2 research outputs found
Iridium(III) Mediated Reductive Transformation of Closed-Shell Azo-Oxime to Open-Shell Azo-Imine Radical Anion: Molecular and Electronic Structure, Electron Transfer, and Optoelectronic Properties
The hydrogen bonded bis azo-oximato
[IrCl<sub>2</sub>(L<sup>NOH</sup>)Â(L<sup>NO</sup>)] <b>2</b> and its deprotonated form (Et<sub>3</sub>NH)Â[IrCl<sub>2</sub>(L<sup>NO</sup>)<sub>2</sub>] <b>(Et</b><sub><b>3</b></sub><b>NH)</b><sup><b>+</b></sup><b>3</b><sup><b>–</b></sup> have been isolated in the crystalline state by a facile synthetic
method. The azo-oxime frameworks in <b>3</b><sup><b>–</b></sup> have been conveniently transformed to the azo-imine by reduction
with NaBH<sub>4</sub> or ascorbic acid. Notably, the coordinated azo-imines
accept an extra electron thereby furnishing the azo-imine radical
anion complex <b>4</b>. The underlying reductive transformation
can be best described by proton-coupled electron transfer (PCET) process.
Both the coordinated ligands (azo-oxime) in <b>3</b><sup><b>–</b></sup> are typically closed-shell monoanion (L<sup>NO–</sup>), but their reduced form (azo-imine) can behave
as open-shell monoanion (L<sup>NH•–</sup>) owing to
the presence of highly stabilized virtual orbitals. Remarkable enhancement
of the π-acidity in azo-imine relative to the precursor azo-oxime
has also been reflected from the electrochemical study. The irido
complexes display rich optoelectronic properties, and the origin of
the transitions has been scrutinized by the TD-DFT method. The molecular
geometries of the complexes <b>2</b> and <b>3</b><sup><b>–</b></sup> reveal that the <i>syn</i> orientation
of the azo-oximes frameworks is favored because of strong noncovalent
H-bonding and π–π stacking interactions. In the
course of the reduction of <b>3</b><sup><b>–</b></sup>, the sterically encumbered disposition of the azo-oximes is
converted to the relaxed <i>anti</i> form in the transformed
azo-imines. Diffraction study reveals the electronic structure of <b>4</b> as [Ir<sup>III</sup>Cl<sub>2</sub>{(L<sup>NH</sup>)<sub>2</sub><sup>•–</sup>}]. The superior stabilization
of the unpaired spin on the ligand array rather than metal has also
been substantiated from EPR and DFT studies. Theoretical analysis
reveals that the odd electron delocalizes primarily over both the
azo-imine moieties ([IrCl<sub>2</sub>(L<sup>NH•–</sup>)Â(L<sup>NH</sup>)] ↔ ([IrCl<sub>2</sub>(L<sup>NH</sup>)Â(L<sup>NH•–</sup>)]) with no apparent contribution from metal,
and this type of ligand-centered mixed valency (LCMV) can be best
expressed as Robin–Day class III (fully delocalized) in nature
Ambient-Stable Bis-Azoaromatic-Centered Diradical [(L<sup>•</sup>)M(L<sup>•</sup>)] Complexes of Rh(III): Synthesis, Structure, Redox, and Spin–Spin Interaction
Bis-azoaromatic electron
traps, viz. 2-(2-pyridylazo)Âazoarene <b>1</b>, have been synthesized
by colligating electron-deficient pyridine and azoarene moieties,
and they act as apposite proradical templates for the formation of
stable open-shell diradical complexes [(<b>1</b><sup>•–</sup>)ÂRh<sup>III</sup>(<b>1</b><sup>•–</sup>)]<sup>+</sup> ([<b>2</b>]<sup>+</sup>), starting from the low-valent
electron reservoir [Rh<sup>I</sup>]. The less stable monoradical [Rh<sup>III</sup>(<b>1</b><sup>•–</sup>)ÂCl<sub>2</sub>(PPh<sub>3</sub>)<sub>3</sub>] (<b>3</b>) has also been isolated
as a minor product. These π-radical complexes are multiredox
systems, and the electron transfer processes occur exclusively within
the pincer-type NNN ligand backbone <b>1</b>. Molecular and
electronic structures of the diradicals and monoradicals have been
ascertained with the aid of X-ray diffraction, electrochemical, spectroelectrochemical,
and spectral (electronic, IR, NMR, and EPR) studies. In the diradicals
[<b>2</b>]<sup>+</sup>, the orthogonal disposition of two ligand
Ï€ orbitals linked via a closed-shell metal center (t<sub>2</sub><sup>6</sup>) impedes significant coupling between the radicals.
Indeed, the observed magnetic moment of [<b>2a</b>]<sup><b>+</b></sup> lies near ∼2.3 μ<sub>B</sub> over the
temperature range 50–300 K. A very weak antiferromagnetic (AF)
intramolecular spin–spin interaction between two ligand π
arrays in [<b>(1</b><sup>•–</sup>)ÂRh<sup>III</sup>(<b>1</b><sup>•–</sup>)]<sup>+</sup> have been
found experimentally (<i>J</i> ≈ −5 cm<sup>–1</sup>), and this is further substantiated by density functional
theory (DFT) calculations at the (U)ÂB3LYP/6-31GÂ(d,p) level