12 research outputs found
Lattice Registry and Evidence for Surface Reconstructions of Metal Films on Suspended 2D Membranes Following Annealing
Controlling Morphology and Excitonic Disorder in Monolayer WSe2 Grown by Salt-Assisted CVD Methods
Characterizing Multi-layer Pristine Graphene, Its Contaminants, and Their Origin Using Transmission Electron Microscopy
Ultraviolet and Visible Photochemistry of Methanol at 3D Mesoporous Networks: TiO<sub>2</sub> and Au–TiO<sub>2</sub>
Comparison of methanol photochemistry
at three-dimensionally (3D)
networked aerogels of TiO<sub>2</sub> or Au–TiO<sub>2</sub> reveals that incorporated Au nanoparticles strongly sensitize the
oxide nanoarchitecture to visible light. Methanol dissociatively adsorbs
at the surfaces of TiO<sub>2</sub> and Au–TiO<sub>2</sub> aerogels
under dark, high-vacuum conditions. Upon irradiation of either ultraporous
material with broadband UV light under anaerobic conditions, adsorbed
methoxy groups act as hole-traps and extend conduction-band and shallow-trapped
electron lifetimes. A higher excited-state electron density arises
for UV-irradiated TiO<sub>2</sub> aerogel relative to commercial nanoparticulate
TiO<sub>2</sub>, indicating that 3D networked TiO<sub>2</sub> more
efficiently separates electron–hole pairs. Upon excitation
with narrow-band visible light centered at 550 nm, long-lived excited-state
electrons are evident on CH<sub>3</sub>OH-exposed Au–TiO<sub>2</sub> aerogelsbut not on identically dosed TiO<sub>2</sub> aerogelsverifying that incorporated Au nanoparticles sensitize
the networked oxide to visible light. Under aerobic conditions (20
Torr O<sub>2</sub>) and broadband UV illumination, surface-sited formates
accumulate as adsorbed methoxy groups oxidize, at similar rates, on
Au–TiO<sub>2</sub> and TiO<sub>2</sub> aerogels. Moving to
excitation wavelengths longer than ∼400 nm (i.e., the low-energy
range of UV light) dramatically decreases methoxy photoconversion
for methanol-saturated TiO<sub>2</sub> aerogel, while Au–TiO<sub>2</sub> aerogel remains highly active for methanol photooxidation.
The wavelength dependence of formate production on Au–TiO<sub>2</sub> tracks the absorbance spectrum for this material, which peaks
at λ = 550 nm due to resonance with the surface plasmon in the
Au particles. The photooxidation rate for Au–TiO<sub>2</sub> aerogel at 550 nm is comparable to that for TiO<sub>2</sub> aerogel
under broadband UV illumination, indicating efficient energy transfer
from Au to TiO<sub>2</sub> in the 3D mesoporous nanoarchitecture
Correlating Changes in Electron Lifetime and Mobility on Photocatalytic Activity at Network-Modified TiO 2
Plasmonic Aerogels as a Three-Dimensional Nanoscale Platform for Solar Fuel Photocatalysis
We use plasmonic Au–TiO<sub>2</sub> aerogels as a platform
in which to marry synthetically thickened particle–particle
junctions in TiO<sub>2</sub> aerogel networks to Au∥TiO<sub>2</sub> interfaces and then investigate their cooperative influence
on photocatalytic hydrogen (H<sub>2</sub>) generation under both broadband
(i.e., UV + visible light) and visible-only excitation. In doing so,
we elucidate the dual functions that incorporated Au can play as a
water reduction cocatalyst and as a plasmonic sensitizer. We also
photodeposit non-plasmonic Pt cocatalyst nanoparticles into our composite
aerogels in order to leverage the catalytic water-reducing abilities
of Pt. This Au–TiO<sub>2</sub>/Pt arrangement in three dimensions
effectively utilizes conduction−band electrons injected into
the TiO<sub>2</sub> aerogel network upon exciting the Au SPR at the
Au∥TiO<sub>2</sub> interface. The extensive nanostructured
high surface-area oxide network in the aerogel provides a matrix that
spatially separates yet electrochemically connects plasmonic nanoparticle
sensitizers and metal nanoparticle catalysts, further enhancing solar-fuels
photochemistry. We compare the photocatalytic rates of H<sub>2</sub> generation with and without Pt cocatalysts added to Au–TiO<sub>2</sub> aerogels and demonstrate electrochemical linkage of the SPR-generated
