An Approach to Estimate the Refractive Index and the Electronic Polarizability of the Ternary Ag <sub>2</sub> O‐B <sub>2</sub> O <sub>3</sub> ‐TeO <sub>2</sub> Glasses

Each of the static properties such as refractive index (n<sub>0</sub>), cation ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mrow><mml:mo>∑</mml:mo> <mml:msub><mml:mi>α</mml:mi> <mml:mi>i</mml:mi></mml:msub> </mml:mrow> <mml:annotation>$$ \sum {\alpha}_i $$</mml:annotation></mml:semantics> </mml:math> ), and anion ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics> <mml:mrow><mml:msubsup><mml:mi>α</mml:mi> <mml:mi>O</mml:mi> <mml:mrow><mml:mn>2</mml:mn> <mml:mo>-</mml:mo></mml:mrow> </mml:msubsup> </mml:mrow> <mml:annotation>$$ {\alpha}_O^{2-} $$</mml:annotation></mml:semantics> </mml:math> ) oxide polarizabilities for the ternary 30Ag<sub>2</sub>O⋅xB<sub>2</sub>O<sub>3</sub>⋅(70 - x)TeO<sub>2</sub> (30AgBTe) glasses has been predicted theoretically from those of the binary 30Ag<sub>2</sub>O-70B<sub>2</sub>O<sub>3</sub> and 30Ag<sub>2</sub>O-70TeO<sub>2</sub> glasses. This can be done based on two assumptions: that each of these static properties (n<sub>0</sub>, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mrow><mml:mo>∑</mml:mo> <mml:msub><mml:mi>α</mml:mi> <mml:mi>i</mml:mi></mml:msub> </mml:mrow> <mml:annotation>$$ \sum {\upalpha}_i $$</mml:annotation></mml:semantics> </mml:math> , and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics> <mml:mrow><mml:msubsup><mml:mi>α</mml:mi> <mml:mi>O</mml:mi> <mml:mrow><mml:mn>2</mml:mn> <mml:mo>-</mml:mo></mml:mrow> </mml:msubsup> </mml:mrow> <mml:annotation>$$ {\upalpha}_{\mathrm{O}}^{2-} $$</mml:annotation></mml:semantics> </mml:math> ) can be considered as an additive property and that ternary 30AgBTe glasses can be treated as a mixture of two binary 30Ag<sub>2</sub>O-70B<sub>2</sub>O<sub>3</sub> and 30Ag<sub>2</sub>O-70TeO<sub>2</sub> glasses. In addition, n<sub>0</sub> values for the ternary 30AgBTe glasses can be predicted in terms of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics> <mml:mrow><mml:msubsup><mml:mi>α</mml:mi> <mml:mi>O</mml:mi> <mml:mrow><mml:mn>2</mml:mn> <mml:mo>-</mml:mo></mml:mrow> </mml:msubsup> </mml:mrow> <mml:annotation>$$ {\upalpha}_{\mathrm{O}}^{2-} $$</mml:annotation></mml:semantics> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mrow><mml:mo>∑</mml:mo> <mml:msub><mml:mi>α</mml:mi> <mml:mi>i</mml:mi></mml:msub> </mml:mrow> <mml:annotation>$$ \sum {\upalpha}_i $$</mml:annotation></mml:semantics> </mml:math> values for the ternary 30AgBTe glasses, and these later properties can be predicted from that of two binaries like as n<sub>0</sub> at first stage. The n<sub>0</sub> values obtained by using two methods are exactly the same for the corresponding compositions in the studied glasses, confirming the validity of the two assumptions and the procedure described in the present work. This conclusion is valid for the ternary glasses with a fixed content of either basic former/or modifier oxides for all compositions such as xPbO⋅(40 - x)Sb<sub>2</sub>O<sub>3</sub>⋅60B<sub>2</sub>O<sub>3</sub> and 30Ag<sub>2</sub>O⋅xB<sub>2</sub>O<sub>3</sub>⋅(70 - x)TeO<sub>2</sub> glasses, respectively.

