Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system
Nd-doped Tellurite glasses of the (80-x)TeO2-10PbO-10Li2O-xNd2O3 system, where x = 0.5, 1.0, 1.5, 2.0, 2.5 and 3.0 mol% have successfully been synthesized by melt-quenching techniques. Their absorption spectra had been characterized in the ranges of 400-900 nm while the luminescence spectra are meas...
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my.utm.67292017-09-07T03:44:46Z http://eprints.utm.my/id/eprint/6729/ Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system Sahar, M. R. Kassim, Azman Rohani, M. S. Ariffin, R. QC Physics Nd-doped Tellurite glasses of the (80-x)TeO2-10PbO-10Li2O-xNd2O3 system, where x = 0.5, 1.0, 1.5, 2.0, 2.5 and 3.0 mol% have successfully been synthesized by melt-quenching techniques. Their absorption spectra had been characterized in the ranges of 400-900 nm while the luminescence spectra are measured in the range of 400 to 1500 nm. The experimental, and calculated, oscillator strength results are found to vary from 1.1566 x 10-6 to 0.8041 x 10-6 and from 1.0257 x 10-6 to 0.7715 x 10-6 with respect to the Nd3+content respectively. Meanwhile, the Judd-Ofelt parameters, varies from 3.472 x 1020cm2 to 2.576 x 1020cm2, varies from 2.110 x 1020cm2 to 2.108 x 1020cm2 and varies from 2.424 x 1020cm2 to 2.392 x 1020cm2 with respect to Nd3+ content. From the luminescence spectra it is observed that the emission occurs at 485nm, 560nm, 605nm, 880nm, 1062nm and 1340nm, which is due to 4G9/2 → 4I9/2, 2G9/2 → 4I11/2 , 2H11/2 → 4I9/2 , 4F3/2 → 4I9/2 , 4F3/2 → 4I11/2 and 4F3/2 → 4I13/2 transitions respectively. 2008 Article NonPeerReviewed application/msword en http://eprints.utm.my/id/eprint/6729/1/rahimsahar-PAPER_optial_SPECTROSCOPY1.doc Sahar, M. R. and Kassim, Azman and Rohani, M. S. and Ariffin, R. (2008) Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system. - . (Unpublished) |
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QC Physics Sahar, M. R. Kassim, Azman Rohani, M. S. Ariffin, R. Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system |
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Nd-doped Tellurite glasses of the (80-x)TeO2-10PbO-10Li2O-xNd2O3 system, where x = 0.5, 1.0, 1.5, 2.0, 2.5 and 3.0 mol% have successfully been synthesized by melt-quenching techniques. Their absorption spectra had been characterized in the ranges of 400-900 nm while the luminescence spectra are measured in the range of 400 to 1500 nm. The experimental, and calculated, oscillator strength results are found to vary from 1.1566 x 10-6 to 0.8041 x 10-6 and from 1.0257 x 10-6 to 0.7715 x 10-6 with respect to the Nd3+content respectively. Meanwhile, the Judd-Ofelt parameters, varies from 3.472 x 1020cm2 to 2.576 x 1020cm2, varies from 2.110 x 1020cm2 to 2.108 x 1020cm2 and varies from 2.424 x 1020cm2 to 2.392 x 1020cm2 with respect to Nd3+ content. From the luminescence spectra it is observed that the emission occurs at 485nm, 560nm, 605nm, 880nm, 1062nm and 1340nm, which is due to 4G9/2 → 4I9/2, 2G9/2 → 4I11/2 , 2H11/2 → 4I9/2 , 4F3/2 → 4I9/2 , 4F3/2 → 4I11/2 and 4F3/2 → 4I13/2 transitions respectively. |
format |
Article |
author |
Sahar, M. R. Kassim, Azman Rohani, M. S. Ariffin, R. |
author_facet |
Sahar, M. R. Kassim, Azman Rohani, M. S. Ariffin, R. |
author_sort |
Sahar, M. R. |
title |
Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system |
title_short |
Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system |
title_full |
Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system |
title_fullStr |
Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system |
title_full_unstemmed |
Optical properties of the TeO2-PbO-Li2O-Nd2O3 glass system |
title_sort |
optical properties of the teo2-pbo-li2o-nd2o3 glass system |
publishDate |
2008 |
url |
http://eprints.utm.my/id/eprint/6729/1/rahimsahar-PAPER_optial_SPECTROSCOPY1.doc http://eprints.utm.my/id/eprint/6729/ |
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13.160551 |