3 research outputs found
Sensitive and Specific Detection of lâLactate Using an AIE-Active Fluorophore
l-Lactate is a vital biomarker for many diseases and physiological
fatigue. An AIE-active fluorophore (TPE-HPro) is combined with l-lactate oxidase (LOx) to determine l-lactate in aqueous
fluid. The assay shows excellent sensitivity and anti-interference
performance with a limit of detection (LOD) of 5.5 ÎŒM. In addition,
sensitive detection of l-lactate is achieved even in a protein-rich
environment. It is proposed that quantification of l-lactate
be performed at 20 or 60 min in the current method. These characteristics
endow the fluorometric assay with great potential for biomedical diagnostics
Thiol-Reactive Molecule with Dual-Emission-Enhancement Property for Specific Prestaining of Cysteine Containing Proteins in SDS-PAGE
1-[4-(Bromomethyl)Âphenyl]-1,2,2-triphenylethene
(<b>2</b>) was synthesized and evaluated for specific fluorescent
prestaining of proteins containing cysteine (Cys) in SDS-PAGE. The
molecule showed classic aggregation-induced emission (AIE) property
in protein labeling and its quantum efficiency was further enhanced
upon reacting with Cys. The parameters of reaction such as labeling
time and concentration of dye and reducing reagent-trisÂ(2-carboxyethyl)Âphosphine
(TCEP) were examined to obtain the optimal labeling condition. In
addition to its specific labeling effect, molecule <b>2</b> also
showed its advantage over traditional self-quenching dyes through
labeling Cys containing BSA with different dye/Cys ratios
High Thermoelectric Performance in Crystallographically Textured nâType Bi<sub>2</sub>Te<sub>3â<i>x</i></sub>Se<sub><i>x</i></sub> Produced from Asymmetric Colloidal Nanocrystals
In the present work, we demonstrate
crystallographically textured
n-type Bi<sub>2</sub>Te<sub>3â<i>x</i></sub>Se<sub><i>x</i></sub> nanomaterials with exceptional thermoelectric
figures of merit produced by consolidating disk-shaped Bi<sub>2</sub>Te<sub>3â<i>x</i></sub>Se<sub><i>x</i></sub> colloidal nanocrystals (NCs). Crystallographic texture was
achieved by hot pressing the asymmetric NCs in the presence of an
excess of tellurium. During the hot press, tellurium acted both as
lubricant to facilitate the rotation of NCs lying close to normal
to the pressure axis and as solvent to dissolve the NCs approximately
aligned with the pressing direction, which afterward recrystallize
with a preferential orientation. NC-based Bi<sub>2</sub>Te<sub>3â<i>x</i></sub>Se<sub><i>x</i></sub> nanomaterials showed
very high electrical conductivities associated with large charge carrier
concentrations, <i>n</i>. We hypothesize that such large <i>n</i> resulted from the presence of an excess of tellurium during
processing, which introduced a high density of donor Te<sub>Bi</sub> antisites. Additionally, the presence in between grains of traces
of elemental Te, a narrow band gap semiconductor with a work function
well below Bi<sub>2</sub>Te<sub>3â<i>x</i></sub>Se<sub><i>x</i></sub>, might further contribute to increase <i>n</i> through spillover of electrons, while at the same time
blocking phonon propagation and hole transport through the nanomaterial.
NC-based Bi<sub>2</sub>Te<sub>3â<i>x</i></sub>Se<sub><i>x</i></sub> nanomaterials were characterized by very
low thermal conductivities in the pressing direction, which resulted
in <i>ZT</i> values up to 1.31 at 438 K in this direction.
This corresponds to a <i>ca</i>. 40% <i>ZT</i> enhancement from commercial ingots. Additionally, high <i>ZT</i> values were extended over wider temperature ranges due to reduced
bipolar contribution to the Seebeck coefficient and the thermal conductivity.
Average <i>ZT</i> values up to 1.15 over a wide temperature
range, 320 to 500 K, were measured, which corresponds to a <i>ca</i>. 50% increase over commercial materials in the same temperature
range. Contrary to most previous works, highest <i>ZT</i> values were obtained in the pressing direction, corresponding to
the <i>c</i> crystallographic axis, due to the predominance
of the thermal conductivity reduction over the electrical conductivity
difference when comparing the two crystal directions