6 research outputs found
<sup>125</sup>Te NMR Probes of Tellurium Oxide Crystals: Shielding-Structure Correlations
The
local environments around tellurium atoms in a series of tellurium
oxide crystals were probed by <sup>125</sup>Te solid-state NMR spectroscopy.
Crystals with distinct TeO<sub><i>n</i></sub> units (<i>n</i> from 3 to 6), including Na<sub>2</sub>TeO<sub>3</sub>,
α-TeO<sub>2</sub> and γ-TeO<sub>2</sub>, Te<sub>2</sub>O(PO<sub>4</sub>)<sub>2</sub>, K<sub>3</sub>LaTe<sub>2</sub>O<sub>9</sub>, BaZnTe<sub>2</sub>O<sub>7</sub>, and CsYTe<sub>3</sub>O<sub>8</sub> were studied. The latter four were synthesized through a
solid-state process. X-ray diffraction was used to confirm the successful
syntheses. The <sup>125</sup>Te chemical shift was found to exhibit
a strong linear correlation with the Te coordination number. The <sup>125</sup>Te chemical-shift components (δ<sub>11</sub>, δ<sub>22</sub>, and δ<sub>33</sub>) of the TeO<sub>4</sub> units
were further correlated to the O–Te–O-bond angles. With
the aid of <sup>125</sup>Te NMR, it is likely that these relations
can be used to estimate the coordination states of Te atoms in unknown
Te crystals and glasses
Relating <sup>139</sup>La Quadrupolar Coupling Constants to Polyhedral Distortion in Crystalline Structures
A broad
series of crystalline lanthanum oxide-based materials has been investigated
through high-field <sup>139</sup>La solid state nuclear magnetic resonance
(ssNMR) spectroscopy and ab initio density functional theory (DFT)
calculations. The <sup>139</sup>La NMR spectra of LaBGeO<sub>5</sub>, LaBSiO<sub>5</sub>, LaBO<sub>3</sub>, LaPO<sub>4</sub>·1.8H<sub>2</sub>O, La<sub>2</sub>(SO<sub>4</sub>)<sub>3</sub>·9H<sub>2</sub>O, and La<sub>2</sub>(CO<sub>3</sub>)<sub>3</sub>·8H<sub>2</sub>O are reported for the first time. Both newly reported and
literature values of <sup>139</sup>La quadrupolar coupling constants
(<i>C</i><sub>Q</sub>) are related to various quantitative
expressions of polyhedral distortion, including sphericity (Σ)
and ellipsoid span (ϵ). The compounds were separated into two
groups based upon their polyhedral distortion behavior: compounds
with the general formula LaMO<sub>3</sub>, where M is a trivalent
cation; compounds with different general formulas. The <sup>139</sup>La <i>C</i><sub>Q</sub> of the LaMO<sub>3</sub> family
was found to correlate best with ϵ. The <sup>139</sup>La <i>C</i><sub>Q</sub> of non-LaMO<sub>3</sub> compounds correlates
adequately to ϵ but is better described by Σ. The <sup>139</sup>La isotropic chemical shift (δ<sub>iso</sub><sup>CS</sup>) of the non-LaMO<sub>3</sub> compounds is negatively correlated with the lanthanum coordination
number; there is insufficient data from the LaMO<sub>3</sub> compounds
to draw conclusions relating to chemical shift. DFT calculations of
NMR parameters prove to be a sensitive probe of the quality of input
geometry, with predicted parameters agreeing with experiment except
in cases where the crystal structure is suspect
Control of Ultrasmall Sub-10 nm Ligand-Functionalized Fluorescent Core–Shell Silica Nanoparticle Growth in Water
Ultrasmall
fluorescent silica nanoparticles (SNPs) and core–shell
SNPs surface functionalized with polyethylene glycol (PEG), specific
surface ligands, and overall SNP size in the regime below 10 nm are
of rapidly increasing interest for clinical applications, because
of their favorable biodistribution and safety profiles. Here, we present
an aqueous synthesis methodology for the preparation of narrowly size-dispersed
SNPs and core–shell SNPs with size control below 1 nm, i.e.,
at the level of a single atomic layer. Different types of fluorophores,
including near-infrared (NIR) emitters, can be covalently encapsulated.
Brightness can be enhanced via addition of extra silica shells. This
methodology further enables synthesis of <10 nm sized fluorescent
core and core–shell SNPs with previously unknown compositions.
In particular, the addition of an aluminum sol gel precursor leads
to fluorescent aluminosilicate nanoparticles (ASNPs) and core–shell
ASNPs. Encapsulation efficiency and brightness of highly negatively
charged NIR fluorophores is enhanced, relative to the corresponding
SNPs without aluminum. Resulting particles show quantum yields of
∼0.8, i.e., starting to approach the theoretical brightness
limit. All particles can be PEGylated providing steric stability.
