<p>Nonlinear effects and other optical phenomena would become nontrivial at greater optical intensities. This article discusses the annealing effect on the linear and third-order nonlinear optical response of Physical Vapour Deposited (PVD), naturally oxidized Cu<sub>x</sub>O thin films that are thermally annealed under N<sub>2</sub> ambience at different temperatures. In particular, the nonlinear absorption (NLA)&#xa0;coefficient, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8385_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\beta\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> </InlineEquation>, nonlinear refractive (NLR)&#xa0;index, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8385_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(n_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>n</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> of naturally oxidized and thermally treated Cu<sub>x</sub>O thin film on a quartz glass substrate were determined using continuous-wave (CW) laser Z-scan techniques at 637&#xa0;nm wavelength. The optimal third-order nonlinear susceptibility, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8385_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\({\upchi }^{\left( 3 \right)}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="normal">χ</mi> </mrow> <mfenced close=")" open="("> <mn>3</mn> </mfenced> </msup> </math></EquationSource> </InlineEquation> of the prepared Cu<sub>x</sub>O thin film was measured to be 4.19 × 10⁻<sup>2</sup> esu at an annealing temperature of 450&#xa0;°C, corresponding to the lowest energy bandgap of 2.12&#xa0;eV. In addition, the exploration of crystal, structural, morphological, topological, and compositional characteristics ascertained the good quality growth of prepared Cu<sub>x</sub>O thin films. These findings&#xa0;unambiguously establish that the thermally treated absorption of prepared Cu<sub>x</sub>O thin films are pivotal for advancing integrated photonics platforms,&#xa0;particularly in nonlinear as well as quantum photonics applications.</p>

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Annealing-driven third-order optical nonlinear properties of naturally oxidized copper oxide thin films

  • Md Rumon Shahrier,
  • Sabah M. Mohammad,
  • Mundzir Abdullah,
  • Aijaz Ali Soomro,
  • Hameed Naser,
  • Abubakar A. Sifawa

摘要

Nonlinear effects and other optical phenomena would become nontrivial at greater optical intensities. This article discusses the annealing effect on the linear and third-order nonlinear optical response of Physical Vapour Deposited (PVD), naturally oxidized CuxO thin films that are thermally annealed under N2 ambience at different temperatures. In particular, the nonlinear absorption (NLA) coefficient, \(\beta\) β , nonlinear refractive (NLR) index, \(n_{2}\) n 2 of naturally oxidized and thermally treated CuxO thin film on a quartz glass substrate were determined using continuous-wave (CW) laser Z-scan techniques at 637 nm wavelength. The optimal third-order nonlinear susceptibility, \({\upchi }^{\left( 3 \right)}\) χ 3 of the prepared CuxO thin film was measured to be 4.19 × 10⁻2 esu at an annealing temperature of 450 °C, corresponding to the lowest energy bandgap of 2.12 eV. In addition, the exploration of crystal, structural, morphological, topological, and compositional characteristics ascertained the good quality growth of prepared CuxO thin films. These findings unambiguously establish that the thermally treated absorption of prepared CuxO thin films are pivotal for advancing integrated photonics platforms, particularly in nonlinear as well as quantum photonics applications.