8 research outputs found
Catalyst-Free C(sp<sup>2</sup>)‑H Borylation through Aryl Radical Generation from Thiophenium Salts via Electron Donor–Acceptor Complex Formation
Aryl borates lie at the heart of carbon–carbon
bond couplings,
and they are widely applied to the synthesis of functional materials,
pharmaceutical compounds, and natural products. Currently, synthetic
methods for aryl borates are mostly limited to metal-catalyzed routes,
and nonmetallic strategies remain comparatively underdeveloped. Herein,
we report a mild, scalable, visible-light-induced cross-coupling between
aryl dibenzothiophenium triflate salts and bis(catecholato)-diboron
for the construction of C–B bonds in the absence of base, transition
metal–ligand complex, or photoredox catalyst. Mechanistic studies
reveal that this transformation is achieved through an electron donor–acceptor
(EDA) complex activation in the absence of a catalyst. The mild reaction
conditions allow the preparation of aromatic borates in good yields
with excellent functional group tolerance. This photochemical protocol
was also successfully applied to the late-stage modification of natural
products and the synthesis of a drug intermediate, greatly demonstrating
broadened utility
Co Nanoparticles Encapsulated in N‑Doped Carbon Nanosheets: Enhancing Oxygen Reduction Catalysis without Metal–Nitrogen Bonding
It is known that
introducing metal nanoparticles (e.g., Fe and
Co) into N-doped carbons can enhance the activity of N-doped carbons
toward the oxygen reduction reaction (ORR). However, introducing metals
into N-doped carbons inevitably causes the formation of multiple active
sites. Thus, it is challenging to identify the active sites and unravel
mechanisms responsible for enhanced ORR activity. Herein, by developing
a new N-heterocyclic carbene (NHC)–Co complex as the nitrogen-
and metal-containing precursor, we report the synthesis of N-doped
carbon nanosheets embedded with Co nanoparticles as highly active
ORR catalysts without direct metal–nitrogen bonding. Electrochemical
measurements and X-ray absorption spectroscopy indicate that the carbon–nitrogen
sites surrounding Co nanoparticles are responsible for the observed
ORR activity and stability. Density functional theory calculations
further reveal that Co nanoparticles could facilitate the protonation
of O<sub>2</sub> and thus promote the ORR activity. These results
provide new prospects in the rational design and synthesis of heteroatom-doped
carbon materials as non-precious-metal catalysts for various electrochemical
reactions
Supplementary document for Broadband ASE source-enabled self-homodyne DA-RoF fronthaul using cascaded SOAs and multicore fiber - 6853676.pdf
Supplemental Documen
Sr<sub>2</sub>Mn<sub>3</sub>Sb<sub>2</sub>O<sub>2</sub> Type Oxyselenides: Structures, Magnetism, and Electronic Properties of Sr<sub>2</sub><i>A</i>O<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>A</i>=Co, Mn; <i>M</i>=Cu, Ag)
Four new oxyselenides with nominal formula Sr<sub>2</sub><i>A</i>O<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>A</i>=Co, Mn; <i>M</i>=Cu, Ag) have
been
synthesized. They all crystallize in an <i>I</i>4/<i>mmm</i> space group and consist of alternating perovskite-like
(Sr<sub>2</sub><i>A</i>O<sub>2</sub>)<sup>2+</sup> blocks
and antiflourie (<i>M</i><sub>2</sub>Se<sub>2</sub>)<sup>2‑</sup> layers, which are relatively rare layered oxyselenides
reported so far that are isostructural to Sr<sub>2</sub>Mn<sub>3</sub>Sb<sub>2</sub>O<sub>2</sub>. From powder X-ray diffraction data,
compounds Sr<sub>2</sub>CoO<sub>2</sub>Cu<sub>2</sub>Se<sub>2</sub> and Sr<sub>2</sub>CoO<sub>2</sub>Ag<sub>2</sub>Se<sub>2</sub> are
found near stoichiometric, whereas Sr<sub>2</sub>MnO<sub>2</sub>Cu<sub>2‑δ</sub>Se<sub>2</sub> and Sr<sub>2</sub>MnO<sub>2</sub>Ag<sub>2‑δ</sub>Se<sub>2</sub> possess substantial copper
or silver vacancies (δ≈0.5), consistent with their oxysulfide
