<p>A nearly linear decrease in the spectral vision of the UV absorption edge of the gradient <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq1.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="161" /> </InlineMediaObject> <EquationSource Format="TEX">\(LiNbO_3:Er^{3+}:Yb^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mi>i</mi> <mi>N</mi> <mi>b</mi> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>:</mo> <mi>E</mi> <msup> <mi>r</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> <mo>:</mo> <mi>Y</mi> <msup> <mi>b</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> crystal along the ferroelectric axis was detected. The second-order IR absorption spectra of the gradient <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq1.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="161" /> </InlineMediaObject> <EquationSource Format="TEX">\(LiNbO_3:Er^{3+}:Yb^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mi>i</mi> <mi>N</mi> <mi>b</mi> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>:</mo> <mi>E</mi> <msup> <mi>r</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> <mo>:</mo> <mi>Y</mi> <msup> <mi>b</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> crystal in the wavenumber range of 2000–3000 cm<sup>−1</sup> have been recorded for the first time. The appearance of absorption lines in the specified spectral range is typical of defective and highly anharmonic crystals. Based on the IR absorption spectra in the region of stretching vibrations of the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(OH^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <msup> <mi>H</mi> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>-groups, it has been found that the oxygen-octahedral clusters <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(MeO_6\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mi>e</mi> <msub> <mi>O</mi> <mn>6</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> (Me–<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(Li^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <msup> <mi>i</mi> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(Nb^{5+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <msup> <mi>b</mi> <mrow> <mn>5</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>, vacant octahedron V, impurity ions <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(Er^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>E</mi> <msup> <mi>r</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">\(Yb^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>Y</mi> <msup> <mi>b</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>) of the structure of the gradient <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq1.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="161" /> </InlineMediaObject> <EquationSource Format="TEX">\(LiNbO_3:Er^{3+}:Yb^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mi>i</mi> <mi>N</mi> <mi>b</mi> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>:</mo> <mi>E</mi> <msup> <mi>r</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> <mo>:</mo> <mi>Y</mi> <msup> <mi>b</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> crystal are practically not distorted. It has been shown that the volume concentration of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(OH^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <msup> <mi>H</mi> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>-groups in the gradient <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11082_2025_8392_Article_IEq1.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="161" /> </InlineMediaObject> <EquationSource Format="TEX">\(LiNbO_3:Er^{3+}:Yb^{3+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mi>i</mi> <mi>N</mi> <mi>b</mi> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>:</mo> <mi>E</mi> <msup> <mi>r</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> <mo>:</mo> <mi>Y</mi> <msup> <mi>b</mi> <mrow> <mn>3</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> crystal is several times less than in compositionally uniform congruent and stoichiometric lithium niobate crystals. The obtained results are significant for the complex analysis of the nonlinear materials.</p>

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Studies of the defect structure of the active-nonlinear gradient \(LiNbO_3:Er^{3+}:Yb^{3+}\) crystal by UV and IR absorption spectra

  • N. V. Sidorov,
  • A. Yu. Pyatyshev,
  • E. V. Stroganova,
  • V. V. Galutskiy,
  • O. A. Klimenko,
  • A. V. Skrabatun

摘要

A nearly linear decrease in the spectral vision of the UV absorption edge of the gradient \(LiNbO_3:Er^{3+}:Yb^{3+}\) L i N b O 3 : E r 3 + : Y b 3 + crystal along the ferroelectric axis was detected. The second-order IR absorption spectra of the gradient \(LiNbO_3:Er^{3+}:Yb^{3+}\) L i N b O 3 : E r 3 + : Y b 3 + crystal in the wavenumber range of 2000–3000 cm−1 have been recorded for the first time. The appearance of absorption lines in the specified spectral range is typical of defective and highly anharmonic crystals. Based on the IR absorption spectra in the region of stretching vibrations of the \(OH^-\) O H - -groups, it has been found that the oxygen-octahedral clusters \(MeO_6\) M e O 6 (Me– \(Li^+\) L i + , \(Nb^{5+}\) N b 5 + , vacant octahedron V, impurity ions \(Er^{3+}\) E r 3 + and \(Yb^{3+}\) Y b 3 + ) of the structure of the gradient \(LiNbO_3:Er^{3+}:Yb^{3+}\) L i N b O 3 : E r 3 + : Y b 3 + crystal are practically not distorted. It has been shown that the volume concentration of \(OH^-\) O H - -groups in the gradient \(LiNbO_3:Er^{3+}:Yb^{3+}\) L i N b O 3 : E r 3 + : Y b 3 + crystal is several times less than in compositionally uniform congruent and stoichiometric lithium niobate crystals. The obtained results are significant for the complex analysis of the nonlinear materials.