Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass

Optimizing the rare earth doping in inorganic binary glasses for tuneable structural and optical properties is ever-demanding for lasing glass. A series of Er3+ and Nd3+ doped lithium niobate tellurite glasses with compositions of (70-x-y)TeO2–15Li2CO3–15Nb2O5–(x)Er2O3–(y)Nd2O3, where x = 0.0, 1.0 m...

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Main Authors: Hasim, N., Rohani, M. S., Sahar, M. R.
Format: Conference or Workshop Item
Published: Trans Tech Publications Ltd 2016
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Online Access:http://eprints.utm.my/id/eprint/73593/
https://www.scopus.com/inward/record.uri?eid=2-s2.0-84959885119&doi=10.4028%2fwww.scientific.net%2fMSF.846.126&partnerID=40&md5=0a9cb4f6b9247946d1a0a00e62400fbb
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spelling my.utm.735932017-11-28T05:01:12Z http://eprints.utm.my/id/eprint/73593/ Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass Hasim, N. Rohani, M. S. Sahar, M. R. QC Physics Optimizing the rare earth doping in inorganic binary glasses for tuneable structural and optical properties is ever-demanding for lasing glass. A series of Er3+ and Nd3+ doped lithium niobate tellurite glasses with compositions of (70-x-y)TeO2–15Li2CO3–15Nb2O5–(x)Er2O3–(y)Nd2O3, where x = 0.0, 1.0 mol % and 0 ≤ y ≤ 1.0 mol% are synthesized using melt-quench technique. Influence of Nd3+ ion concentrations on physical and optical behaviour is examined. X–Ray diffraction pattern confirm the amorphous nature of glasses. The strong dependence of spectral properties on rare-earth dopant indicates the alteration in structures and bonding of glass network. The structural properties of the glass represented by the FTIR spectrum indicate that as Nd2O3 content increases, the sharp infrared absorption peaks are shifted from 474.7 cm-1 to 499.4 cm-1. These peaks are due to Nb-O, Te-O-Te and O-Te-O bond linkage bending vibrations. For TeO4 trigonal bipyramid, the peak occurred at 676.5 cm-1 whereas for TeO3 trigonal pyramid, two infrared band peaks are found at 787.5 cm-1 and 887.6cm-1, respectively. The absorption peaks around 1382.7 cm-1 is due to the Te-O-Nb stretching vibration while peaks at 1635.5cm-1 and 3411.7 cm-1 are due to the stretching vibrations of the hydroxyl group participating in the strong metal bonding as well as in the hydrogen bonding, respectively. Trans Tech Publications Ltd 2016 Conference or Workshop Item PeerReviewed Hasim, N. and Rohani, M. S. and Sahar, M. R. (2016) Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass. In: 28th Regional Conference on Solid State Science and Technology, RCSSST 2014, 25-27 Nov 2014, Pahang, Malaysia. https://www.scopus.com/inward/record.uri?eid=2-s2.0-84959885119&doi=10.4028%2fwww.scientific.net%2fMSF.846.126&partnerID=40&md5=0a9cb4f6b9247946d1a0a00e62400fbb
institution Universiti Teknologi Malaysia
building UTM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Teknologi Malaysia
content_source UTM Institutional Repository
url_provider http://eprints.utm.my/
topic QC Physics
spellingShingle QC Physics
Hasim, N.
Rohani, M. S.
Sahar, M. R.
Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
description Optimizing the rare earth doping in inorganic binary glasses for tuneable structural and optical properties is ever-demanding for lasing glass. A series of Er3+ and Nd3+ doped lithium niobate tellurite glasses with compositions of (70-x-y)TeO2–15Li2CO3–15Nb2O5–(x)Er2O3–(y)Nd2O3, where x = 0.0, 1.0 mol % and 0 ≤ y ≤ 1.0 mol% are synthesized using melt-quench technique. Influence of Nd3+ ion concentrations on physical and optical behaviour is examined. X–Ray diffraction pattern confirm the amorphous nature of glasses. The strong dependence of spectral properties on rare-earth dopant indicates the alteration in structures and bonding of glass network. The structural properties of the glass represented by the FTIR spectrum indicate that as Nd2O3 content increases, the sharp infrared absorption peaks are shifted from 474.7 cm-1 to 499.4 cm-1. These peaks are due to Nb-O, Te-O-Te and O-Te-O bond linkage bending vibrations. For TeO4 trigonal bipyramid, the peak occurred at 676.5 cm-1 whereas for TeO3 trigonal pyramid, two infrared band peaks are found at 787.5 cm-1 and 887.6cm-1, respectively. The absorption peaks around 1382.7 cm-1 is due to the Te-O-Nb stretching vibration while peaks at 1635.5cm-1 and 3411.7 cm-1 are due to the stretching vibrations of the hydroxyl group participating in the strong metal bonding as well as in the hydrogen bonding, respectively.
format Conference or Workshop Item
author Hasim, N.
Rohani, M. S.
Sahar, M. R.
author_facet Hasim, N.
Rohani, M. S.
Sahar, M. R.
author_sort Hasim, N.
title Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
title_short Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
title_full Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
title_fullStr Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
title_full_unstemmed Structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
title_sort structural characteristics of er3+ and nd3+ doped lithium niobate tellurite glass
publisher Trans Tech Publications Ltd
publishDate 2016
url http://eprints.utm.my/id/eprint/73593/
https://www.scopus.com/inward/record.uri?eid=2-s2.0-84959885119&doi=10.4028%2fwww.scientific.net%2fMSF.846.126&partnerID=40&md5=0a9cb4f6b9247946d1a0a00e62400fbb
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score 13.18916