analogues. X-ray photoelectron spectroscopy measurements indicate
the readily oxidization of Mn<sup>2+</sup> ions should be responsible
for the occurrence of Cu/Ag vacancies. The rigid (Sr<sub>2</sub><i>A</i>O<sub>2</sub>)<sup>2+</sup> blocks within these compounds
constrain the basal lattice parameters in the <i>ab</i> plane
and result in largely deformed tetrahedral sites for the large silver
ions. Magnetic susceptibility measurements of Sr<sub>2</sub>CoO<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>M</i>=Cu, Ag) show complex antiferromagnetic transitions, while Sr<sub>2</sub>MnO<sub>2</sub><i>M</i><sub>2‑δ</sub>Se<sub>2</sub> (<i>M</i>=Cu, Ag) show high-temperature
Curie–Weiss behavior, followed by low-temperature antiferromagnetic
transitions at 54 K and 67 K, respectively. Except for Sr<sub>2</sub>MnO<sub>2</sub>Ag<sub>2‑δ</sub>Se<sub>2</sub>, the other
three compounds exhibit p-type semiconducting transport properties,
with the measured resistivities several orders lower than their oxysulfide
analogues. Hall measurement reveals high mobilities of Sr<sub>2</sub>CoO<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>M</i>=Cu, Ag) compounds at room temperature. The unusually small
optical band gaps (∼0.07 eV) of Sr<sub>2</sub>CoO<sub>2</sub>Cu<sub>2</sub>Se<sub>2</sub>, Sr<sub>2</sub>CoO<sub>2</sub>Ag<sub>2</sub>Se<sub>2</sub>, and Sr<sub>2</sub>MnO<sub>2</sub>Cu<sub>2‑δ</sub>Se<sub>2</sub> are also reported
Sr<sub>2</sub>Mn<sub>3</sub>Sb<sub>2</sub>O<sub>2</sub> Type Oxyselenides: Structures, Magnetism, and Electronic Properties of Sr<sub>2</sub><i>A</i>O<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>A</i>=Co, Mn; <i>M</i>=Cu, Ag)
Four new oxyselenides with nominal formula Sr<sub>2</sub><i>A</i>O<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>A</i>=Co, Mn; <i>M</i>=Cu, Ag) have
been
synthesized. They all crystallize in an <i>I</i>4/<i>mmm</i> space group and consist of alternating perovskite-like
(Sr<sub>2</sub><i>A</i>O<sub>2</sub>)<sup>2+</sup> blocks
and antiflourie (<i>M</i><sub>2</sub>Se<sub>2</sub>)<sup>2‑</sup> layers, which are relatively rare layered oxyselenides
reported so far that are isostructural to Sr<sub>2</sub>Mn<sub>3</sub>Sb<sub>2</sub>O<sub>2</sub>. From powder X-ray diffraction data,
compounds Sr<sub>2</sub>CoO<sub>2</sub>Cu<sub>2</sub>Se<sub>2</sub> and Sr<sub>2</sub>CoO<sub>2</sub>Ag<sub>2</sub>Se<sub>2</sub> are
found near stoichiometric, whereas Sr<sub>2</sub>MnO<sub>2</sub>Cu<sub>2‑δ</sub>Se<sub>2</sub> and Sr<sub>2</sub>MnO<sub>2</sub>Ag<sub>2‑δ</sub>Se<sub>2</sub> possess substantial copper
or silver vacancies (δ≈0.5), consistent with their oxysulfide
analogues. X-ray photoelectron spectroscopy measurements indicate
the readily oxidization of Mn<sup>2+</sup> ions should be responsible
for the occurrence of Cu/Ag vacancies. The rigid (Sr<sub>2</sub><i>A</i>O<sub>2</sub>)<sup>2+</sup> blocks within these compounds
constrain the basal lattice parameters in the <i>ab</i> plane
and result in largely deformed tetrahedral sites for the large silver
ions. Magnetic susceptibility measurements of Sr<sub>2</sub>CoO<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>M</i>=Cu, Ag) show complex antiferromagnetic transitions, while Sr<sub>2</sub>MnO<sub>2</sub><i>M</i><sub>2‑δ</sub>Se<sub>2</sub> (<i>M</i>=Cu, Ag) show high-temperature
Curie–Weiss behavior, followed by low-temperature antiferromagnetic
transitions at 54 K and 67 K, respectively. Except for Sr<sub>2</sub>MnO<sub>2</sub>Ag<sub>2‑δ</sub>Se<sub>2</sub>, the other
three compounds exhibit p-type semiconducting transport properties,
with the measured resistivities several orders lower than their oxysulfide
analogues. Hall measurement reveals high mobilities of Sr<sub>2</sub>CoO<sub>2</sub><i>M</i><sub>2</sub>Se<sub>2</sub> (<i>M</i>=Cu, Ag) compounds at room temperature. The unusually small
