48 research outputs found
[Ag<sub>25</sub>(SR)<sub>18</sub>]<sup>ā</sup>: The āGoldenā Silver Nanoparticle
Silver
nanoparticles with an atomically precise molecular formula
[Ag<sub>25</sub>(SR)<sub>18</sub>]<sup>ā</sup> (āSR:
thiolate) are synthesized, and their single-crystal structure is determined.
This synthesized nanocluster is the only silver nanoparticle that
has a virtually identical analogue in gold, i.e., [Au<sub>25</sub>(SR)<sub>18</sub>]<sup>ā</sup>, in terms of number of metal
atoms, ligand count, superatom electronic configuration, and atomic
arrangement. Furthermore, both [Ag<sub>25</sub>(SR)<sub>18</sub>]<sup>ā</sup> and its gold analogue share a number of features in
their optical absorption spectra. This unprecedented molecular analogue
in silver to mimic gold offers the first model nanoparticle platform
to investigate the centuries-old problem of understanding the fundamental
differences between silver and gold in terms of nobility, catalytic
activity, and optical property
Switching a Nanocluster Core from Hollow to Nonhollow
Modulating the structureāproperty
relationship in atomically
precise nanoclusters (NCs) is vital for developing novel NC materials
and advancing their applications. While promising biphasic ligand-exchange
(LE) strategies have been developed primarily to attain novel NCs,
understanding the mechanistic aspects involved in tuning the core
and the ligand-shell of NCs in such biphasic processes is challenging.
Here, we design a single phase LE process that enabled us to elucidate
the mechanism of how a hollow NC (e.g., [Ag<sub>44</sub>(SR)<sub>30</sub>]<sup>4ā</sup>, SR: thiolate) converts into a nonhollow NC
(e.g., [Ag<sub>25</sub>(SR)<sub>18</sub>]<sup>ā</sup>) and
vice versa. Our study reveals that the complete LE of the hollow [Ag<sub>44</sub>(SPhF)<sub>30</sub>]<sup>4ā</sup> NCs (SPhF: 4-fluorobenzenethiolate)
with incoming 2,4-dimethylbenzenethiol (HSPhMe<sub>2</sub>) induced
distortions in the Ag<sub>44</sub> structure forming the nonhollow
[Ag<sub>25</sub>(SPhMe<sub>2</sub>)<sub>18</sub>]<sup>ā</sup> by a disproportionation mechanism, while the reverse reaction of
[Ag<sub>25</sub>(SPhMe<sub>2</sub>)<sub>18</sub>]<sup>ā</sup> with HSPhF prompted an unusual dimerization of Ag<sub>25</sub>,
followed by a rearrangement step that reproduces the original [Ag<sub>44</sub>(SPhF)<sub>30</sub>]<sup>4ā</sup>. Remarkably, both
the forward and the backward reactions proceed through similar size
intermediates that seem to be governed by the boundary conditions
set by the thermodynamic and electronic stability of the hollow and
nonhollow metal cores. Furthermore, the resizing of NCs highlights
the surprisingly long-range effect of the ligands which are felt by
atoms far deep in the metal core, thus opening a new path for controlling
the structural evolution of nanoparticles
Neat and Complete: Thiolate-Ligand Exchange on a Silver Molecular Nanoparticle
Atomically precise thiolate-protected
noble metal molecular nanoparticles
are a promising class of model nanomaterials for catalysis, optoelectronics,
and the bottom-up assembly of true molecular crystals. However, these
applications have not fully materialized due to a lack of ligand exchange
strategies that add functionality, but preserve the properties of
these remarkable particles. Here we present a method for the rapid
(<30 s) and complete thiolate-for-thiolate exchange of the highly
sought after silver molecular nanoparticle [Ag<sub>44</sub>(SR)<sub>30</sub>]<sup>ā4</sup>. Only by using this method were we
able to preserve the precise nature of the particles and simultaneously
replace the native ligands with ligands containing a variety of functional
groups. Crucially, as a result of our method we were able to process
the particles into smooth thin films, paving the way for their integration
into solution-processed devices
Effect of Precursor Ligands and Oxidation State in the Synthesis of Bimetallic Nano-Alloys
The
characteristics of bimetallic nanomaterials are dictated by
their size, shape, and elemental distribution. Solution synthesis
is widely utilized to form nanomaterials, such as nanoparticles, with
controlled size and shape. However, the effects of variables on the
characteristics of bimetallic nanomaterials are not completely understood.
In this study, we used a continuous-flow synthetic strategy to explore
the effects of the precursor ligands and the precursor oxidation state
in the shape-controlled synthesis of platinum alloy nano-octahedra
and show their effect on the nanoparticle size and the elemental distribution
within the alloy nanoparticle. We demonstrate that this strategy can
tune the size of monodisperse PtM (M = Ni or Cu) alloy nanocrystals
ranging from 3 to 16 nm with an octahedral shape using acetylacetonate
or halide precursors of PtĀ(II), PtĀ(IV), and NiĀ(II) or CuĀ(II). The
nanoparticles formed from halide precursors showed an enrichment of
platinum on their surfaces, and the use bromide ligands in the presence
of air showed the formation of concave and uneven surface facets.
