<p>The copper europium oxide <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(({\text{Eu}}_{2}{\text{CuO}}_{4})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msub> <mtext>Eu</mtext> <mn>2</mn> </msub> <msub> <mtext>CuO</mtext> <mn>4</mn> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> cuprate was synthesized by the solid-state reaction method and investigated in terms of its structural as well as linear and nonlinear optical properties. X-ray diffraction, combined with Rietveld refinement, Rietveld refinement confirmed that the XRD pattern corresponds to the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({\text{Eu}}_{2}{\text{CuO}}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Eu</mtext> <mn>2</mn> </msub> <msub> <mtext>CuO</mtext> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> phase. The lattice parameters for <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({\text{Eu}}_{2}{\text{CuO}}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Eu</mtext> <mn>2</mn> </msub> <msub> <mtext>CuO</mtext> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> were determined to be <i>a</i> = 3.902(2) Å and <i>c</i> = 11.905(6) Å, in accordance with reported data for T′-type cuprates, while revealing slight lattice distortions associated with oxygen stoichiometry. Raman spectroscopy further confirms the stabilization of T′-phase through the identification of the characteristic A<sub>1g</sub> and B<sub>1g</sub> vibrational modes. The direct optical bandgap was evaluated to be 1.55 ± 6.4 × 10<sup>–4</sup> eV, consistent with the 1.45–1.70 eV range reported for <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({\text{Eu}}_{2}{\text{CuO}}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Eu</mtext> <mn>2</mn> </msub> <msub> <mtext>CuO</mtext> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> and other <i>T</i>′-type cuprates, while showing enhanced absorption near the band edge. The refractive index (n), dielectric function (ε), as well as the real and imaginary parts of the optical conductivity (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({\upsigma }_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">σ</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({\upsigma }_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">σ</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>) were determined. Furthermore, optical dispersion was analyzed using the Wemple–DiDomenico model to extract oscillator parameters and to evaluate the third-order nonlinear optical susceptibility (χ<sup>3</sup>). The χ<sup>3</sup> value obtained, previously scarcely investigated, represents an original contribution of this work and highlights the good potential of Eu₂CuO₄ for advanced optoelectronic applications.</p>

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Synthesis and investigation of structural and linear/non-linear optical properties of T’-\({\mathbf{Eu}}_{2} {\mathbf{CuO}}_{4}\) cuprate

  • A. Elgharbi,
  • M. Sadik,
  • M. Lassri,
  • A. El Hachmi,
  • M. Oubla,
  • H. Lassri,
  • M. Abid,
  • Y. Arba

摘要

The copper europium oxide \(({\text{Eu}}_{2}{\text{CuO}}_{4})\) ( Eu 2 CuO 4 ) cuprate was synthesized by the solid-state reaction method and investigated in terms of its structural as well as linear and nonlinear optical properties. X-ray diffraction, combined with Rietveld refinement, Rietveld refinement confirmed that the XRD pattern corresponds to the \({\text{Eu}}_{2}{\text{CuO}}_{4}\) Eu 2 CuO 4 phase. The lattice parameters for \({\text{Eu}}_{2}{\text{CuO}}_{4}\) Eu 2 CuO 4 were determined to be a = 3.902(2) Å and c = 11.905(6) Å, in accordance with reported data for T′-type cuprates, while revealing slight lattice distortions associated with oxygen stoichiometry. Raman spectroscopy further confirms the stabilization of T′-phase through the identification of the characteristic A1g and B1g vibrational modes. The direct optical bandgap was evaluated to be 1.55 ± 6.4 × 10–4 eV, consistent with the 1.45–1.70 eV range reported for \({\text{Eu}}_{2}{\text{CuO}}_{4}\) Eu 2 CuO 4 and other T′-type cuprates, while showing enhanced absorption near the band edge. The refractive index (n), dielectric function (ε), as well as the real and imaginary parts of the optical conductivity ( \({\upsigma }_{1}\) σ 1 and \({\upsigma }_{2}\) σ 2 ) were determined. Furthermore, optical dispersion was analyzed using the Wemple–DiDomenico model to extract oscillator parameters and to evaluate the third-order nonlinear optical susceptibility (χ3). The χ3 value obtained, previously scarcely investigated, represents an original contribution of this work and highlights the good potential of Eu₂CuO₄ for advanced optoelectronic applications.