15 research outputs found
Effects of Embedded Dipole Layers on Electrostatic Properties of Alkanethiolate Self-Assembled Monolayers
Enhancement of Photoexcited Charge Transfer by {001} Facet-Dominating TiO<sub>2</sub> Nanoparticles
The recent discovery of a synthetic method for chemically reactive {001} facet-dominating TiO<sub>2</sub> nanoparticles using hydrofluoric acid provided a new aspect of interfacial chemistry in photo catalysts, batteries, and photoelectrochemical cells using TiO<sub>2</sub>. We reveal the effects of the reactive {001} facet on the photoexcited charge transfer from organic fluorophores, 9-substituted anthracene derivatives (An–X; X = H and COOH) and tetracene, to TiO<sub>2</sub> nanoparticles by differing the fraction of {001} facet. The kinetic analysis of the fluorescence quenching by TiO<sub>2</sub> nanoparticles based on Stern–Volmer relation is employed to estimate the quenching rate constant as a function of the fraction of {001} facet. The results imply a significant enhancement of the photoexcited charge transfer from fluorophores to TiO<sub>2</sub> nanoparticles by the reactive {001} facet with a factor of more than 10 in the quenching rate constant at maximum
Sequential Coupling Approach to the Synthesis of Nickel(II) Complexes with <i>N</i>‑aryl-2-amino Phenolates
A sequential multicomponent coupling approach is a powerful
method for the construction of combinatorial libraries because structurally
complex and diverse molecules can be synthesized from simple materials
in short steps. In this paper, an efficient synthesis of nickel(II)
complexes with <i>N</i>-aryl-2-amino phenols via a sequential
three-step coupling approach is described, for potential use in nonlinear
optical materials, bioinspired catalytic systems, and near-infrared
absorbing filters. Seventeen <i>N</i>-aryl-2-amino phenolates
were successfully synthesized in high yields based on the coupling
of 3,5-di-<i>tert</i>-butylbenzene-1,2-diol with a pivotal
aromatic scaffold, 4-bromo-2-iodo-aniline, followed by sequential
Suzuki–Miyaura coupling with aryl boronates. A total of 16
analytically pure nickel(II) complexes with <i>N</i>-aryl-2-amino
phenolates were obtained from 17 complexation trials. The procedure
allowed us to assemble 4 components in high yields without protection,
deprotection, oxidation or reduction steps. Various building blocks
that included electron-donating, electron-withdrawing, and basic were
used, and readily available, nontoxic and environmentally benign substrates
and reagents were employed with no generation of toxic compounds.
No strict anhydrous or degassed conditions were required. Absorption
spectroscopic measurement of the synthesized nickel(II) complexes
revealed that the <i>ortho</i>-substituent Ar<sup>1</sup> exerted more influence on the absorption wavelength of the complexes
than the <i>para</i>-substituent Ar<sup>2</sup>. On the
other hand, both substituents Ar<sup>1</sup> and Ar<sup>2</sup> influenced
the molar absorptivity values. These observations should be useful
for the design of new and useful nickel(II) complexes as near-infrared
chromophores
Precise Control of Photoinduced Electron Transfer in Alternate Layered Nanostructures of Titanium Oxide–Tungsten Oxide
The alternate layered structure was
synthesized by the thiol–ene
click reaction between the alkylthiol-modified tungsten oxide layer
and the alkene-modified titanium oxide layer. The interlayer distances
between the titanium oxide layer and the tungsten oxide layer were
controlled to 0.72, 0.94, 1.01, and 1.14 nm by changing the carbon
number of the functional groups. Photoinduced electron transfer from
the titanium oxide layer to the tungsten oxide layer depends on the
interlayer distance of the titanium oxide–tungsten oxide alternate
layers from 0.7 to 1.1 nm. The alternate layers of narrow interlayer
distance showed high photocatalytic activity in decomposition of methylene
blue. The amount of the photoexcited electron transfer from titanium
oxides to tungsten oxides was quantitatively measured by the reduction
of Ag ions with the electrons stored in tungsten oxide. Because the
rate of photoinduced electron transfer should be proportional to the
amount of electron transfer, the tunneling decay constant β
was estimated to be 0.63 Å<sup>–1</sup> in the alternate
layer samples, indicating that electrons transfer from titanium oxide
to tungsten oxide by through-space tunneling
Effects of energetics with {001} facet-dominant anatase TiO2 scaffold on electron transport in CH3NH3PbI3 perovskite solar cells
The anatase titania with large fraction of {001} facet on the mesoscopic anatase titania scaffold in the hybrid perovskite solar cells exhibited higher photocurrent and open-circuit voltage. The higher performance with {001}-dominant anatase titania with the fraction of 74% were discussed with the characteristic electron transport properties in addition to the energy levels of trap states and conduction band as compared with those properties of conventional anatase titania scaffold. The resulted higher photocurrent and open-circuit voltage were attributed to the enhancement of the electron injection and suppression of the carrier recombination, respectively, at the titania/perovskite semiconductor interface.NRF (Natl Research Foundation, S’pore)MOE (Min. of Education, S’pore)Accepted versio
Electromagnetic and Heat-Transfer Simulation of the Catalytic Dehydrogenation of Ethylbenzene under Microwave Irradiation
Electromagnetic and heat-transfer
simulations were used to study
the effects of microwave-generated nonuniform temperature distributions
in a catalyst bed on the rate enhancement of a fixed-bed flow reaction.
We used the dehydrogenation of ethylbenzene over a magnetite catalyst
as a model reaction. During the microwave reaction, a temperature
gradient was generated in the catalyst bed; the highest temperature
occurred at the core of the catalyst bed, and it parabolically decreased
toward the surface. Using these simulation results and Arrhenius parameters,
the reaction rates were estimated by considering the nonuniform temperature
distribution. The measured reaction rate was 36% larger than the simulated
value, indicating that the rate enhancement under microwaves can not
only be attributed to the nonuniform temperature distribution in the
catalyst bed. This could be due to nonequilibrium local heating (the
so-called hot spot) in the very small region around the catalyst particle
Microwave Effects on Co–Pi Cocatalysts Deposited on α‑Fe<sub>2</sub>O<sub>3</sub> for Application to Photocatalytic Oxygen Evolution
We analyze the effects of microwave
applied in the process of photoelectrochemical
deposition of cobalt-based cocatalysts, Co–Pi, onto well-orientated
flat α-Fe<sub>2</sub>O<sub>3</sub> thin films, which were fabricated
by pulsed laser deposition. As compared with conventional heating,
microwave significantly affects the morphology, chemical composition,
and photocatalytic activity of Co-Pi/α-Fe<sub>2</sub>O<sub>3</sub> composite. A significant enhancement in photocurrent related to
photocatalytic water oxidation is achieved by the Co–Pi catalyst
prepared under microwave irradiation. This, along with its interfacial
electron-transfer properties, is studied by means of electrochemical
impedance spectroscopy