<p>Dy<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> single- and Dy<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>/Tb<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> double-doped LiAlB and BaB glasses are investigated for their external quantum efficiency under 452-nm excitation. In the case of double-doping, the energy transfer from Dy<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> to Tb<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> results in a combination of both Dy<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>- and Tb<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-related emissions though Tb<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> cannot be excited directly at 452 nm. The energy transfer efficiency is obtained by deconvolution of the photoluminescence spectrum into the corresponding Dy<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> and Tb<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> components. There is, however, also an energy transfer from Tb<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> to Dy<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> which is confirmed by lifetime measurements.</p> Graphical abstract <p></p>

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Energy transfer in Dy/Tb double-doped borate glass for blue-to-green conversion

  • Michelle Grüne,
  • Jan Kückelheim,
  • Henning Lichtenberg,
  • Bernd Ahrens,
  • Stefan Schweizer

摘要

Dy \(^{3+}\) 3 + single- and Dy \(^{3+}\) 3 + /Tb \(^{3+}\) 3 + double-doped LiAlB and BaB glasses are investigated for their external quantum efficiency under 452-nm excitation. In the case of double-doping, the energy transfer from Dy \(^{3+}\) 3 + to Tb \(^{3+}\) 3 + results in a combination of both Dy \(^{3+}\) 3 + - and Tb \(^{3+}\) 3 + -related emissions though Tb \(^{3+}\) 3 + cannot be excited directly at 452 nm. The energy transfer efficiency is obtained by deconvolution of the photoluminescence spectrum into the corresponding Dy \(^{3+}\) 3 + and Tb \(^{3+}\) 3 + components. There is, however, also an energy transfer from Tb \(^{3+}\) 3 + to Dy \(^{3+}\) 3 + which is confirmed by lifetime measurements.

Graphical abstract