optical band gaps (∼0.07 eV) of Sr<sub>2</sub>CoO<sub>2</sub>Cu<sub>2</sub>Se<sub>2</sub>, Sr<sub>2</sub>CoO<sub>2</sub>Ag<sub>2</sub>Se<sub>2</sub>, and Sr<sub>2</sub>MnO<sub>2</sub>Cu<sub>2‑δ</sub>Se<sub>2</sub> are also reported
Potential of fluorescent nanoprobe in diagnosis and treatment of Alzheimer’s disease Supplementary figures nnm-2022-0022
Alzheimer’s disease (AD) is well known for its insidious nature, slow progression and high incidence as
a neurodegenerative disease. In the past, diagnosis of AD mainly depended on analysis of a patient’s
cognitive ability and behavior. Without a unified standard for analysis methods, this is prone to produce
incorrect diagnoses. Currently, definitive diagnosis mainly relies on histopathological examination.
Because of the advantages of precision, noninvasiveness, low toxicity and high spatiotemporal resolution,
fluorescent nanoprobes are suitable for the early diagnosis of AD. This review summarizes the research
progress of different kinds of fluorescent nanoprobes for AD diagnosis and therapy in recent years and
provides an outlook on the development prospects of fluorescent nanoprobes.</p
Enhanced Raman Scattering on In-Plane Anisotropic Layered Materials
Surface-enhanced Raman scattering
(SERS) on two-dimensional (2D)
layered materials has provided a unique platform to study the chemical
mechanism (CM) of the enhancement due to its natural separation from
electromagnetic enhancement. The CM stems from the charge interactions
between the substrate and molecules. Despite the extensive studies
of the energy alignment between 2D materials and molecules, an understanding
of how the electronic properties of the substrate are explicitly involved
in the charge interaction is still unclear. Lately, a new group of
2D layered materials with anisotropic structures, including orthorhombic
black phosphorus (BP) and triclinic rhenium disulfide (ReS<sub>2</sub>), has attracted great interest due to their unique anisotropic electrical
and optical properties. Herein, we report a unique anisotropic Raman
enhancement on few-layered BP and ReS<sub>2</sub> using copper phthalocyanine
(CuPc) molecules as a Raman probe, which is absent on isotropic graphene
and h-BN. According to detailed Raman tensor analysis and density
functional theory calculations, anisotropic charge interactions between
the 2D materials and molecules are responsible for the angular dependence
of the Raman enhancement. Our findings not only provide new insights
into the CM process in SERS, but also open up new avenues for the
exploration and application of the electronic properties of anisotropic
2D layered materials
Optical Anisotropy of Black Phosphorus in the Visible Regime
The
striking in-plane anisotropy remains one of the most intriguing
properties for the newly rediscovered black phosphorus (BP) 2D crystals.
However, because of its rather low-energy band gap, the optical anisotropy
of few-layer BP has been primarily investigated in the near-infrared
(NIR) regime. Moreover, the essential physics that determine the intrinsic
anisotropic optical property of few-layer BP, which is of great importance
for practical applications in optical and optoelectronic devices,
are still in the fancy of theory. Herein, we report the direct observation
of the optical anisotropy of few-layer BP in the visible regime simply
by using polarized optical microscopy. On the basis of the Fresnel
equation, the intrinsic anisotropic complex refractive indices (<i>n</i>–<i>i</i>κ) in the visible regime
(480–650 nm) were experimentally obtained for the first time
using the anisotropic optical contrast spectra. Our findings not only
provide a convenient approach to measure the optical constants of
2D layered materials but also suggest a possibility to design novel
BP-based photonic devices such as atom-thick light modulators, including
linear polarizer, phase plate, and optical compensator in a broad
spectral range extending to the visible window