diethylethylenediamine (H<sub>2</sub>L). Single-crystal X-ray diffraction
analyses have been used to characterize these complexes. The compounds
are all isostructural, having a 3-fold axis of symmetry that passes
through the 4f metal centers. The [M<sup>II</sup>L] units in these
complexes are acting as bis-bidentate metalloligands and, together
with Ī¼<sub>3</sub>-oxido bridging ligands, complete the slightly
distorted monocapped square antiprismatic nine-coordination environment
around the 4f metal centers. The cationic complexes also contain a
H<sup>+</sup> ion that occupies the central position at the 3-fold
axis. Magnetic properties of the copperĀ(II) complexes (<b>3</b>ā<b>5</b>) show a changeover from antiferromagnetic
in <b>3</b> to ferromagnetic 3dā4f interactions in <b>4</b> and <b>5</b>. For the isotropic Cu<sup>II</sup>āGd<sup>III</sup> compound <b>4</b>, the simulation of magnetic data
provides very weak CuāGd (<i>J</i><sub>1</sub> =
0.57 cm<sup>ā1</sup>) and GdāGd exchange constants (<i>J</i><sub>2</sub> = 0.14 cm<sup>ā1</sup>). Compound <b>4</b> is the only member of this triad, showing a tail of an out-of-phase
signal in the ac susceptibility measurement. A large-spin ground state
(<i>S</i> = 17/2) and a negative value of <i>D</i> (ā0.12 cm<sup>ā1</sup>) result in a very small barrier
(8 cm<sup>ā1</sup>) for this compound. Among the three Nd<sup>III</sup><sub>2</sub>M<sup>II</sup><sub>3</sub> (M = Zn<sup>II</sup>, Ni<sup>II</sup>, and Cu<sup>II</sup>) complexes, only the Zn<sup>II</sup> analogue (<b>1</b>) displays an NIR luminescence due
to the <sup>4</sup>F<sub>3/2</sub> ā <sup>4</sup>I<sub>11/2</sub> transition in Nd<sup>III</sup> when excited at 290 nm. The rest
of the compounds do not show such Nd<sup>III</sup>/Tb<sup>III</sup>-based emission. The paramagnetic Cu<sup>II</sup> and Ni<sup>II</sup> ions quench the fluorescence in <b>2</b>ā<b>5</b> and thereby lower the population of the triplet state
Dinuclear Iron(III) and Cobalt(III) Complexes Featuring a Biradical Bridge: Their Molecular Structures and Magnetic, Spectroscopic, and Redox Properties
Bis-bidentate ligand
H<sub>4</sub>L<sup><i>B</i></sup> featuring two <i>o</i>-amidophenol noninnocent units was used to synthesize novel
binuclear complexes [(L<sup><i>R</i></sup>)ĀM<sup>III</sup>(ā¢L<sup><i>B</i></sup>ā¢)ĀM<sup>III</sup>(L<sup><i>R</i></sup>)]Ā(ClO<sub>4</sub>)<sub>2</sub>, M = Fe (<b>1</b>) and Co (<b>2</b>, <b>3</b>), with HL<sup><i>R</i></sup> (R = CH<sub>3</sub>, Cl) being the facially coordinating
tetradentate coligands. Upon the synthesis, the fully reduced amidophenolate
form of the ligand (L<sup><i>B</i></sup>)<sup>4ā</sup> becomes oxidized, resulting in the formation of a rare example of
a biradical (ā¢L<sup><i>B</i></sup>ā¢)<sup>2ā</sup> bridge connecting two metal ions, as supported by X-ray crystallography.
The electronic structures of the complexes have been probed by MoĢssbauer
spectroscopy, magnetic susceptibility measurements, and electron paramagnetic
resonance (EPR) spectroscopy. Species <b>1</b> contains two
high-spin FeĀ(III) ions (<i>S</i> = 5/2) each coupled strongly
antiferromagnetically (|<i>J</i>| > 150 cm<sup>ā1</sup>; <b>HĢ</b> = ā<i>2J</i><b>SĢ</b><sub>1</sub><b>SĢ</b><sub>2</sub>) with a semiquinone
Ļ-radical (<i>S</i> = 1/2) form of the bridging (ā¢L<sup><i>B</i></sup>ā¢)<sup>2ā</sup> ligand. The
effective <i>S</i> = 2 spins of each [FeĀ(III)+R<sup>ā</sup>] monomeric unit are then weakly ferromagnetically coupled with <i>J</i> = +0.22 cm<sup>ā1</sup>. Species <b>2</b> and <b>3</b> reveal very similar electronic structures: the
low-spin CoĀ(III) ion is diamagnetic, which leaves the two-spin carriers
at the bridging (ā¢L<sup><i>B</i></sup>ā¢)<sup>2ā</sup> biradical to display an isotropic EPR signal at <i>g</i> = 1.995 for <b>2</b> (1.993 for <b>3</b>)
in solution at room temperature and in the frozen state with no hyperfine
structure. The weak half-field signal at <i>g</i> = 3.988
for <b>2</b> (3.978 for <b>3</b>) was also observed at
17 K for the spin-forbidden |Ī<i>M</i><sub>S</sub>| = 2 transition due to ferromagnetically coupled <i>S</i> = 1/2 spins (<i>J</i> = +47 cm<sup>ā1</sup>) of
the bridging biradical. The compounds show rich electrochemistry,
displaying two (<b>1</b>) or four (<b>2</b>, <b>3</b>) one-electron reversible processes. Normal and differential pulse
voltammetry as well as constant potential coulometry, combined with
EPR experiments, confirmed that the observed electron transfers are
all localized at the bridging noninnocent (ā¢L<sup><i>B</i></sup>ā¢)<sup>2ā</sup> ligand