39 research outputs found
Unusual Redox Chemistry of Ytterbium Carbazole–Bis(oxazoline) Compounds: Oxidative Coupling of Primary Phosphines by an Ytterbium Carbazole–Bis(oxazoline) Dialkyl
The
1,8-bis(4′,4′-dimethyloxazolin-2′-yl)-3,6-di-<i>tert</i>-butylcarbazole anion (Czx) forms monomeric, six-coordinate
halide complexes of Yb(II), (Czx)Yb(X)(THF)<sub>2</sub> (X = I (<b>2</b>), Cl (<b>3</b>)), by metathesis of YbX<sub>2</sub> with NaCzx (<b>1</b>) or Na/Hg reduction of (Czx)Yb(Cl)<sub>2</sub>(THF). The crystal structure of <b>1</b> reveals a polymeric
chain structure in which the oxazoline ring bridges to the Na<sup>+</sup> of an adjacent unit. The iodo complex <b>2</b> serves
as a precursor to divalent silylamide, alkyl, and phosphide complexes,
(Czx)Yb(X)(THF)<sub><i>n</i></sub> (<b>4</b>, X =
N(SiMe<sub>3</sub>)<sub>2</sub>, <i>n</i> = 1; <b>5</b>, X = CH(SiMe<sub>3</sub>)<sub>2</sub>, <i>n</i> = 1; <b>7a</b>, X = 2,4,6-Me<sub>3</sub>C<sub>6</sub>H<sub>2</sub>PH, <i>n</i> = 2; <b>7b</b>, X = 2,4,6-Pr<sup>i</sup><sub>3</sub>C<sub>6</sub>H<sub>2</sub>PH, <i>n</i> = 2). The X-ray
structure of <b>4</b> reveals a distorted-trigonal-bipyramidal
geometry with the Czx ligand occupying two axial sites and one equatorial
site in a pseudo-<i>mer</i> coordination mode. In contrast
to the typical metathesis chemistry observed with LiCH(SiMe<sub>3</sub>)<sub>2</sub>, an unusual <i>oxidation</i> occurs when <b>2</b> or <b>3</b> is treated with LiCH<sub>2</sub>SiMe<sub>3</sub> to generate the previously isolated trivalent alkyl (Czx)Yb(CH<sub>2</sub>SiMe<sub>3</sub>)<sub>2</sub>. Trivalent Yb complexes with
the Czx ligand also display unusual redox chemistry: rapid <i>reduction</i> to the Yb(II) phosphides <b>7a</b>,<b>b</b> is observed on treatment of <i>mer,cis</i>-(Czx)Yb(Cl)<sub>2</sub>(THF) with ArPH<sup>–</sup> Na<sup>+</sup> (<b>6a</b>,<b>b</b>) or, equivalently, on treatment of (Czx)Yb(CH<sub>2</sub>SiMe<sub>3</sub>)<sub>2</sub> with ArPH<sub>2</sub>. In both
cases, oxidative coupling of the phosphide or phosphine was observed
to form <i>meso</i>- and <i>rac</i>-biphosphines,
ArPH–PHAr (Ar = 2,4,6-Me<sub>3</sub>C<sub>6</sub>H<sub>2</sub> (<b>9a</b>), 2,4,6-Pr<sup>i</sup><sub>3</sub>C<sub>6</sub>H<sub>2</sub> (<b>9b</b>))
Unusual Redox Chemistry of Ytterbium Carbazole–Bis(oxazoline) Compounds: Oxidative Coupling of Primary Phosphines by an Ytterbium Carbazole–Bis(oxazoline) Dialkyl
The
1,8-bis(4′,4′-dimethyloxazolin-2′-yl)-3,6-di-<i>tert</i>-butylcarbazole anion (Czx) forms monomeric, six-coordinate
halide complexes of Yb(II), (Czx)Yb(X)(THF)<sub>2</sub> (X = I (<b>2</b>), Cl (<b>3</b>)), by metathesis of YbX<sub>2</sub> with NaCzx (<b>1</b>) or Na/Hg reduction of (Czx)Yb(Cl)<sub>2</sub>(THF). The crystal structure of <b>1</b> reveals a polymeric
chain structure in which the oxazoline ring bridges to the Na<sup>+</sup> of an adjacent unit. The iodo complex <b>2</b> serves
as a precursor to divalent silylamide, alkyl, and phosphide complexes,
(Czx)Yb(X)(THF)<sub><i>n</i></sub> (<b>4</b>, X =
N(SiMe<sub>3</sub>)<sub>2</sub>, <i>n</i> = 1; <b>5</b>, X = CH(SiMe<sub>3</sub>)<sub>2</sub>, <i>n</i> = 1; <b>7a</b>, X = 2,4,6-Me<sub>3</sub>C<sub>6</sub>H<sub>2</sub>PH, <i>n</i> = 2; <b>7b</b>, X = 2,4,6-Pr<sup>i</sup><sub>3</sub>C<sub>6</sub>H<sub>2</sub>PH, <i>n</i> = 2). The X-ray
structure of <b>4</b> reveals a distorted-trigonal-bipyramidal
geometry with the Czx ligand occupying two axial sites and one equatorial
site in a pseudo-<i>mer</i> coordination mode. In contrast
to the typical metathesis chemistry observed with LiCH(SiMe<sub>3</sub>)<sub>2</sub>, an unusual <i>oxidation</i> occurs when <b>2</b> or <b>3</b> is treated with LiCH<sub>2</sub>SiMe<sub>3</sub> to generate the previously isolated trivalent alkyl (Czx)Yb(CH<sub>2</sub>SiMe<sub>3</sub>)<sub>2</sub>. Trivalent Yb complexes with
