3 research outputs found
Importance of Suppression of Yb<sup>3+</sup> De-Excitation to Upconversion Enhancement in β‑NaYF<sub>4</sub>: Yb<sup>3+</sup>/Er<sup>3+</sup>@β-NaYF<sub>4</sub> Sandwiched Structure Nanocrystals
Nanosized
Yb<sup>3+</sup> and Er<sup>3+</sup> co-doped β-NaYF<sub>4</sub> cores coated with multiple β-NaYF<sub>4</sub> shell layers
were synthesized by a solvothermal process. X-ray diffraction and
scanning electron microscopy were used to characterize the crystal
structure and morphology of the materials. The visible and near-infrared
spectra as well as the decay curves were also measured. A 40-fold
intensity increase for the green upconversion and a 34-fold intensity
increase for the red upconversion were observed as the cores are coated
with three shell layers. The origin of the upconversion enhancement
was studied on the basis of photoluminescence spectra and decay times.
Our results indicate that the upconversion enhancement in the sandwiched
structure mainly originates from the suppression of de-excitation
of Yb<sup>3+</sup> ions. We also explored the population of the Er<sup>3+4</sup>F<sub>9/2</sub> level. The results reveal that energy transfer
from the lower intermediate Er<sup>3+4</sup>I<sub>13/2</sub> level
is dominant for populating the Er<sup>3+4</sup>F<sub>9/2</sub> level
when the nanocrystal size is relatively small; however, with increasing
nanocrystal size, the contribution of the green emitting Er<sup>3+4</sup>S<sub>3/2</sub> level for populating the Er<sup>3+4</sup>F<sub>9/2</sub> level, which mainly comes from the cross relaxation energy transfer
from Er<sup>3+</sup> ions to Yb<sup>3+</sup> ions followed by energy
back transfer within the same Er<sup>3+</sup>–Yb<sup>3+</sup> pair, becomes more and more important. Moreover, this mechanism
takes place only in the nearest Er<sup>3+</sup>–Yb<sup>3+</sup> pairs. This population route is in good agreement with that in nanomaterials
and bulk materials
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