Synthesis, Physical, Optical Characteristics and Ionizing Radiation Resistance of Newly Boro-Bariofluoride/Sodium/Calcium/Nickel Glasses: B2O3·BaF2·CaO·Na2O·NiO

A novel boro-bariofluoride/sodium/calcium/nickel glasses with chemical compositions (40-x)B 2 O 3 ·30BaF 2 ·15CaO·15Na 2 O·xNiO, where x = 0.0 (Ni0.0)–1.5 (Ni1.5) in steps of 0.3 mol% were prepared using the conventional melt quenching technique. Physical and optical features as well as ionizing rad...

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Veröffentlicht in:Journal of inorganic and organometallic polymers and materials 2022, Vol.32 (11), p.4260-4269
Hauptverfasser: Görke, Oliver, Shah, Asma Tufail, Kudrevatykh, N. V., Abouhaswa, A. S., Rammah, Y. S.
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container_issue 11
container_start_page 4260
container_title Journal of inorganic and organometallic polymers and materials
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creator Görke, Oliver
Shah, Asma Tufail
Kudrevatykh, N. V.
Abouhaswa, A. S.
Rammah, Y. S.
description A novel boro-bariofluoride/sodium/calcium/nickel glasses with chemical compositions (40-x)B 2 O 3 ·30BaF 2 ·15CaO·15Na 2 O·xNiO, where x = 0.0 (Ni0.0)–1.5 (Ni1.5) in steps of 0.3 mol% were prepared using the conventional melt quenching technique. Physical and optical features as well as ionizing radiation resistance capacities of the synthesized glass have been examined using various characterization techniques. Radiation shielding abilities have been examined via Phy-X/PSD software. Amorphous state of the Ni-glasses was confirmed by XRD data. Addition of NiO increased the density of glasses from 3.53 to 3.80 g/cm 3 . The direct optical band gap ( E Direct Optical ) was reduced from 3.58 to 3.33 eV, while the indirect ( E Indirect Optical ) one was reduced from 3.08 to 2.84 eV. Urbach’s edge (E U ) was enhanced from 0.4197 to 0.5009 eV as NiO content increased from 0.0 to 1.5 mol%. At a certain wavelength λ = 500 nm, the values of refractive index (n) increased from 1.84 to 2.56. In the photon energy range (0.15–15 MeV), the mass attenuation coefficient (MAC) results had the following trend: (MAC) Ni0.0   (HVL) Ni1.5 . The effective atomic number (Z eff ) of the prepared Ni-glasses has the same trend of MAC and LAC shielding parameters. The Ni-glasses can be applied in optical areas and considered as superior light glasses for radiation shielding applications.
doi_str_mv 10.1007/s10904-022-02444-4
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Urbach’s edge (E U ) was enhanced from 0.4197 to 0.5009 eV as NiO content increased from 0.0 to 1.5 mol%. At a certain wavelength λ = 500 nm, the values of refractive index (n) increased from 1.84 to 2.56. In the photon energy range (0.15–15 MeV), the mass attenuation coefficient (MAC) results had the following trend: (MAC) Ni0.0  &lt; (MAC) Ni0.3  &lt; (MAC) Ni0.6  &lt; (MAC) Ni0.9  &lt; (MAC) Ni1.2  &lt; (MAC) Ni1.5 . The linear attenuation coefficient (LAC) showed a similar trend of the MAC. In the same photon energy range, the half value layer (HVL) of Ni-glasses was reduced as NiO level increased, i.e. (HVL) Ni0.0  &gt; (HVL) Ni0.3  &gt; (HVL) Ni0.6  &gt; (HVL) Ni0.9  &gt; (HVL) Ni1.2  &gt; (HVL) Ni1.5 . The effective atomic number (Z eff ) of the prepared Ni-glasses has the same trend of MAC and LAC shielding parameters. 