the Czx ligand also display unusual redox chemistry: rapid <i>reduction</i> to the Yb(II) phosphides <b>7a</b>,<b>b</b> is observed on treatment of <i>mer,cis</i>-(Czx)Yb(Cl)<sub>2</sub>(THF) with ArPH<sup>–</sup> Na<sup>+</sup> (<b>6a</b>,<b>b</b>) or, equivalently, on treatment of (Czx)Yb(CH<sub>2</sub>SiMe<sub>3</sub>)<sub>2</sub> with ArPH<sub>2</sub>. In both
cases, oxidative coupling of the phosphide or phosphine was observed
to form <i>meso</i>- and <i>rac</i>-biphosphines,
ArPH–PHAr (Ar = 2,4,6-Me<sub>3</sub>C<sub>6</sub>H<sub>2</sub> (<b>9a</b>), 2,4,6-Pr<sup>i</sup><sub>3</sub>C<sub>6</sub>H<sub>2</sub> (<b>9b</b>))
An Integrated Amplification-Free Digital CRISPR/Cas-Assisted Assay for Single Molecule Detection of RNA
Conventional nucleic acid detection technologies usually
rely on
amplification to improve sensitivity, which has drawbacks, such as
amplification bias, complicated operation, high requirements for complex
instruments, and aerosol pollution. To address these concerns, we
developed an integrated assay for the enrichment and single molecule
digital detection of nucleic acid based on a CRISPR/Cas13a and microwell
array. In our design, magnetic beads capture and concentrate the target
from a large volume of sample, which is 100 times larger than reported
earlier. The target-induced CRISPR/Cas13a cutting reaction was then
dispersed and limited to a million individual femtoliter-sized microwells,
thereby enhancing the local signal intensity to achieve single-molecule
detection. The limit of this assay for amplification-free detection
of SARS-CoV-2 is 2 aM. The implementation of this study will establish
a “sample-in-answer-out” single-RNA detection technology
without amplification and improve the sensitivity and specificity
while shortening the detection time. This research has broad prospects
in clinical application
Anisotropic Electrical Properties from Vapor–Solid–Solid Grown Bi<sub>2</sub>Se<sub>3</sub> Nanoribbons and Nanowires
High-quality Bi<sub>2</sub>Se<sub>3</sub> nanoribbons and nanowires were synthesized by a Au-catalyzed
chemical vapor deposition method. Detailed structural and chemical
characterizations using scanning and transmission electron microscopy
show that the growth of both Bi<sub>2</sub>Se<sub>3</sub> nanoribbons
and nanowires is governed by the vapor–solid–solid growth
mechanism, and the nanoribbons grow along ⟨112̅0⟩
and nanowires grow along ⟨0001⟩ directions. Detailed <i>in situ</i> scanning tunneling microscope–transmission
electron microscopy electrical measurements show that the nanoribbons
are much more conductive than the nanowires with a conductivity anisotropy
ratio of ∼2.5 × 10<sup>2</sup> at room temperature
Highly Ordered Cubic Mesoporous Materials with the Same Symmetry but Tunable Pore Structures
In this article, two highly ordered mesoporous silica
materials
with the same face-centered cubic (<i>fcc</i>) symmetry
but distinctly different pore structures have been synthesized by
simply changing the amount of silica source. Their structures have
been extensively studied by Synchrotron small-angle X-ray scattering,
N<sub>2</sub> sorption analysis, scanning and transmission electron
microscopy observations, and electron tomography. One mesoporous material
formed by a hard sphere packing (HSP) pathway exhibits a bimodal pore
distribution, while the other has a conventional FDU-12-type mesostructure
with a single-sized pore. By increasing the amount of the silica source,
the cavities formed by the packing of composite spherical micelles
in the HSP mesostructure are gradually filled by the excess of siliceous
species, leading to the conventional FDU-12-type mesostructure with
the disappearance of bimodal pores. The pore connectivity of the HSP
