66 research outputs found
In Situ Observation of the Growth of ZnO Nanostructures Using Liquid Cell Electron Microscopy
Understanding
the growth mechanisms and associated kinetics is a fundamental issue
toward the specific function-oriented controlled synthesis of nanostructures.
In this work, the growth of zinc oxide nanostructures with different
sizes and morphologies are directly observed by in situ liquid-cell
transmission electron microscopy (TEM). Real-time observation and
quantitative analysis reveal that the concentration ratios of the
precursors are responsible for the different growth kinetics, resulting
in different morphology and size of the synthesized ZnO nanostructures
Facile Method toward Hierarchical Fullerene Architectures with Enhanced Hydrophobicity and Photoluminescence
A two-step self-assembly strategy
has been developed for the preparation of fullerene hierarchical architectures.
Typically, the precipitation method is utilized to synthesize the
initial fullerene microstructures, and subsequently a drop-drying
process is employed to facilitate the fullerene microstructures to
self-assemble into the final hierarchical structures. Overall, this
methodology is quite simple and feasible, which can be applied to
prepare fullerene hierarchical structures with different morphological
features, simply by choosing proper solvent. Moreover, the as-obtained
C<sub>70</sub> hierarchical structures have many superior properties
over the original C<sub>70</sub> microrods such as superhydrophobicity
and unique photoluminescence behaviors, promising their applications
as waterproof optoelectronics
Anion Templated Synthesis of Silver(I)-Ethynide Dithiophosphate Clusters
Reaction
of AgCC<sup><i>t</i></sup>Bu with (EtO)<sub>2</sub>PS<sub>2</sub>Na at room temperature leads to the isolation
of two new silver(I)-ethynide compounds incorporating the dithiophosphate
ligand, namely, {CO<sub>3</sub>@(Ag<sub>3</sub>)<sub>4</sub>(CC<sup><i>t</i></sup>Bu)<sub>4</sub>(EtO)<sub>2</sub>PS<sub>2</sub>]<sub>6</sub>}·0.5H<sub>2</sub>O (<b>1</b>) and {(CO<sub>3</sub>)<sub>2</sub>@Ag<sub>26</sub>(CC<sup><i>t</i></sup>Bu)<sub>16</sub>[(EtO)<sub>2</sub>PS<sub>2</sub>]<sub>4</sub>}·2(OH)·4MeOH·6H<sub>2</sub>O (<b>2</b>). Besides,
we obtain another three silver(I)-ethynide clusters S@Ag<sub>11</sub>(CC<sup><i>t</i></sup>Bu)<sub>2</sub>[(EtO)<sub>2</sub>PS<sub>2</sub>]<sub>7</sub> (<b>3</b>), {S@Ag<sub>14</sub>(CCPh)<sub>8</sub>[(EtO)<sub>2</sub>PS<sub>2</sub>]<sub>4</sub>(TMEDA)<sub>2</sub>}·5MeOH (<b>4</b>), and {S@Ag<sub>14</sub>(CCPh)<sub>8</sub>[(<sup><i>i</i></sup>PrO)<sub>2</sub>PS<sub>2</sub>]<sub>4</sub>(TMEDA)<sub>2</sub>}·7CH<sub>3</sub>OH (<b>5</b>), with AgCCR (R= <sup><i>t</i></sup>Bu, Ph) and (RO)<sub>2</sub>PS<sub>2</sub>Na (R= Et, <sup><i>i</i></sup>Pr) as the starting materials. Complexes <b>1</b>–<b>2</b> are templated by a carbonate anion in situ
generated from the fixation of atmospheric CO<sub>2</sub> in a basic
TMEDA-containing solution, and TMEDA can also lead to the disassembly
of dithiophosphate to give a sulfide ion as the template for the generation
of <b>3</b>–<b>5</b>
Lu<sub>2</sub>@C<sub>82</sub> Nanorods with Enhanced Photoluminescence and Photoelectrochemical Properties
One-dimensional
(1D) single-crystalline hexagonal nanorods of Lu<sub>2</sub>@<i>C</i><sub>3<i>v</i></sub>(8)–C<sub>82</sub> were prepared for the first time using the liquid–liquid
interface precipitation (LLIP) method from the interfaces between
carbon disulfide (CS<sub>2</sub>) and isopropyl alcohol (IPA). The
length of the nanorods can be readily controlled by varying the concentration
of the Lu<sub>2</sub>@C<sub>82</sub> solution in addition to the volume
ratio of CS<sub>2</sub> to IPA. The latter factor also exhibits a
significant influence on the morphology of the crystals. The crystalline
structure of the nanorods has been investigated by XRD and selected
area electron diffraction (SAED), suggesting a face-centered cubic
structure. Photoluminescence of the Lu<sub>2</sub>@C<sub>82</sub> nanorods
shows a remarkable enhancement as compared to that of pristine Lu<sub>2</sub>@C<sub>82</sub> powder because of the high crystallinity.
