<p>A relation between the vibrational nonlinear refractive index coefficient <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4122_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\({{n}_{2}}(\omega )\)</EquationSource> <!--JETPLet2460430Guselnikov-m1--> </InlineEquation> and the vibrational cubic susceptibility <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4122_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="129" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\chi }^{{(3)}}}(\omega ';\omega ',\omega , - \omega )\)</EquationSource> <!--JETPLet2460430Guselnikov-m2--> </InlineEquation> has been analytically derived involving well-known optical, spectral, and thermal matter parameters. This relation allows one to estimate the nonlinear phase shift of low-power probe radiation at the frequency <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4122_Article_IEq3.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega '\)</EquationSource> <!--JETPLet2460430Guselnikov-m3--> </InlineEquation>, which propagates in the field of a high-power terahertz pump wave at the frequency <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4122_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega \)</EquationSource> <!--JETPLet2460430Guselnikov-m4--> </InlineEquation>. Theoretical estimates of the nonlinear susceptibility <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4122_Article_IEq5.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="129" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\chi }^{{(3)}}}(\omega ';\omega ',\omega , - \omega )\)</EquationSource> <!--JETPLet2460430Guselnikov-m5--> </InlineEquation> for water and fused silica for terahertz Kerr effect measurements have been obtained in good agreement with experimental data.</p>

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Features of the Nonlinear Vibrational Response of Dielectric Media at Two-Wave Mixing

  • M. S. Guselnikov

摘要

A relation between the vibrational nonlinear refractive index coefficient \({{n}_{2}}(\omega )\) and the vibrational cubic susceptibility \({{\chi }^{{(3)}}}(\omega ';\omega ',\omega , - \omega )\) has been analytically derived involving well-known optical, spectral, and thermal matter parameters. This relation allows one to estimate the nonlinear phase shift of low-power probe radiation at the frequency \(\omega '\) , which propagates in the field of a high-power terahertz pump wave at the frequency \(\omega \) . Theoretical estimates of the nonlinear susceptibility \({{\chi }^{{(3)}}}(\omega ';\omega ',\omega , - \omega )\) for water and fused silica for terahertz Kerr effect measurements have been obtained in good agreement with experimental data.