In photocatalytic
reactions, the interfacial transfer of electrons
from semiconductor nanostructures to cocatalysts is the key step that
determines the utilization of photogenerated charges and is sensitively
influenced by the behaviors of this electronic process. Under weak
illumination, photocatalytic reaction rates deviate from linearity
to incident light intensity (r = k
ss·P
inc
α, with α → 0.5), because charge recombination predominates
interfacial transfer. When the irradiation intensity is high, theoretically,
thermionic emission would be the major electronic process (r = k
te·P
inc
α, with α → 2). The ratio
of photocatalytic reaction rate to incident light intensity that mainly
reflects the energy utilization would encounter a minimum along the
variation of irradiation intensity. This crucial relationship, however,
has hardly been consciously considered. In this work, inspired by
theoretical simulation, we demonstrate that sunlight-driven photocatalysis
is generally on the bottom of the energy utilization curves for certain
common semiconductors (CdS, TiO2, or C3N4).
We report a new and effective method to prepare high activity graphitic carbon nitride (g-C3N4) by a simple ammonia etching treatment. The obtained g-C3N4 displays a high BET surface area and enhanced electron/hole separation efficiency. The hydrogen evolution rates improved from 52 μmol h(-1) to 316.7 μmol h(-1) under visible light.
The construction of C−C bonds by coupling reactions is an important process in synthetic chemistry though expensive catalysts are required. Heterogeneous photocatalysis offers a platform for C−C coupling of aromatic halides via hydro-dehalogenation by employing alcohols as the hydrogen donor; however, a designed photocatalyst with high activity and selectivity is lacking. Here, we show that Cu is a promising candidate to promote the coupling of aromatic halides due to the optimized adsorption energy of the reaction intermediates (benzyl radical and Br atom) over a series of transition metals. The Cu-modified TiO 2 shows a remarkable apparent quantum efficiency (15%) and a great tolerance of harsh reaction conditions for the homocoupling of benzyl bromides into bibenzyl under UV irradiation. The low-cost photocatalyst also shows high performance upon scaling-up and selective coupling of a series of benzyl bromide derivatives, demonstrating the heterogeneous photocatalytic C−C coupling as an attractive process for applications. Additionally, the design strategy can be applied to modify other photocatalysts (i.e., g-C 3 N 4 ) to realize the C−C coupling of benzyl bromide under visible light.
Metal nanoparticles (NPs) are heavily involved in photocatalytic transformations to manipulate charge separation and storage, yet the catalytic role of metal NPs in tuning the selectivity of photoreactions is rarely addressed. Here, the photodehydrogenative coupling of primary amines is selected as the model reaction to probe the catalytic role of Pt and Pd NPs supported on graphitic carbon nitride (Pt/C 3 N 4 and Pd/C 3 N 4 ). When Pt/C 3 N 4 is employed as the photocatalyst, imine is produced via dehydrogenative homocoupling of primary amines owing to the weak adsorption of photogenerated imines and H atoms on Pt NPs. In comparison, Pd/C 3 N 4 promotes the consecutive hydrogenation of photogenerated imines into secondary amines due to a strong affinity of both imine and H atom for the surface of Pd NPs. This strategy is applicable for the synthesis of a series of imines and secondary amines with high yields.
Despite thermodynamic
feasibility, the high activation energy originating
from potential barriers and trap states kinetically prevents the interfacial
transfer of electrons from semiconductor nanostructures to reduction
cocatalysts, resulting in a lowered utilization of photogenerated
charge carriers in photocatalysis. Nanostructuring-induced narrowing
of potential barriers offers a rational solution to kinetically facilitate
interfacial electron transfer by tunneling. Here, inspired by theoretical
simulation, we manage to promote the separation of photogenerated
charge carriers by coating the semiconductor nanostructures with a
homogeneous interlayer. The low activation energy for interfacial
electron transfer endows photocatalysis with nearly constant quantum
yields and a quasi-first-order reaction to the incident photons and
grants evident superiority over the photocatalyst without interlayers,
especially under sunlight. In our demonstrated sunlight-driven hydrogen
evolution integrated with benzylamine oxidation, the production rates
for both reduction and oxidation half-reactions reach as high as ∼0.77
mmol dm–2 h–1, which are ∼10
times higher than that without an interlayer.
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