3 research outputs found
Ligand Coordination and Spin Crossover in a Nickel Porphyrin Anchored to Mesoporous TiO<sub>2</sub> Thin Films
The coordination and spin equilibrium
of a Ni<sup>II</sup> <i>meso</i>-tetra(4-carboxyphenyl)porphyrin
compound, NiP,
was quantified both in fluid solution and when anchored to mesoporous,
nanocrystalline TiO<sub>2</sub> thin films. This comparison provides
insights into the relative rate constants for excited-state injection
and ligand field population. In the presence of pyridine, the spectroscopic
data were consistent with the presence of equilibrium concentrations
of a 4-coordinate low-spin <i>S</i> = 0 (<sup>1</sup>A<sub>1g</sub>) Ni<sup>II</sup> compound and a high-spin <i>S</i> = 1 (<sup>3</sup>B<sub>1g</sub>) 6-coordinate compound. Temperature-dependent
equilibrium constants were consistently smaller for the surface-anchored
NiP/TiO<sub>2</sub>, as were the absolute values of Δ<i>H</i> and Δ<i>S</i>. In the presence of diethylamine
(DEA), the ground-state 6-coordinate compound was absent, but evidence
for it was present after pulsed light excitation of NiP. Arrhenius
analysis of data, measured from −40 to −10 °C,
revealed activation energies for ligand dissociation that were the
same for the compound in fluid solution and anchored to TiO<sub>2</sub>, <i>E</i><sub>a</sub> = 6.6 kcal/mol, within experimental
error. At higher temperatures, a significantly smaller activation
energy of 3.5 kcal/mol was found for NiP(DEA)<sub>2</sub>/TiO<sub>2</sub>. A model is proposed wherein the TiO<sub>2</sub> surface
sterically hinders ligand coordination to NiP. The lack of excited-state
electron transfer from Ni<sup>II</sup>P*/TiO<sub>2</sub> indicates
that internal conversion to ligand field states was at least 10 times
greater than that of excited-state injection into TiO<sub>2</sub>
Increase in the Coordination Number of a Cobalt Porphyrin after Photo-Induced Interfacial Electron Transfer into Nanocrystalline TiO<sub>2</sub>
Spectroscopic, electrochemical, and kinetic data provide
compelling
evidence for a coordination number increase initiated by interfacial
electron transfer. Light excitation of Co<sup>I</sup>(<i>meso-</i>5,10,15,20-tetrakis(4-carboxyphenyl)porphyrin) anchored to a nanocrystalline
TiO<sub>2</sub> thin film, abbreviated Co<sup>I</sup>P/TiO<sub>2</sub>, immersed in an acetonitrile:pyridine electrolyte resulted in rapid
excited state injection, <i>k</i><sub>inj</sub> > 10<sup>8</sup> s<sup>–1</sup>, to yield Co<sup>II</sup>P/TiO<sub>2</sub>(e<sup>–</sup>), followed by axial coordination of
pyridine to the Co<sup>II</sup>P and hence an increase in coordination
number from four to five. The formal oxidation state and coordination
environment of the Co metalloporphyrin on TiO<sub>2</sub> were assigned
through comparative studies in fluid solution as well as by comparisons
to previously reported data. The kinetics for pyridine coordination
were successfully modeled with a pseudo-first order kinetic model
that yielded a second-order rate constant of <i>k</i><sub>+py</sub> = 2 × 10<sup>8</sup> M<sup>–1</sup> s<sup>–1</sup>. Spectro-electrochemical measurements showed that pyridine coordination
resulted in a ∼200 mV negative shift in the Co<sup>II/I</sup> reduction potential, <i>E</i>°(Co<sup>II/I</sup>/TiO<sub>2</sub>) = −0.72 V and <i>E</i>°(Co<sup>II/I</sup>(py)/TiO<sub>2</sub>) = −0.85 V vs NHE. With some assumptions,
this indicated an equilibrium formation constant <i>K</i><sub>f</sub> = 400 M<sup>–1</sup> for the Co<sup>II</sup>P(py)/TiO<sub>2</sub> compound. The kinetics for charge recombination
were non-exponential under all conditions studied, but were successfully
modeled by the Kohlrausch–Williams–Watts (KWW) function
with observed rate constants that decreased by about a factor of 100
when pyridine was present. The possible mechanisms for charge recombination
are discussed
Non-Nernstian Two-Electron Transfer Photocatalysis at Metalloporphyrin–TiO<sub>2</sub> Interfaces
A long-standing question in the photochemical sciences concerns how to integrate single-electron transfers to catalytic multielectron transfer reactions that produce useful chemical fuels. Here we provide a strategy for the two-electron formation of C–C bonds with molecular catalysts anchored to semiconductor nanocrystallites. The blue portion of the solar spectrum provides band gap excitation of the semiconductor while longer wavelengths of light initiate homolytic cleavage of metal–carbon bonds that, after interfacial charge transfer, restore the catalyst. The semiconductor utilized was the anatase polymorph of TiO2 present as a nanocrystalline, mesoporous thin film. The catalyst was cobalt meso-5,10,15,20-tetrakis(4-carboxyphenyl)porphyrin chloride, Co(TCPP)Cl. For this catalyst and iron protoporphyrin IX chloride, Fe(PPIX)Cl, two distinct and sequential metal-based MIII/II and MII/I reductions were observed under band gap illumination. Spectroelectrochemical characterization indicated that both reductions were non-Nernstian, behavior attributed to an environmentally dependent potential drop across the molecule–semiconductor interface. Reaction of CoI(TCPP)/TiO2 with organobromides (RBr = 1-Br-hexane or benzyl bromide) resulted in the formation of CoIII–R(TCPP)/TiO2. Visible light excitation induced homolytic cleavage of the Co–C bond and the formation of C–C-bonded products. The reactions were catalytic when band gap excitation or an electrochemical bias provided TiO2 electrons to the oxidized catalyst. Sustained photocurrents were quantified in photoelectrosynthetic solar cells under forward bias