mesoporous material hydrothermally treated at 150 °C has been
further investigated. Taking advantage of the ultrathin tomographic
slices, the sizes of cage, cavity, and connectivity are measured to
be 14.5, 10.5, and 6.4 nm, respectively. More importantly, the pore
connection between the cage and cavity is directly observed to occur
along the ⟨100⟩ direction, different from the FDU-12-type
mesostructure in which the connection appears between two adjacent
cages along the ⟨110⟩ direction. This work represents
an unusual example where two ordered cage-type mesoporous materials
with the same symmetry can be synthesized by slightly changing the
synthesis condition, but their pore structures and pore connections
are significantly different. Our finding is important for understanding
the formation mechanism and for the rational design and controllable
synthesis of novel mesoporous materials
Highly Ordered Cubic Mesoporous Materials with the Same Symmetry but Tunable Pore Structures
In this article, two highly ordered mesoporous silica
materials
with the same face-centered cubic (<i>fcc</i>) symmetry
but distinctly different pore structures have been synthesized by
simply changing the amount of silica source. Their structures have
been extensively studied by Synchrotron small-angle X-ray scattering,
N<sub>2</sub> sorption analysis, scanning and transmission electron
microscopy observations, and electron tomography. One mesoporous material
formed by a hard sphere packing (HSP) pathway exhibits a bimodal pore
distribution, while the other has a conventional FDU-12-type mesostructure
with a single-sized pore. By increasing the amount of the silica source,
the cavities formed by the packing of composite spherical micelles
in the HSP mesostructure are gradually filled by the excess of siliceous
species, leading to the conventional FDU-12-type mesostructure with
the disappearance of bimodal pores. The pore connectivity of the HSP
mesoporous material hydrothermally treated at 150 °C has been
further investigated. Taking advantage of the ultrathin tomographic
slices, the sizes of cage, cavity, and connectivity are measured to
be 14.5, 10.5, and 6.4 nm, respectively. More importantly, the pore
connection between the cage and cavity is directly observed to occur
along the ⟨100⟩ direction, different from the FDU-12-type
mesostructure in which the connection appears between two adjacent
cages along the ⟨110⟩ direction. This work represents
an unusual example where two ordered cage-type mesoporous materials
with the same symmetry can be synthesized by slightly changing the
synthesis condition, but their pore structures and pore connections
are significantly different. Our finding is important for understanding
the formation mechanism and for the rational design and controllable
synthesis of novel mesoporous materials
Immagini d'acqua nelle poesie d'amore del Kokinwakashu
Influenced by the Buddhist view of human life as transient, and by the Buddhist distrust of love, the compilers of the Kokinwakashū in the five books of love poems structured the development of an imaginary romance according to a pattern of blossoming, flourishing and decline. It is interesting to note that the different stages of this romance are described from beginning to end through impressive images of water. A mountain torrent running swiftly suggests the intense agitation of feelings caused by love. Waterfalls and waves are very effective to express people’s rising rumors about a love affair, whereas rivers and sometimes oceans offer an obvious metaphor for lover’s tears of grief and tears of longing. In some cases, an heartless woman who refuses her suitor is described as a desolate bay, while an abandoned lover feels like vanishing bubbles on running water.
