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Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods

(Tl(2)O(3))(30)-(Li(2)O)(10)-(B(2)O(3))((60−y)())-(Sm(2)O(3))(y) glass system with various Sm(2)O(3) additives (y = 0, 0.2, 0.4, 0.6) was studied in detail. The vibrational modes of the (Tl(2)O(3))(30)-(Li(2)O)(10)-(B(2)O(3))((60−y)) network were active at three composition-related IR spectral peaks...

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Autores principales: Issa, Shams A. M., Zakaly, Hesham M. H., Tekin, Huseyin O., Saudi, Heba A., Badawi, Ali, Pyshkina, Mariia, Susoy, Gulfem, Elazaka, Ahmed I., Ene, Antoaneta
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8306404/
https://www.ncbi.nlm.nih.gov/pubmed/34209698
http://dx.doi.org/10.3390/nano11071713
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author Issa, Shams A. M.
Zakaly, Hesham M. H.
Tekin, Huseyin O.
Saudi, Heba A.
Badawi, Ali
Pyshkina, Mariia
Susoy, Gulfem
Elazaka, Ahmed I.
Ene, Antoaneta
author_facet Issa, Shams A. M.
Zakaly, Hesham M. H.
Tekin, Huseyin O.
Saudi, Heba A.
Badawi, Ali
Pyshkina, Mariia
Susoy, Gulfem
Elazaka, Ahmed I.
Ene, Antoaneta
author_sort Issa, Shams A. M.
collection PubMed
description (Tl(2)O(3))(30)-(Li(2)O)(10)-(B(2)O(3))((60−y)())-(Sm(2)O(3))(y) glass system with various Sm(2)O(3) additives (y = 0, 0.2, 0.4, 0.6) was studied in detail. The vibrational modes of the (Tl(2)O(3))(30)-(Li(2)O)(10)-(B(2)O(3))((60−y)) network were active at three composition-related IR spectral peaks that differed from those mixed with Samarium (III) oxide at high wavenumber ranges. These glass samples show that their permeability increased with the Samarium (III) oxide content increase. Additionally, the electronic transition between localized states was observed in the samples. The MAC, HVL, and Zeff values for radiation shielding parameters were calculated in the energy range of 0.015–15 MeV using the FLUKA algorithm. In addition, EBF, EABF, and Σ(R) values were also determined for the prepared glasses. These values indicated that the parameters for shielding (MAC, HVL, Z(eff), EBF, EABF, and Σ(R)) are dependent upon the Samarium (III) oxide content. Furthermore, the addition of Samarium (III) oxide to the examined glass samples greatly reinforced their shielding capacity against gamma photon. The findings of the current study were compared to analyses of the XCOM software, some concretes, and lead. In the experiment, it was found that the SMG0.6 glass sample was the strongest shield.
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spelling pubmed-83064042021-07-25 Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods Issa, Shams A. M. Zakaly, Hesham M. H. Tekin, Huseyin O. Saudi, Heba A. Badawi, Ali Pyshkina, Mariia Susoy, Gulfem Elazaka, Ahmed I. Ene, Antoaneta Nanomaterials (Basel) Article (Tl(2)O(3))(30)-(Li(2)O)(10)-(B(2)O(3))((60−y)())-(Sm(2)O(3))(y) glass system with various Sm(2)O(3) additives (y = 0, 0.2, 0.4, 0.6) was studied in detail. The vibrational modes of the (Tl(2)O(3))(30)-(Li(2)O)(10)-(B(2)O(3))((60−y)) network were active at three composition-related IR spectral peaks that differed from those mixed with Samarium (III) oxide at high wavenumber ranges. These glass samples show that their permeability increased with the Samarium (III) oxide content increase. Additionally, the electronic transition between localized states was observed in the samples. The MAC, HVL, and Zeff values for radiation shielding parameters were calculated in the energy range of 0.015–15 MeV using the FLUKA algorithm. In addition, EBF, EABF, and Σ(R) values were also determined for the prepared glasses. These values indicated that the parameters for shielding (MAC, HVL, Z(eff), EBF, EABF, and Σ(R)) are dependent upon the Samarium (III) oxide content. Furthermore, the addition of Samarium (III) oxide to the examined glass samples greatly reinforced their shielding capacity against gamma photon. The findings of the current study were compared to analyses of the XCOM software, some concretes, and lead. In the experiment, it was found that the SMG0.6 glass sample was the strongest shield. MDPI 2021-06-29 /pmc/articles/PMC8306404/ /pubmed/34209698 http://dx.doi.org/10.3390/nano11071713 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Issa, Shams A. M.
Zakaly, Hesham M. H.
Tekin, Huseyin O.
Saudi, Heba A.
Badawi, Ali
Pyshkina, Mariia
Susoy, Gulfem
Elazaka, Ahmed I.
Ene, Antoaneta
Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
title Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
title_full Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
title_fullStr Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
title_full_unstemmed Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
title_short Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
title_sort exploring the ftir, optical and nuclear radiation shielding properties of samarium-borate glass: a characterization through experimental and simulation methods
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8306404/
https://www.ncbi.nlm.nih.gov/pubmed/34209698
http://dx.doi.org/10.3390/nano11071713
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