The two nanocrystal precursors can be utilized independently and can
control the size with a trend of PtĀ(acac)<sub>2</sub> < PtCl<sub>2</sub> < PtCl<sub>4</sub> < PtBr<sub>2</sub> < PtBr<sub>4</sub> and MĀ(acac)<sub>2</sub> < MCl<sub>2</sub> < MBr<sub>2</sub> for the secondary metal (copper or nickel). These results
open up avenues to understand the effect of the ligand shell of a
precursor during the synthesis of alloy nanoparticles as well as to
control, in a scalable manner, the nanomaterial size and surface chemistry
Room-Temperature Engineering of All-Inorganic Perovskite Nanocrsytals with Different Dimensionalities
Room-Temperature Engineering of All-Inorganic Perovskite
Nanocrsytals with Different Dimensionalitie
Synthesis and Optical Properties of a Dithiolate/Phosphine-Protected Au<sub>28</sub> Nanocluster
While
monothiols and simple phosphines are commonly exploited for
size-controlled synthesis of atomically precise gold nanoclusters
(NCs), dithiols or dithiol-phosphine combinations are seldom applied.
Herein, we used a dithiol (benzene-1,3-dithiol, BDT) and a phosphine
(triphenylphosphine, TPP) together as ligands and synthesized an atomically
precise gold NC with the formula [Au<sub>28</sub>(BDT)<sub>4</sub>(TPP)<sub>9</sub>]<sup>2+</sup>. This NC exhibited multiple absorption
features and a charge of +2, which are distinctly different from the
reported all-thiolated [Au<sub>28</sub>(SR)<sub>20</sub>]<sup>0</sup> NC (SR: monothiolate). The composition of [Au<sub>28</sub>(BDT)<sub>4</sub>(TPP)<sub>9</sub>]<sup>2+</sup> NC was deduced from high-resolution
electrospray ionization mass spectrometry (ESI MS) and it was further
corroborated by thermogravimetric analysis (TGA). Differential pulse
voltammetry (DPV) revealed a HOMOāLUMO gap of 1.27 eV, which
is in good agreement with the energy gap of 1.3 eV obtained from its
UVāvis spectrum. The successful synthesis of atomically precise,
dithiol-protected Au<sub>28</sub> NC would stimulate theoretical and
experimental research into bidentate ligands as a new path for expanding
the library of different metal NCs, which have so far been dominated
by monodentate thiols
Ligand-Free Nanocrystals of Highly Emissive Cs<sub>4</sub>PbBr<sub>6</sub> Perovskite
Although
ligands of long carbon chains are very crucial to form
stable colloidal perovskite nanocrystals (NCs), they create a severe
barrier for efficient charge injection or extraction in quantum-dot-based
optoelectronics, such as light emitting diode or solar cell. Here,
we report a new approach to preparing ligand-free perovskite NCs of
Cs<sub>4</sub>PbBr<sub>6</sub>, which retained high photoluminescence quantum yield (44%). Such an
approach involves a polar solvent (acetonitrile) and two small molecules
(ammonium acetate and cesium chloride), which replace the organic
ligand and still protect the nanocrystals from dissolution. The successful
removal of hydrophobic long ligands was evidenced by Fourier transform
infrared spectroscopy, Ī¶ potential analysis, and thermogravimetric
analysis. Unlike conventional perovskite NCs that are extremely susceptible
to polar solvents, the ligand-free Cs<sub>4</sub>PbBr<sub>6</sub> NCs
show robust resistance to polar solvents. Our ligand-free procedure
opens many possibilities not only from a material hybridization perspective
but also in optimizing charge injection and extraction in semiconductor
quantum-dot-based optoelectronics applications
Quantum Confinement-Tunable Ultrafast Charge Transfer at the PbS Quantum Dot and PhenylāC<sub>61</sub>-butyric Acid Methyl Ester Interface
Quantum
dot (QD) solar cells have emerged as promising low-cost
alternatives to existing photovoltaic technologies. Here, we investigate
charge transfer and separation at PbS QDs and phenyl-C<sub>61</sub>-butyric acid methyl ester (PCBM) interfaces using a combination
of femtosecond broadband transient absorption (TA) spectroscopy and
steady-state photoluminescence quenching measurements. We analyzed
ultrafast electron injection and charge separation at PbS QD/PCBM
interfaces for four different QD sizes and as a function of PCBM concentration.
The results reveal that the energy band alignment, tuned by the quantum
size effect, is the key element for efficient electron injection and
charge separation processes. More specifically, the steady-state and
time-resolved data demonstrate that only small-sized PbS QDs with
a bandgap larger than 1 eV can transfer electrons to PCBM upon light
absorption. We show that these trends result from the formation of
a type-II interface band alignment, as a consequence of the size distribution
of the QDs. Transient absorption data indicate that electron injection
from photoexcited PbS QDs to PCBM occurs within our temporal resolution
of 120 fs for QDs with bandgaps that achieve type-II alignment, while
virtually all signals observed in smaller bandgap QD samples result
from large bandgap outliers in the size distribution. Taken together,
our results clearly demonstrate that charge transfer rates at QD interfaces
can be tuned by several orders of magnitude by engineering the QD
size distribution. The work presented here will advance both the design
and the understanding of QD interfaces for solar energy conversion