According to the first imperial anthology, love is a force of nature whose power is great enough to destroy man but it is also an impermanent and unreliable thing like a mountain torrent which continuously brings wherever it wants its agitated water
Scalable Growth of High Mobility Dirac Semimetal Cd<sub>3</sub>As<sub>2</sub> Microbelts
Three-dimensional
(3D) Dirac semimetals are 3D analogues of graphene, which display
Dirac points with linear dispersion in <i>k</i>-space, stabilized
by crystal symmetry. Cd<sub>3</sub>As<sub>2</sub> has been predicted
to be 3D Dirac semimetals and was subsequently demonstrated by angle-resolved
photoemission spectroscopy. As unveiled by transport measurements,
several exotic phases, such as Weyl semimetals, topological insulators,
and topological superconductors, can be deduced by breaking time reversal
or inversion symmetry. Here, we reported a facile and scalable chemical
vapor deposition method to fabricate high-quality Dirac semimetal
Cd<sub>3</sub>As<sub>2</sub> microbelts; they have shown ultrahigh
mobility up to 1.15 × 10<sup>5</sup> cm<sup>2</sup> V<sup>−1</sup> s<sup>−1</sup> and pronounced Shubnikov–de Haas oscillations.
Such extraordinary features are attributed to the suppression of electron
backscattering. This research opens a new avenue for the scalable
fabrication of Cd<sub>3</sub>As<sub>2</sub> materials toward exciting
electronic applications of 3D Dirac semimetals
Rational Design of Bi<sub>2</sub>Te<sub>3</sub> Polycrystalline Whiskers for Thermoelectric Applications
Bi<sub>2</sub>Te<sub>3</sub> polycrystalline
whiskers consisting of interconnected nanoplates have been synthesized
through chemical transformation from In<sub>2</sub>Te<sub>3</sub> polycrystalline
whisker templates assembled by nanoparticles. The synthesized Bi<sub>2</sub>Te<sub>3</sub> whiskers preserve the original one-dimensional
morphology of the In<sub>2</sub>Te<sub>3</sub>, while the In<sub>2</sub>Te<sub>3</sub> nanoparticles can be transformed into the Bi<sub>2</sub>Te<sub>3</sub> thin nanoplates, accompanied by the formation of high-density
interfaces between nanoplates. The hot-pressed nanostructures consolidated
from Bi<sub>2</sub>Te<sub>3</sub> polycrystalline whiskers at 400
°C demonstrate a promising figure of merit (<i>ZT</i>) of 0.71 at 400 K, which can be attributed to their low thermal
conductivity and relatively high electrical conductivity. The small
nanoparticles inherited from the polycrystalline whiskers and high-density
nanoparticle interfaces in the hot-pressed nanostructures contribute
to the significant reduction of thermal conductivity. This study provides
a rational chemical transformation approach to design and synthesize
polycrystalline microstructures for enhanced thermoelectric performances
Planar Vacancies in Sn<sub>1–<i>x</i></sub>Bi<sub><i>x</i></sub>Te Nanoribbons
Vacancy
engineering is a crucial approach to manipulate physical
properties of semiconductors. Here, we demonstrate that planar vacancies
are formed in Sn<sub>1–<i>x</i></sub>Bi<sub><i>x</i></sub>Te nanoribbons by using Bi dopants <i>via</i> a facile chemical vapor deposition. Through combination of sub-angstrom-resolution
imaging and density functional theory calculations, these planar vacancies
are found to be associated with Bi segregations, which significantly
lower their formation energies. The planar vacancies exhibit polymorphic
structures with local variations in the lattice relaxation level,
determined by their proximity to the nanoribbon surface. Such polymorphic
planar vacancies, in conjunction with Bi dopants, trigger distinct
localized electronic states, offering platforms for device applications
of ternary chalcogenide materials