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Journal
Luminescence
Published
2024-10-01
DOI
https://doi.org/10.1002/bio.4931
Primary Topic
Glass properties and applications
Type
article
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article

An Approach to Estimate the Refractive Index and the Electronic Polarizability of the Ternary Ag 2 O‐B 2 O 3 ‐TeO 2 Glasses

A.A. Al‐Muntaser, E.F. El Agammy, Eman Alzahrani, Abdullah F. Al Naim et al.
Luminescence
Glass properties and applications
article

An Approach to Estimate the Refractive Index and the Electronic Polarizability of the Ternary Ag 2 O‐B 2 O 3 ‐TeO 2 Glasses

A.A. Al‐Muntaser, E.F. El Agammy, Eman Alzahrani, Abdullah F. Al Naim, M. El‐Zaibani
article en

Abstract

Each of the static properties such as refractive index (n<sub>0</sub>), cation ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mrow><mml:mo>∑</mml:mo> <mml:msub><mml:mi>α</mml:mi> <mml:mi>i</mml:mi></mml:msub> </mml:mrow> <mml:annotation>$$ \sum {\alpha}_i $$</mml:annotation></mml:semantics> </mml:math> ), and anion ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics> <mml:mrow><mml:msubsup><mml:mi>α</mml:mi> <mml:mi>O</mml:mi> <mml:mrow><mml:mn>2</mml:mn> <mml:mo>-</mml:mo></mml:mrow> </mml:msubsup> </mml:mrow> <mml:annotation>$$ {\alpha}_O^{2-} $$</mml:annotation></mml:semantics> </mml:math> ) oxide polarizabilities for the ternary 30Ag<sub>2</sub>O⋅xB<sub>2</sub>O<sub>3</sub>⋅(70 - x)TeO<sub>2</sub> (30AgBTe) glasses has been predicted theoretically from those of the binary 30Ag<sub>2</sub>O-70B<sub>2</sub>O<sub>3</sub> and 30Ag<sub>2</sub>O-70TeO<sub>2</sub> glasses. This can be done based on two assumptions: that each of these static properties (n<sub>0</sub>, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mrow><mml:mo>∑</mml:mo> <mml:msub><mml:mi>α</mml:mi> <mml:mi>i</mml:mi></mml:msub> </mml:mrow> <mml:annotation>$$ \sum {\upalpha}_i $$</mml:annotation></mml:semantics> </mml:math> , and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics> <mml:mrow><mml:msubsup><mml:mi>α</mml:mi> <mml:mi>O</mml:mi> <mml:mrow><mml:mn>2</mml:mn> <mml:mo>-</mml:mo></mml:mrow> </mml:msubsup> </mml:mrow> <mml:annotation>$$ {\upalpha}_{\mathrm{O}}^{2-} $$</mml:annotation></mml:semantics> </mml:math> ) can be considered as an additive property and that ternary 30AgBTe glasses can be treated as a mixture of two binary 30Ag<sub>2</sub>O-70B<sub>2</sub>O<sub>3</sub> and 30Ag<sub>2</sub>O-70TeO<sub>2</sub> glasses. In addition, n<sub>0</sub> values for the ternary 30AgBTe glasses can be predicted in terms of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics> <mml:mrow><mml:msubsup><mml:mi>α</mml:mi> <mml:mi>O</mml:mi> <mml:mrow><mml:mn>2</mml:mn> <mml:mo>-</mml:mo></mml:mrow> </mml:msubsup> </mml:mrow> <mml:annotation>$$ {\upalpha}_{\mathrm{O}}^{2-} $$</mml:annotation></mml:semantics> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:mrow><mml:mo>∑</mml:mo> <mml:msub><mml:mi>α</mml:mi> <mml:mi>i</mml:mi></mml:msub> </mml:mrow> <mml:annotation>$$ \sum {\upalpha}_i $$</mml:annotation></mml:semantics> </mml:math> values for the ternary 30AgBTe glasses, and these later properties can be predicted from that of two binaries like as n<sub>0</sub> at first stage. The n<sub>0</sub> values obtained by using two methods are exactly the same for the corresponding compositions in the studied glasses, confirming the validity of the two assumptions and the procedure described in the present work. This conclusion is valid for the ternary glasses with a fixed content of either basic former/or modifier oxides for all compositions such as xPbO⋅(40 - x)Sb<sub>2</sub>O<sub>3</sub>⋅60B<sub>2</sub>O<sub>3</sub> and 30Ag<sub>2</sub>O⋅xB<sub>2</sub>O<sub>3</sub>⋅(70 - x)TeO<sub>2</sub> glasses, respectively.

LuminescenceVol. 39(10)
Sana'a University (YE), Taif University (SA), Jouf University (SA), Amran University (YE), King Faisal University (SA)
Taif University
Openalex Percentile: Top 90%
Glass properties and applications
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