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

    No full text
    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

    No full text
    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

    No full text
    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
    corecore