carriers at the Au∥TiO<sub>2</sub> interfaces to downfield
Pt nanoparticle cocatalysts. Finally, we investigate visible light–stimulated
generation of conduction band electrons in Au–TiO<sub>2</sub> and TiO<sub>2</sub> aerogels using ultrafast visible pump/IR probe
spectroscopy. Substantially more electrons are produced at Au–TiO<sub>2</sub> aerogels due to the incorporated SPR-active Au nanoparticle,
whereas the smaller population of electrons generated at Au-free TiO<sub>2</sub> aerogels likely originate at shallow traps in the high surface-area
mesoporous aerogel
Synthesis and Characterization of PbS/ZnS Core/Shell Nanocrystals
We
demonstrate a synthetic method to add a ZnS shell, with controlled
thickness, to PbS nanocrystals using Zn oleate and thioacetamide as
Zn and S precursors. The ZnS shell reaction is self-limiting and deposits
approximately a monolayer of ZnS per shell reaction without causing
the PbS nanocrystals to Ostwald ripen. The reaction is self-limiting
because the sulfur precursor, thioacetamide, is less reactive toward
the PbS/ZnS core/shell nanocrystal surface as compared to the Zn oleate
precursor present in the reaction solution. To increase the ZnS shell
thickness beyond a monolayer, subsequent ZnS shell reactions are modified
by adding the thioacetamide 10 minutes before the Zn oleate. This
gives the thioacetamide time to react at the PbS/ZnS core/shell nanocrystal
surface before the Zn oleate is added. High angle annular dark field
scanning transmission electron microscopy (HAADF-STEM) shows most
ZnS shells lack crystalline order. However, select core/shell nanocrystals
have epitaxial crystalline (zinc-blende) ZnS shells or crystalline
(zinc-blende) shells with no obvious epitaxial relationship to the
PbS core. The PbS core 1S<sub>h</sub>–1S<sub>e</sub> absorbance
and photoluminescence peak energies redshift upon shell addition due
to relief of a ligand-induced tensile strain and wave function leakage
into the shell. The photoluminescence quantum yield decreases after
ZnS shell addition likely due to nonradiative defect states at the
core/shell interface
Correlating Changes in Electron Lifetime and Mobility on Photocatalytic Activity at Network-Modified TiO<sub>2</sub> Aerogels
We use intensity-modulated photovoltage
spectroscopy (IMVS) and intensity-modulated photocurrent spectroscopy
(IMPS) to characterize carrier dynamics in titania (TiO<sub>2</sub>) aerogels under photocatalytic conditions. By systematically increasing
the weight fraction of the sol–gel precursor during TiO<sub>2</sub> sol–gel synthesis, we are able to impart drastic changes
in carrier transport/trapping and improve the photocatalytic activity
of TiO<sub>2</sub> aerogels for two mechanistically divergent photochemical
reactions: reductive water splitting (H<sub>2</sub> generation) and
oxidative degradation of dichloroacetate (DCA). The lifetimes of photogenerated
electrons increase in going from lowest-to-highest precursor concentrations,
as measured by IMVS, indicating increasing site density for electron
trapsî—¸a trend that correlates with an 8Ă— improvement for
photocatalytic H<sub>2</sub> generation. Electron mobility in the
aerogel films, as measured by IMPS, decreases with increasing trap
density, further implicating the trapping sites as reactive sites.
In contrast, photocatalytic DCA degradationî—¸driven primarily
by direct hole transfer to adsorbed DCAî—¸depends only weakly
on the electron dynamics in the film. Transient infrared spectroscopy
shows no difference in carrier decay among the aerogel samples on
picosecond time scales, indicating that changes in carrier dynamics
within these networked nanomaterials are only observable at time scales
measured by IMPV and IMPS. Correlating hole-mediated and electron-mediated
photocatalytic activity with direct measurement of electron dynamics
under photocatalytically relevant conditions and time scales comprises
a powerful approach to determine how synthetic modifications to networked
nanostructured photocatalysts affect the relevant physicochemical
phenomena underlying their photocatalytic performance