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Addition of NiO increased the density of glasses from 3.53 to 3.80 g/cm 3 . The direct optical band gap ( E Direct Optical ) was reduced from 3.58 to 3.33 eV, while the indirect ( E Indirect Optical ) one was reduced from 3.08 to 2.84 eV. Urbach’s edge (E U ) was enhanced from 0.4197 to 0.5009 eV as NiO content increased from 0.0 to 1.5 mol%. At a certain wavelength λ = 500 nm, the values of refractive index (n) increased from 1.84 to 2.56. In the photon energy range (0.15–15 MeV), the mass attenuation coefficient (MAC) results had the following trend: (MAC) Ni0.0  &lt; (MAC) Ni0.3  &lt; (MAC) Ni0.6  &lt; (MAC) Ni0.9  &lt; (MAC) Ni1.2  &lt; (MAC) Ni1.5 . The linear attenuation coefficient (LAC) showed a similar trend of the MAC. In the same photon energy range, the half value layer (HVL) of Ni-glasses was reduced as NiO level increased, i.e. (HVL) Ni0.0  &gt; (HVL) Ni0.3  &gt; (HVL) Ni0.6  &gt; (HVL) Ni0.9  &gt; (HVL) Ni1.2  &gt; (HVL) Ni1.5 . 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S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Synthesis, Physical, Optical Characteristics and Ionizing Radiation Resistance of Newly Boro-Bariofluoride/Sodium/Calcium/Nickel Glasses: B2O3·BaF2·CaO·Na2O·NiO</atitle><jtitle>Journal of inorganic and organometallic polymers and materials</jtitle><stitle>J Inorg Organomet Polym</stitle><date>2022</date><risdate>2022</risdate><volume>32</volume><issue>11</issue><spage>4260</spage><epage>4269</epage><pages>4260-4269</pages><issn>1574-1443</issn><eissn>1574-1451</eissn><abstract>A novel boro-bariofluoride/sodium/calcium/nickel glasses with chemical compositions (40-x)B 2 O 3 ·30BaF 2 ·15CaO·15Na 2 O·xNiO, where x = 0.0 (Ni0.0)–1.5 (Ni1.5) in steps of 0.3 mol% were prepared using the conventional melt quenching technique. Physical and optical features as well as ionizing radiation resistance capacities of the synthesized glass have been examined using various characterization techniques. Radiation shielding abilities have been examined via Phy-X/PSD software. Amorphous state of the Ni-glasses was confirmed by XRD data. Addition of NiO increased the density of glasses from 3.53 to 3.80 g/cm 3 . The direct optical band gap ( E Direct Optical ) was reduced from 3.58 to 3.33 eV, while the indirect ( E Indirect Optical ) one was reduced from 3.08 to 2.84 eV. Urbach’s edge (E U ) was enhanced from 0.4197 to 0.5009 eV as NiO content increased from 0.0 to 1.5 mol%. At a certain wavelength λ = 500 nm, the values of refractive index (n) increased from 1.84 to 2.56. In the photon energy range (0.15–15 MeV), the mass attenuation coefficient (MAC) results had the following trend: (MAC) Ni0.0  &lt; (MAC) Ni0.3  &lt; (MAC) Ni0.6  &lt; (MAC) Ni0.9  &lt; (MAC) Ni1.2  &lt; (MAC) Ni1.5 . The linear attenuation coefficient (LAC) showed a similar trend of the MAC. In the same photon energy range, the half value layer (HVL) of Ni-glasses was reduced as NiO level increased, i.e. (HVL) Ni0.0  &gt; (HVL) Ni0.3  &gt; (HVL) Ni0.6  &gt; (HVL) Ni0.9  &gt; (HVL) Ni1.2  &gt; (HVL) Ni1.5 . The effective atomic number (Z eff ) of the prepared Ni-glasses has the same trend of MAC and LAC shielding parameters. The Ni-glasses can be applied in optical areas and considered as superior light glasses for radiation shielding applications.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10904-022-02444-4</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0003-3106-5571</orcidid></addata></record>
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subjects Atomic properties
Attenuation coefficients
Barium fluorides
Boron oxides
Calcium
Chemical composition
Chemistry
Chemistry and Materials Science
Inorganic Chemistry
Ionizing radiation
Nickel oxides
Optical properties
Organic Chemistry
Photons
Polymer Sciences
Radiation
Radiation shielding
Radiation tolerance
Refractivity
Sodium
title Synthesis, Physical, Optical Characteristics and Ionizing Radiation Resistance of Newly Boro-Bariofluoride/Sodium/Calcium/Nickel Glasses: B2O3·BaF2·CaO·Na2O·NiO
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