4 research outputs found
Ultrasensitive Detection of <i>Shigella</i> Species in Blood and Stool
A modified immunosensing system with
voltage-controlled signal
amplification was used to detect <i>Shigella</i> in stool
and blood matrixes at the single-digit CFU level. Inactivated <i>Shigella</i> was spiked in these matrixes and detected directly.
The detection was completed in 78 min. Detection limits of 21 CFU/mL
and 18 CFU/mL were achieved in stool and blood, respectively, corresponding
to 2–7 CFUs immobilized on the detecting electrode. The outcome
of the detection of extremely low bacterium concentration, i.e., below
100 CFU/mL, blood samples show a random nature. An analysis of the
detection probabilities indicates the correlation between the sample
volume and the success of detection and suggests that sample volume
is critical for ultrasensitive detection of bacteria. The calculated
detection limit is qualitatively in agreement with the empirically
determined detection limit. The demonstrated ultrasensitive detection
of <i>Shigella</i> on the single-digit CFU level suggests
the feasibility of the direct detection of the bacterium in the samples
without performing a culture
Improvement of Green Upconversion Monochromaticity by Doping Eu<sup>3+</sup> in Lu<sub>2</sub>O<sub>3</sub>:Yb<sup>3+</sup>/Ho<sup>3+</sup> Powders with Detailed Investigation of the Energy Transfer Mechanism
The monochromaticity
improvement of green upconversion (UC) in Lu<sub>2</sub>O<sub>3</sub>:Yb<sup>3+</sup>/Ho<sup>3+</sup> powders has been successfully realized
by tridoping Eu<sup>3+</sup>. The integral area ratio of green emission
to red emission of Ho<sup>3+</sup> increases 4.3 times with increasing
Eu<sup>3+</sup> doping concentration from 0 to 20 mol %. The energy
transfer (ET) mechanism in the Yb<sup>3+</sup>/Ho<sup>3+</sup>/Eu<sup>3+</sup> tridoping system has been investigated carefully by visible
and near-infrared (NIR) emission spectra along with the decay curves,
revealing the existence of ET from the Ho<sup>3+</sup> <sup>5</sup>F<sub>4</sub>/<sup>5</sup>S<sub>2</sub> level tothe Eu<sup>3+</sup> <sup>5</sup>D<sub>0</sub> level and ET from the Ho<sup>3+</sup> <sup>5</sup>I<sub>6</sub> level to the Eu<sup>3+</sup> <sup>7</sup>F<sub>6</sub> level. In addition, the population routes of the red-emitting
Ho<sup>3+</sup> <sup>5</sup>F<sub>5</sub> level in the Yb<sup>3+</sup>/Ho<sup>3+</sup> codoped system under 980 nm wavelength excitation
have also been explored. The ET process from the Yb<sup>3+</sup> <sup>2</sup>F<sub>5/2</sub> level to the Ho<sup>3+</sup> <sup>5</sup>I<sub>7</sub> level and the cross-relaxation process between two nearby
Ho<sup>3+</sup> ions in the <sup>5</sup>F<sub>4</sub>/<sup>5</sup>S<sub>2</sub> level and <sup>5</sup>I<sub>7</sub> level, respectively,
have been demonstrated to be the dominant approaches for populating
the Ho<sup>3+</sup> <sup>5</sup>F<sub>5</sub> level. The multiphonon
relaxation process originating from the Ho<sup>3+</sup> <sup>5</sup>F<sub>4</sub>/<sup>5</sup>S<sub>2</sub> level is useless to populate
the Ho<sup>3+</sup> <sup>5</sup>F<sub>5</sub> level. As the energy
level gap between the Ho<sup>3+</sup> <sup>5</sup>I<sub>7</sub> level
and Ho<sup>3+</sup> <sup>5</sup>I<sub>8</sub> level matches well with
that between Eu<sup>3+</sup> <sup>7</sup>F<sub>6</sub> level and Eu<sup>3+</sup> <sup>7</sup>F<sub>0</sub> level, the energy of the Ho<sup>3+</sup> <sup>5</sup>I<sub>7</sub> level can be easily transferred
to the Eu<sup>3+</sup> <sup>7</sup>F<sub>6</sub> level by an approximate
