Issue 22, 2020

Structure of bismuth tellurite and bismuth niobium tellurite glasses and Bi2Te4O11 anti-glass by high energy X-ray diffraction

Abstract

Glass and anti-glass samples of bismuth tellurite (xBi2O3–(100 − x)TeO2) and bismuth niobium tellurite (xBi2O3xNb2O5–(100 − 2x)TeO2) systems were prepared by melt-quenching. The bismuth tellurite system forms glasses at low Bi2O3 concentration of 3 to 7 mol%. At 20 mol% Bi2O3, the glass forming ability of the Bi2O3–TeO2 system decreases drastically and the anti-glass phase of monoclinic Bi2Te4O11 is produced. Structures of glass and the anti-glass Bi2Te4O11 samples were studied by high-energy X-ray diffraction, reverse Monte Carlo simulations and Rietveld Fullprof refinement. All glasses have short short-range disorder due to the existence of at least three types of Te–O bonds of lengths: 1.90, 2.25 and 2.59 Å, besides a variety of Bi–O and Nb–O bond-lengths. The medium-range order in glasses is also disturbed due to the distribution of Te–Te pair distances. The average Te–O co-ordination (NTe–O) in the glass network decreases with an increase in Bi2O3 and Nb2O5 mol% and is in the range: 4.17 to 3.56. The anti-glass Bi2Te4O11 has a long-range order of cations but it has vibrational disorder and it exhibits sharp X-ray reflections but broad vibrational bands similar to that in glasses. Anti-glass Bi2Te4O11 has an NTe–O of 2.96 and is significantly lower than in glass samples.

Graphical abstract: Structure of bismuth tellurite and bismuth niobium tellurite glasses and Bi2Te4O11 anti-glass by high energy X-ray diffraction

Article information

Article type
Paper
Submitted
14 Feb 2020
Accepted
24 Mar 2020
First published
02 Apr 2020
This article is Open Access
Creative Commons BY-NC license

RSC Adv., 2020,10, 13237-13251

Structure of bismuth tellurite and bismuth niobium tellurite glasses and Bi2Te4O11 anti-glass by high energy X-ray diffraction

N. Gupta, A. Khanna, Hirdesh, A. Dippel and O. Gutowski, RSC Adv., 2020, 10, 13237 DOI: 10.1039/D0RA01422B

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