1 research outputs found
New Transparent Glass-Ceramics Based on the Crystallization of āAnti-glassā Spherulites in the Bi<sub>2</sub>O<sub>3</sub>āNb<sub>2</sub>O<sub>5</sub>āTeO<sub>2</sub> System
The crystallization of the Bi<sub>0.5</sub>Nb<sub>0.5</sub>Te<sub>3</sub>O<sub>8</sub> (7.14 Bi<sub>2</sub>O<sub>3</sub>ā7.14Nb<sub>2</sub>O<sub>5</sub>ā85.72TeO<sub>2</sub>) glass composition
shows numerous original spherulite-like shape or ādropletsā
crystalline domains through the bulk. Both SEM-EDS and microprobe
measurements demonstrate that both these droplets and the glassy matrix
present the same composition. The combination of information obtained
from various complementary techniques, electron probe microanalysis,
Raman, and SEM-EDS, then leads to the identification of the spherulites
as a new Bi<sub>0.5</sub>Nb<sub>0.5</sub>Te<sub>3</sub>O<sub>8</sub> āanti-glassā phase. However, the crystallization mechanism
is complex since microcracks are observed at the surface of the spherulites
in some glass-ceramic materials, suggesting a confined crystal growth.
Therefore, the crystallization process appears much different from
a homogeneous congruent crystallization. The photoluminescence (PL)
properties of the (1 wt %) Er<sub>2</sub>O<sub>3</sub>-doped Bi<sub>0.5</sub>Nb<sub>0.5</sub>Te<sub>3</sub>O<sub>8</sub> glass-ceramics
were investigated during isothermal crystallization of the parent
glass at 380 Ā°C. The evolution of the PL signal (<sup>4</sup>I<sub>13/2</sub> ā <sup>4</sup>I<sub>15/2</sub> transition)
enables indirect detection of the first steps of crystallization.
Moreover, the PL data indicate random nucleation with respect to the
location of Er<sup>3+</sup> ions, whereas the integrated PL intensity
and lifetime values show very comparable evolution trends as a function
of the crystallization rate