Furthermore, we have investigated the photoelectrochemical properties
of Lu<sub>2</sub>@C<sub>82</sub> nanorods, proving their potential
applications as photodetectors
Isolation and Crystallographic Characterization of La<sub>2</sub>C<sub>2</sub>@C<sub>s</sub>(574)‑C<sub>102</sub> and La<sub>2</sub>C<sub>2</sub>@C<sub>2</sub>(816)‑C<sub>104</sub>: Evidence for the Top-Down Formation Mechanism of Fullerenes
Tubular
higher fullerenes are prototypes of finite-length end-capped
carbon nanotubes (CNTs) whose structures can be accurately characterized
by single-crystal X-ray diffraction crystallography. We present here
the isolation and crystallographic characterization of two unprecedented
higher fullerenes stabilized by the encapsulation of a La<sub>2</sub>C<sub>2</sub> cluster, namely, La<sub>2</sub>C<sub>2</sub>@C<sub>s</sub>(574)-C<sub>102</sub>, which has a perfect tubular cage corresponding
to a short (10, 0) zigzag carbon nanotube, and La<sub>2</sub>C<sub>2</sub>@C<sub>2</sub>(816)-C<sub>104</sub> which has a defective
cage with a pyracylene motif inserting into the cage waist. Both cages
provide sufficient spaces for the large La<sub>2</sub>C<sub>2</sub> cluster to adopt a stretched and nearly planar configuration, departing
from the common butterfly-like configuration which has been frequently
observed in midsized carbide metallofullerenes (e.g., Sc<sub>2</sub>C<sub>2</sub>@C<sub>80–84</sub>), to achieve strong metal–cage
interactions. More meaningfully, our crystallographic results demonstrate
that the defective cage of C<sub>2</sub>(816)-C<sub>104</sub> is a
starting point to form the other three tubular cages known so far,
i.e., D<sub>5</sub>(450)-C<sub>100</sub>, C<sub>s</sub>(574)-C<sub>102</sub>, and D<sub>3d</sub>(822)-C<sub>104</sub>, presenting evidence
for the top-down formation mechanism of fullerenes. The fact that
only the large La<sub>2</sub>C<sub>2</sub> cluster has been found
in giant fullerene cages (C<sub>>100</sub>) and the small clusters
M<sub>2</sub>C<sub>2</sub> (M = Sc, Y, Er, etc.) are present in midsized
fullerenes (C<sub>80</sub>–C<sub>86</sub>) indicates that geometrical
matching between the cluster and the cage, which ensures strong metal–cage
interactions, is an important factor controlling the stability of
the resultant metallofullerenes, in addition to charge transfer
Exceptional Chemical Properties of Sc@<i>C</i><sub>2<i>v</i></sub>(9)–C<sub>82</sub> Probed with Adamantylidene Carbene
It has been an interesting finding that reactions of
M@<i>C</i><sub>2<i>v</i></sub>(9)–C<sub>82</sub> (M = Y, La, Ce, Gd) with diazirine adamantylidene (AdN<sub>2</sub>, <b>1</b>) gave rise to only two monoadduct isomers,
indicating
that the cage reactivity of monometallofullerenes is not dependent
on the type of the internal metal. However, we found here that Sc@<i>C</i><sub>2<i>v</i></sub>(9)–C<sub>82</sub> shows an exceptional chemical reactivity toward the electrophile <b>1</b>, affording four monoadduct isomers (<b>2a</b>–<b>d</b>). Single-crystal X-ray diffraction crystallographic results
of the most abundant isomer (<b>2a</b>) confirm that the addition
takes place at a [6,6]-bond junction which is very close to the internal
metal ion. Theoretical calculations reveal that 2 out of the 24 nonequivalent
cage carbons of Sc@<i>C</i><sub>2<i>v</i></sub>(9)–C<sub>82</sub> are highly reactive toward <b>1</b>, but only one cage carbon of the other M@<i>C</i><sub>2<i>v</i></sub>–C<sub>82</sub> (M = Y, La, Ce, Gd)
is sufficiently reactive. The exceptional chemical property of Sc@<i>C</i><sub>2<i>v</i></sub>(9)–C<sub>82</sub> is associated with the small ionic radius of Sc<sup>3+</sup>, which
allows stronger metal–cage interactions and makes back-donation
of charge from the cage to the metal more pronounced. Our results
have provided new insights into the art of altering the chemical properties
of fullerene molecules at the atomic level, which would be useful
in the future in utilizing EMFs in quantum computing systems
Characterization of Zebrafish Abcc4 as an Efflux Transporter of Organochlorine Pesticides
