<p>Glasses with the configuration 72.5B<sub>2</sub>O<sub>3</sub>-7.5MoO<sub>3</sub>-(<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11897_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(20 - x\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>20</mn> <mo>-</mo> <mi>x</mi> </mrow> </math></EquationSource> </InlineEquation>) Li<sub>2</sub>O-<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11897_Article_IEq2.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>x</mi> </math></EquationSource> </InlineEquation> CdO: <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11897_Article_IEq2.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>x</mi> </math></EquationSource> </InlineEquation>(<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11897_Article_IEq4.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="81" /> </InlineMediaObject> <EquationSource Format="TEX">\(0 \le x \ge 16\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≤</mo> <mi>x</mi> <mo>≥</mo> <mn>16</mn> </mrow> </math></EquationSource> </InlineEquation>) mol.% were synthesized using the melt-quenching technique. The density increased from 2.61&#xa0;g&#xa0;cm<sup>−3</sup> to 3.79&#xa0;g&#xa0;cm<sup>−3</sup>, whereas the molar volume decreased from 27.79 to 21.9. The optical spectra of the BMLC glasses were measured. The optical bandgap increased from 2.12&#xa0;eV to 2.89&#xa0;eV. On the other hand, the Urbach energy decreased from 0.847&#xa0;eV to 0.49&#xa0;eV. It was found that the <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11897_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\( (Z_{{{\text{eff}}}} )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msub> <mi>Z</mi> <mtext>eff</mtext> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> values increased as the CdO content increased. Therefore, the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11897_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="62" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{BMLC}}_{16} \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>BMLC</mtext> <mn>16</mn> </msub> </math></EquationSource> </InlineEquation> sample demonstrated the highest effectiveness for γ shielding. The fast neutron removal cross section (FNRCS) value increased from 0.105 to 0.137, which confirmed that the BMLC glasses with high CdO exhibit excellent neutron and γ shielding. From the results obtained, our proposed glass showed good prospects for use in radiation-shielding applications.</p>

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Composition-Dependent Basic Physical Properties and Radiation Shielding Performance of B2O3-Li2O-MoO3-CdO Glasses

  • Dalal Abdullah Aloraini,
  • Ateyyah M. Al-Baradi,
  • K. Kreen

摘要

Glasses with the configuration 72.5B2O3-7.5MoO3-( \(20 - x\) 20 - x ) Li2O- \(x\) x CdO: \(x\) x ( \(0 \le x \ge 16\) 0 x 16 ) mol.% were synthesized using the melt-quenching technique. The density increased from 2.61 g cm−3 to 3.79 g cm−3, whereas the molar volume decreased from 27.79 to 21.9. The optical spectra of the BMLC glasses were measured. The optical bandgap increased from 2.12 eV to 2.89 eV. On the other hand, the Urbach energy decreased from 0.847 eV to 0.49 eV. It was found that the \( (Z_{{{\text{eff}}}} )\) ( Z eff ) values increased as the CdO content increased. Therefore, the \({\text{BMLC}}_{16} \) BMLC 16 sample demonstrated the highest effectiveness for γ shielding. The fast neutron removal cross section (FNRCS) value increased from 0.105 to 0.137, which confirmed that the BMLC glasses with high CdO exhibit excellent neutron and γ shielding. From the results obtained, our proposed glass showed good prospects for use in radiation-shielding applications.