5 research outputs found
Magnetic Dipolar Interactions in Solid Gold Nanosphere Dimers
We report the first observation of a magnetic dipolar
contribution
to the nonlinear optical (NLO) response of colloidal metal nanostructures.
Second-order NLO responses from several individual solid gold nanosphere
(SGN) dimers, which we prepared by a bottom-up approach, were examined
using polarization-resolved second harmonic generation (SHG) spectroscopy
at the single-particle level. Unambiguous circular dichroism in the
SH signal was observed for most of the dimeric colloids, indicating
that the plasmon field located within the interparticle gap was chiral.
Detailed analysis of the polarization line shapes of the SH intensities
obtained by continuous polarization variation suggested that the effect
resulted from strong magnetic-dipole contributions to the nanostructure’s
optical properties
Three-Dimensional Interfacial Structure Determination of Hollow Gold Nanosphere Aggregates
The boundary regions between hollow gold nanospheres (HGNs) comprising an extended aggregate were examined using 3-D electron tomography. The images obtained from these experiments allowed for precise determination of the 3-D arrangement of the HGNs within the aggregate and revealed structural heterogeneities that were not resolvable with traditional two-dimensional techniques. These features included particle necking, point contacts, lattice pinholes, and HGN cavities that were joined by pores. The theoretical influence of these interfacial substructures on nanoscale plasmon properties was assessed using finite difference time domain (FDTD) numerical simulations. These results demonstrated the prospective impact of 3-D imaging techniques on the development of complete-structure descriptions of nanoscale optical properties
Ultrafast Spectroscopic Signature of Charge Transfer between Single-Walled Carbon Nanotubes and C<sub>60</sub>
The time scales for interfacial charge separation and recombination play crucial roles in determining efficiencies of excitonic photovoltaics. Near-infrared photons are harvested efficiently by semiconducting single-walled carbon nanotubes (SWCNTs) paired with appropriate electron acceptors, such as fullerenes (<i>e</i>.<i>g</i>., C<sub>60</sub>). However, little is known about crucial photochemical events that occur on femtosecond to nanosecond time scales at such heterojunctions. Here, we present transient absorbance measurements that utilize a distinct spectroscopic signature of charges within SWCNTs, the absorbance of a trion quasiparticle, to measure both the ultrafast photoinduced electron transfer time (τ<sub>pet</sub>) and yield (ϕ<sub>pet</sub>) in photoexcited SWCNT–C<sub>60</sub> bilayer films. The rise time of the trion-induced absorbance enables the determination of the photoinduced electron transfer (PET) time of τ<sub>pet</sub> ≤ 120 fs, while an experimentally determined trion absorbance cross section reveals the yield of charge transfer (ϕ<sub>pet</sub> ≈ 38 ± 3%). The extremely fast electron transfer times observed here are on par with some of the best donor:acceptor pairs in excitonic photovoltaics and underscore the potential for efficient energy harvesting in SWCNT-based devices
Charge Transfer Dynamics between Carbon Nanotubes and Hybrid Organic Metal Halide Perovskite Films
In
spite of the rapid rise of metal organic halide perovskites
for next-generation solar cells, little quantitative information on
the electronic structure of interfaces of these materials is available.
The present study characterizes the electronic structure of interfaces
between semiconducting single walled carbon nanotube (SWCNT) contacts
and a prototypical methylammonium lead iodide (MAPbI<sub>3</sub>)
absorber layer. Using photoemission spectroscopy we provide quantitative
values for the energy levels at the interface and observe the formation
of an interfacial dipole between SWCNTs and perovskite. This process
can be ascribed to electron donation from the MAPbI<sub>3</sub> to
the adjacent SWCNT making the nanotube film <i>n</i>-type
at the interface and inducing band bending throughout the SWCNT layer.
We then use transient absorbance spectroscopy to correlate this electronic
alignment with rapid and efficient photoexcited charge transfer. The
results indicate that SWCNT transport and contact layers facilitate
rapid charge extraction and suggest avenues for enhancing device performance
Photoluminescence Imaging of Polyfluorene Surface Structures on Semiconducting Carbon Nanotubes: Implications for Thin Film Exciton Transport
Single-walled
carbon nanotubes (SWCNTs) have potential to act as
light-harvesting elements in thin film photovoltaic devices, but performance
is in part limited by the efficiency of exciton diffusion processes
within the films. Factors contributing to exciton transport can include
film morphology encompassing nanotube orientation, connectivity, and
interaction geometry. Such factors are often defined by nanotube surface
structures that are not yet well understood. Here, we present the
results of a combined pump–probe and photoluminescence imaging
study of polyfluorene (PFO)-wrapped (6,5) and (7,5) SWCNTs that provide
additional insight into the role played by polymer structures in defining
exciton transport. Pump–probe measurements suggest exciton
transport occurs over larger length scales in films composed of PFO-wrapped
(7,5) SWCNTs, compared to those prepared from PFO-bpy-wrapped (6,5)
SWCNTs. To explore the role the difference in polymer structure may
play as a possible origin of differing transport behaviors, we performed
a photoluminescence imaging study of individual polymer-wrapped (6,5)
and (7,5) SWCNTs. The PFO-bpy-wrapped (6,5) SWCNTs showed more uniform
intensity distributions along their lengths, in contrast to the PFO-wrapped
(7,5) SWCNTs, which showed irregular, discontinuous intensity distributions.
These differences likely originate from differences in surface coverage
and suggest the PFO wrapping on (7,5) nanotubes produces a more open
surface structure than is available with the PFO-bpy wrapping of (6,5)
nanotubes. The open structure likely leads to improved <i>intertube</i> coupling that enhances exciton transport within the (7,5) films,
consistent with the results of our pump–probe measurements