<p>Compact and cost-effective pulsed yellow lasers have a growing demand for important medical applications including eye treatment, dermatology, and novel biomedical imaging. However, the efficient pulsed yellow light generation from a compact laser structure has historically been quite challenging. Recently, a dysprosium (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {Dy}^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>Dy</mtext> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>)-doped fiber laser has emerged as a promising candidate to produce yellow light directly and efficiently, paving the way for a simple and compact source. To date, major attention has been paid to the design of continuous wave (CW) <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {Dy}^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>Dy</mtext> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>-doped yellow fiber lasers. Here, we report, to the best of our knowledge, the first numerical investigation on the pulse-generating potential of a <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {Dy}^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>Dy</mtext> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>-doped fiber laser using a convenient gain-switching technique. With a particular emphasis on future experimental demonstrations, we consider the parameters of a commercially available <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {Dy}^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>Dy</mtext> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>-doped ZBLAN fiber and utilize a 450&#xa0;nm pumping wavelength, which can be accessed from commercial laser diodes. In our investigation, we use a feasible peak pump power of 4&#xa0;W and simulate a peak yellow output power of 11&#xa0;W with a minimum pulse width (full width at half maximum) of 0.8&#xa0;<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq5.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\upmu\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">μ</mi> </math></EquationSource> </InlineEquation>s at a pulse repetition rate of 25&#xa0;kHz. In a <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hbox {Dy}^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>Dy</mtext> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>-doped ZBLAN fiber, the lower level (<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(^6\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>6</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>H<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{13/2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn>13</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>) of the yellow lasing transition has a comparable lifetime (650&#xa0;<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq9.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\upmu\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">μ</mi> </math></EquationSource> </InlineEquation>s) to that of the upper laser level (<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(^4\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>4</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>F<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1303_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(_{9/2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow> <mn>9</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>). Therefore, we also analyze the impact of the lower laser level lifetime on the gain-switching laser performance and discuss the further developmental potential.</p>

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Numerical modeling of gain-switched dysprosium-doped yellow fiber lasers

  • Iffat Ara Talin,
  • Md. Ziaul Amin,
  • Md. Abdus Samad

摘要

Compact and cost-effective pulsed yellow lasers have a growing demand for important medical applications including eye treatment, dermatology, and novel biomedical imaging. However, the efficient pulsed yellow light generation from a compact laser structure has historically been quite challenging. Recently, a dysprosium ( \(\hbox {Dy}^{3+}\) Dy 3 + )-doped fiber laser has emerged as a promising candidate to produce yellow light directly and efficiently, paving the way for a simple and compact source. To date, major attention has been paid to the design of continuous wave (CW) \(\hbox {Dy}^{3+}\) Dy 3 + -doped yellow fiber lasers. Here, we report, to the best of our knowledge, the first numerical investigation on the pulse-generating potential of a \(\hbox {Dy}^{3+}\) Dy 3 + -doped fiber laser using a convenient gain-switching technique. With a particular emphasis on future experimental demonstrations, we consider the parameters of a commercially available \(\hbox {Dy}^{3+}\) Dy 3 + -doped ZBLAN fiber and utilize a 450 nm pumping wavelength, which can be accessed from commercial laser diodes. In our investigation, we use a feasible peak pump power of 4 W and simulate a peak yellow output power of 11 W with a minimum pulse width (full width at half maximum) of 0.8  \(\upmu\) μ s at a pulse repetition rate of 25 kHz. In a \(\hbox {Dy}^{3+}\) Dy 3 + -doped ZBLAN fiber, the lower level ( \(^6\) 6 H \(_{13/2}\) 13 / 2 ) of the yellow lasing transition has a comparable lifetime (650  \(\upmu\) μ s) to that of the upper laser level ( \(^4\) 4 F \(_{9/2}\) 9 / 2 ). Therefore, we also analyze the impact of the lower laser level lifetime on the gain-switching laser performance and discuss the further developmental potential.