resonant ET process, resulting in a serious decrease in the red UC
emission intensity. Since this ET process is more efficient than the
ET from the Ho<sup>3+</sup> <sup>5</sup>F<sub>4</sub>/<sup>5</sup>S<sub>2</sub> level to the Eu<sup>3+</sup> <sup>5</sup>D<sub>0</sub> level as well as the ET from the Ho<sup>3+</sup> <sup>5</sup>I<sub>6</sub> level to the Eu<sup>3+</sup> <sup>7</sup>F<sub>6</sub> level,
the integral area ratio of green emission to red emission of Ho<sup>3+</sup> has been improved significantly
Enhancement of Eu<sup>3+</sup> Red Upconversion in Lu<sub>2</sub>O<sub>3</sub>: Yb<sup>3+</sup>/Eu<sup>3+</sup> Powders under the Assistance of Bridging Function Originated from Ho<sup>3+</sup> Tridoping
The red upconversion
(UC) emission of Eu<sup>3+</sup> ions in Lu<sub>2</sub>O<sub>3</sub>: Yb<sup>3+</sup>/Eu<sup>3+</sup> powders was successfully enhanced
by tridoping Ho<sup>3+</sup> ions in the matrix, which is due to the
bridging function of Ho<sup>3+</sup> ions. The experiment data manifest
that, in Yb<sup>3+</sup>/Eu<sup>3+</sup>/Ho<sup>3+</sup> tridoped
system, the Ho<sup>3+</sup> ions are first populated to the green
emitting level <sup>5</sup>F<sub>4</sub>/<sup>5</sup>S<sub>2</sub> through the energy transfer (ET) processes from the excited Yb<sup>3+</sup> ions. Subsequently, the Ho<sup>3+</sup> ions at <sup>5</sup>F<sub>4</sub>/<sup>5</sup>S<sub>2</sub> level can transfer their
energy to the Eu<sup>3+</sup> ions at the ground state, resulting
in the population of Eu<sup>3+</sup> <sup>5</sup>D<sub>0</sub> level.
With the assistance of the bridging function of Ho<sup>3+</sup> ion,
this ET process is more efficient than the cooperative sensitization
process between Yb<sup>3+</sup> ion and Eu<sup>3+</sup> ion. Compared
with Lu<sub>2</sub>O<sub>3</sub>: 5 mol % Yb<sup>3+</sup>/1 mol %
Eu<sup>3+</sup>, the UC intensity of Eu<sup>3+</sup> <sup>5</sup>D<sub>0</sub>→<sup>7</sup>F<sub>2</sub> transition in Lu<sub>2</sub>O<sub>3</sub>: 5 mol % Yb<sup>3+</sup>/1 mol % Eu<sup>3+</sup>/0.5
mol % Ho<sup>3+</sup> is increased by a factor of 8
Stacking faults enabled second harmonic generation in centrosymmetric van der Waals RhI3
Second harmonic generation (SHG) in van der Waals (vdWs) materials has garnered significant attention due to its potential for integrated nonlinear optical and optoelectronic applications. Stacking faults in vdWs materials, a typical kind of planar defect, can introduce a new degree of freedom to modulate the crystal symmetry and resultant SHG response, however, the physical origin and tunability of stacking-fault-governed SHG in vdWs materials remain unclear. Here, taking the intrinsically centrosymmetric vdWs RhI3 as an example, we theoretically reveal the origin of stacking-fault-governed SHG response, where the SHG response comes from the energetically favorable AC- Cstacking fault of which the electrical transitions along the high symmetry paths Gamma-M and Gamma-K in the Brillion zone play the dominant role at 810 nm. Such stacking-fault-governed SHG response is further confirmed via structural characterizations and SHG measurements. Furthermore, by applying hydrostatic pressure on RhI3, the correlation between structural evolution and SHG response is revealed with SHG enhancement up to 6.9 times, where the decreased electronic transition energies and huger momentum matrix elements due to the stronger interlayer interactions upon compression magnify the SHG susceptibility. This study develops a promising foundation based on strategically designed stacking faults for pioneering new avenues in nonlinear nano-optics