<p>Lithium borate glass and dysprosium (Dy<sup>3+</sup>) ions are tissue-equivalent materials for radiation dosimetry due to their effective atomic numbers, which closely resemble those of human tissue and light emission properties of Dy<sup>3+</sup> ions. Lithium borate glasses with compositions <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1347_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="165" /> </InlineMediaObject> <EquationSource Format="TEX">\((50-x{)Li}_{2}O: 50{B}_{2}{O}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mn>50</mn> <mo>-</mo> <mi>x</mi> <msub> <mrow> <mo stretchy="false">)</mo> <mi>L</mi> <mi>i</mi> </mrow> <mn>2</mn> </msub> <mi>O</mi> <mo>:</mo> <mn>50</mn> <msub> <mi>B</mi> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>: <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1347_Article_IEq2.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(x{Dy}_{2}{O}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <msub> <mrow> <mi mathvariant="italic">Dy</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> (where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1347_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(x=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 0.1, 0.2, 0.5, 0.7, and 1&#xa0;mol %), labeled as LBD1, and (<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1347_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="216" /> </InlineMediaObject> <EquationSource Format="TEX">\(100-y) {B}_{2}{O}_{3 }:(y-0.5){Li}_{2}O\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mn>100</mn> <mo>-</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mi>B</mi> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>:</mo> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo>-</mo> <mn>0.5</mn> <mo stretchy="false">)</mo> </mrow> <msub> <mrow> <mi mathvariant="italic">Li</mi> </mrow> <mn>2</mn> </msub> <mi>O</mi> </mrow> </math></EquationSource> </InlineEquation>:0.5 <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1347_Article_IEq5.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\({Dy}_{2}{O}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Dy</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> (where <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1347_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="29" /> </InlineMediaObject> <EquationSource Format="TEX">\(y=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>y</mi> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 30, 40, 45, 50, 55&#xa0;mol %), labeled as LBD2, were fabricated using the melt-quench method. The properties analyzed include structural, X-ray and proton-induced luminescence, optical, photoluminescence (PL), and thermoluminescence (TL). XRD spectra confirmed amorphous structure with broad humps and no sharp peaks. X-ray luminescence shows two highest peaks at 575&#xa0;nm and 484&#xa0;nm due to the <sup>4</sup>F<sub>9/2</sub> →<sup>6</sup>H<sub>13/2</sub> and <sup>4</sup>F<sub>9/2</sub> → <sup>6</sup>H<sub>15/2</sub> transition, respectively. PL excitation spectra show seven peaks from Dy<sup>3+</sup> due to 4f–4f transitions, with emission spectra at 484&#xa0;nm (blue) and 575&#xa0;nm (yellow). LBD1 glass, doped with 0.5&#xa0;mol% Dy<sub>2</sub>O<sub>3</sub>, exhibits highest intensity in both X-ray luminescence and PL measurements. The proton-induced spectrum exhibits peak around 450–500&#xa0;nm and 550–600&#xa0;nm. The PL intensity increases under 349&#xa0;nm laser excitation. Optical band-gap energies decrease with increasing concentrations of Dy<sup>3+</sup> ions. After X-ray irradiation, the samples exhibit high-intensity TL peaks around 137–187&#xa0;°C measured from 10&#xa0;min to 48&#xa0;h post-irradiation. These findings emphasize the distinctive features of dysprosium-doped lithium borate glasses, making them valuable for various purposes, particularly in photonics, laser, radiation detection, and dosimetry.</p>

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Dysprosium-doped lithium borate glass for dosimetry applications

  • Anastazia Tarimo Felix,
  • Nguyen Duc Ton,
  • Jaeyoung Cho,
  • Nguyen Thanh Luan,
  • D. Joseph Daniel,
  • Faizan Anjum,
  • Syed Azaz Ali,
  • Hong Joo Kim

摘要

Lithium borate glass and dysprosium (Dy3+) ions are tissue-equivalent materials for radiation dosimetry due to their effective atomic numbers, which closely resemble those of human tissue and light emission properties of Dy3+ ions. Lithium borate glasses with compositions \((50-x{)Li}_{2}O: 50{B}_{2}{O}_{3}\) ( 50 - x ) L i 2 O : 50 B 2 O 3 : \(x{Dy}_{2}{O}_{3}\) x Dy 2 O 3 (where \(x=\) x = 0.1, 0.2, 0.5, 0.7, and 1 mol %), labeled as LBD1, and ( \(100-y) {B}_{2}{O}_{3 }:(y-0.5){Li}_{2}O\) 100 - y ) B 2 O 3 : ( y - 0.5 ) Li 2 O :0.5 \({Dy}_{2}{O}_{3}\) Dy 2 O 3 (where \(y=\) y = 30, 40, 45, 50, 55 mol %), labeled as LBD2, were fabricated using the melt-quench method. The properties analyzed include structural, X-ray and proton-induced luminescence, optical, photoluminescence (PL), and thermoluminescence (TL). XRD spectra confirmed amorphous structure with broad humps and no sharp peaks. X-ray luminescence shows two highest peaks at 575 nm and 484 nm due to the 4F9/26H13/2 and 4F9/2 → 6H15/2 transition, respectively. PL excitation spectra show seven peaks from Dy3+ due to 4f–4f transitions, with emission spectra at 484 nm (blue) and 575 nm (yellow). LBD1 glass, doped with 0.5 mol% Dy2O3, exhibits highest intensity in both X-ray luminescence and PL measurements. The proton-induced spectrum exhibits peak around 450–500 nm and 550–600 nm. The PL intensity increases under 349 nm laser excitation. Optical band-gap energies decrease with increasing concentrations of Dy3+ ions. After X-ray irradiation, the samples exhibit high-intensity TL peaks around 137–187 °C measured from 10 min to 48 h post-irradiation. These findings emphasize the distinctive features of dysprosium-doped lithium borate glasses, making them valuable for various purposes, particularly in photonics, laser, radiation detection, and dosimetry.