<div><p>DDT and lindane are highly toxic organochlorine pesticides and posing adverse effects on the environment and public health due to their frequent usage in developing countries. ABCC4/MRP4 is an organic anion transporter that mediates cellular efflux of a wide range of exogenous and endogenous compounds such as cyclic nucleotides and anti-cancer drugs; however, it remains unclear whether ABCC4 and its orthologs function in the detoxification of organochlorine pesticides. Here, we demonstrated the roles of zebrafish Abcc4 in cellular efflux of DDT and lindane. Zebrafish <i>abcc4</i> was maternally expressed in the oocytes and its transcripts were detected in the lens, pancreas, gills, liver, intestine and bladder of developing embryos and in adult tissues examined. DDT and lindane were able to induce the expression of <i>abcc4</i> gene and overexpression of Abcc4 significantly decreased the cytotoxicity and accumulation of DDT and lindane in LLC-PK1 cells and developing embryos. In contrast, overexpression of an Abcc4-G1188D mutant abolished its transporter function without effects on its substrate binding activity, and sensitized LLC-PK1 cells and developing embryos to toxic pesticides. Moreover, glutathione (GSH) was involved in the efflux of cellular pesticides and ATPase activity in developing embryos can be induced by DDT or lindane. Thus, zebrafish Abcc4 plays crucial roles in cellular efflux of organochlorine pesticides and can be used a potential molecular marker for the monitor of DDT and lindane contamination in the aquatic environment.</p></div
Zebrafish Abcc4 is involved in the excretion of DDT and lindane in developing embryos.
<p>(<b>A and B</b>) Contents of DTT or lindane in embryos expressing GFP, Abcc4 and Abcc4-G1188D at the indicated exposure time points. (<b>C and D</b>) Contents of MCB in embryos expressing GFP, Abcc4 and Abcc4-G1188D after exposed to DTT or lindane at indicated concentrations. Values are expressed as means ± standard deviations (n = 3). Significant differences are indicated by <sup>*</sup><i>p</i><0.05 and <sup>**</sup><i>p</i><0.01.</p
DDT and lindane are potential efflux substrates of zebrafish Abcc4 in LLC-PK1 cells.
<p>(<b>A and B</b>) Effect of Abcc4 on the accumulation of MCB. Stable cell lines were exposed to 25 µM MCB and 0.1–5 µg/mL of DDT or 1–100 µg/mL of lindane for 24 hours. (<b>C and D</b>) Effect of Abcc4 on the excretion of DDT or lindane. Stable cell lines were exposed to 2.5 µg/mL of DDT or 10 µg/mL of lindane for 5 to 180 minutes. Values are expressed as means ± standard deviations (n = 3). Significant differences are indicated by <sup>*</sup><i>p</i><0.05 and <sup>**</sup><i>p</i><0.01.</p
Th-Based Endohedral Metallofullerenes: Anomalous Metal Position and Significant Metal-Cage Covalent Interactions with the Involvement of Th 5f Orbitals
Endohedral metallofullerenes (EMFs)
containing actinides are rather intriguing due to potential 5f-orbital
participation in the metal–metal or metal–cage bonding.
In this work, density functional theory calculations first characterized
the structure of recently synthesized ThC<sub>74</sub> as Th@<i>D</i><sub>3<i>h</i></sub>(14246)-C<sub>74</sub>. We
found that the thorium atom adopts an unusual off-axis position inside
cage due to small metal ion size and the requirement of large coordination
number, which phenomenon was further extended to other Th-based EMFs.
Significantly, besides the strong metal–cage electrostatic
attractions, topological and orbital analysis revealed that all the
investigated Th-based EMFs exhibit obvious covalent interactions between
metal and cage with substantial contribution from the Th 5f orbitals.
The encapsulation by fullerenes is thus proposed as a practical pathway
toward the f-orbital covalency for thorium. Interestingly, the anomalous
internal position of Th led to a novel three-dimensional metal trajectory
at elevated temperatures in the <i>D</i><sub>3<i>h</i></sub>-C<sub>74</sub> cavity, as elucidated by the static computations
and molecular dynamic simulations
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