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M2O3 = Al2O3, Ga2O3, Sc2O3, La2O3, Bi2O3 - Ceramics-Silikaty

M2O3 = Al2O3, Ga2O3, Sc2O3, La2O3, Bi2O3 - Ceramics-Silikaty

M2O3 = Al2O3, Ga2O3, Sc2O3, La2O3, Bi2O3 - Ceramics-Silikaty

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Figure 1. Boundaries between one- and two-phase glass regions<br />

in the systems TeO 2-B 2O 3-M 2O 3: M 2O 3= (1) Al 2O 3; (2) Ga 2O 3;<br />

(3) Sc 2O 3; (4) La 2O 3; (5) Bi 2O 3.<br />

The results of TEM observations show the<br />

influence of the third component on the immiscibility<br />

tendency in different tellurite-borate glasses. In our<br />

previous works [5 - 8], the pronounced trend for cluster<br />

formation in slowly cooled pure vitreous B 2O 3 (v-B 2O 3)<br />

has been discussed. The presence of nano-scale<br />

heterogeneities in v-B 2O 3 ranging in sizes between 1.5 -<br />

2 nm was experimentally established by TEM data<br />

[6, 7]. According to the classification of Zarzycki [9]<br />

and Porai-Koshits [10], they were associated with the<br />

thermal density fluctuations. By means of MM<br />

computer simulation, we made an attempt to model the<br />

cluster formation in borate network at the presence of<br />

BO 3-groups and B 3O 6-boroxol rings [5, 7, 8]. The<br />

addition of TeO 2, containing mainly TeO 3-groups,<br />

stimulates the clustering at micro-scale level [5, 7] and<br />

leads to appearance of metastable phase separation. In<br />

this sense, the role of the third component should be<br />

assigned to its influence on the formation of different<br />

borate or tellurite complexes.<br />

Some typical IR-spectra of chosen compositions in<br />

binary and three component systems are shown in<br />

figures 5 and 6. Their interpretation is based on IR data<br />

analysis of borate glasses [11 - 15]. According to the<br />

obtained IR-spectra the B 2O 3 participates as BO 3- (1380<br />

and 1240 cm -1 ) and BO 4-groups (900 cm -1 ) in the<br />

network of the binary tellurite glass, in spite the small<br />

B 2O 3 amount in the composition (figure 5 - 1). Similar<br />

spectra are obtained when La 2O 3 is added to TeO 2-B 2O 3<br />

glass, but the intensity of the band at 1325 cm -1<br />

increases at the expense of the band at 1215 cm -1 ,<br />

leading to an increase in the tendency for formation of<br />

superstructural units containing BO 3- and BO 4-groups<br />

(figure 5 - 2). This trend is developed (1380, 1050 and<br />

940 cm -1 ) for composition with higher B 2O 3 content<br />

E. Kashchieva, M. Pankova, Y. Dimitriev<br />

Figure 2. Immiscibility droplets and micro-aggregates in onephase<br />

glass with composition 70TeO 2,20B 2O 3,10Bi 2O 3<br />

(mol.%).<br />

Figure 3. B 2O 3-enriched immiscibility droplets in the low layer<br />

of two-phase glass with composition 20TeO 2,70B 2O 3,10 Ga 2O 3<br />

(mol.%).<br />

Figure 4. Microcrystals dispersed in amorphous matrix of glass<br />

with composition 50TeO 2,30B 2O 3,20Al 2O 3 (mol.%).<br />

112 <strong>Ceramics</strong> − Silikáty 45 (3) 111-114 (2001)

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