Finally, heterobifunctional PEGs can be employed to introduce ligands
onto the PEGylated particle surface of fluorescent SNPs, core–shell
SNPS, and their aluminum-containing analogues, producing ligand-functionalized
<10 nm NIR fluorescent nanoprobes. In order to distinguish these
water-based-synthesis-derived materials from the earlier alcohol-based
modified Stöber process derived fluorescent core–shell
SNPs referred to as Cornell dots or C dots, the SNPs and ASNPs described
here and synthesized in water will be referred to as Cornell prime
dots or C′ dots and AlC′ dots. These organic–inorganic
hybrid nanomaterials may find applications in nanomedicine, including
cancer diagnostics and therapy (theranostics)
Self-Assembled Gyroidal Mesoporous Polymer-Derived High Temperature Ceramic Monoliths
Polymer-derived
ceramics (PDCs) have enabled the development of
nonoxide ceramic coatings and fibers with exceptional thermo-mechanical
stability. Here, we report the self-assembly based synthesis of gyroidal
(space group Q<sup>230</sup>, <i>Ia</i>3̅<i>d</i>) mesoporous silicon oxynitride ceramic monoliths by pyrolysis of
blends of commercially available preceramic polysilazane with a structure-directing
triblock terpolymer up to temperatures of 1000 °C. Monoliths
had pore diameters of 9.4 ± 1.1 nm and surface area of 160 m<sup>2</sup>/g. The three-dimensionally (3D) ordered periodic pore structure
of the as-made hybrids acts to relieve stresses by allowing the escape
of gases formed during ceramization. This process in turn enables
the retention of smooth monoliths during ceramization under ammonia,
a process that both adds nitrogen to the material and removes carbon
pyrolysis products. The monoliths are appealing for high-temperature
applications such as catalyst supports and microelectromechanical
system (MEMS) devices including gas and pressure sensors, as well
as strong, stiff, and creep-resistant scaffolds for ordered interpenetrating
phase composites
Stimuli-Responsive Shapeshifting Mesoporous Silica Nanoparticles
Stimuli-responsive materials have
attracted great interest
in catalysis, sensing, and drug delivery applications and are typically
constituted by soft components. We present a one-pot synthetic method
for a type of inorganic silica-based shape change material that is
responsive to water vapor exposure. After the wetting treatment, the
cross-sectional shape of aminated mesoporous silica nanoparticles
(MSNs) with hexagonal pore lattice changed from hexagonal to six-angle-star,
accompanied by the loss of periodic mesostructural order. Nitrogen
sorption measurements suggested that the wetting treatment induced
a shrinkage of mesopores resulting in a broad size distribution and
decreased mesopore volume. Solid-state <sup>29</sup>Si nuclear magnetic
resonance (NMR) spectroscopy of samples after wetting treatment displayed
a higher degree of silica condensation, indicating that the shape
change was associated with the formation of more siloxane bonds within
the silica matrix. On the basis of material characterization results,
a mechanism for the observed anisotropic shrinkage is suggested based
on a buckling deformation induced by capillary forces in the presence
of a threshold amount of water vapor available beyond a humidity of
about 50%. The work presented here may open a path toward novel stimuli-responsive
materials based on inorganic components
Zero Thermal Expansion in ZrMgMo<sub>3</sub>O<sub>12</sub>: NMR Crystallography Reveals Origins of Thermoelastic Properties
The
coefficient of thermal expansion of ZrMgMo<sub>3</sub>O<sub>12</sub> has been measured and was found to be extremely close to
zero over a wide temperature range including room temperature (αl = (1.6 ± 0.2) ×
10<sup>–7</sup> K<sup>–1</sup> from 25 to 450 °C
by X-ray diffraction
(XRD)). ZrMgMo<sub>3</sub>O<sub>12</sub> belongs to the family of
AMgM<sub>3</sub>O<sub>12</sub> materials, for which coefficients of
thermal expansion have previously been reported to range from low-positive
to low-negative. However, the low thermal expansion property had not
previously been explained because atomic position information was
not available for any members of this family of materials. We determined
the structure of ZrMgMo<sub>3</sub>O<sub>12</sub> by nuclear magnetic
resonance (NMR) crystallography, using <sup>91</sup>Zr, <sup>25</sup>Mg, <sup>95</sup>Mo, and <sup>17</sup>O magic angle spinning (MAS)
and <sup>17</sup>O multiple quantum MAS (MQMAS) NMR in conjunction
with XRD and density functional theory calculations. The resulting
structure was of sufficient detail that the observed zero thermal
expansion could be explained using quantitative measures of the properties
of the coordination polyhedra. We also found that ZrMgMo<sub>3</sub>O<sub>12</sub> shows significant ionic conductivity, a property that
is also related to its structure