<p>We investigate quantitative estimates in homogenization of the locally periodic parabolic operator with multiscales <Equation ID="Equ141"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2962_Article_Equ141.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="327" /> </MediaObject> <EquationSource Format="TEX">\( {\partial _t} - \mathrm{{div}}\left( {A\left( {x,t,x/\varepsilon ,t/{\kappa ^2}} \right) \nabla } \right) ,\;\varepsilon&gt; 0,{\hspace{0.55542pt}} \kappa &gt; 0. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mo>-</mo> <mi mathvariant="normal">div</mi> <mfenced close=")" open="("> <mrow> <mi>A</mi> <mfenced close=")" open="("> <mrow> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <mi>x</mi> <mo stretchy="false">/</mo> <mi>ε</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">/</mo> <msup> <mi>κ</mi> <mn>2</mn> </msup> </mrow> </mfenced> <mi mathvariant="normal">∇</mi> </mrow> </mfenced> <mo>,</mo> <mspace width="0.277778em" /> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mspace width="0.55542pt" /> <mi>κ</mi> <mo>&gt;</mo> <mn>0</mn> <mo>.</mo> </mrow> </math></EquationSource> </Equation>Under proper assumptions, we establish the full-scale interior and boundary Lipschitz estimates. These results are new even for the case <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2962_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa =\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>κ</mi> <mo>=</mo> <mi>ε</mi> </mrow> </math></EquationSource> </InlineEquation>, and for the periodic operators <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2962_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="300" /> </InlineMediaObject> <EquationSource Format="TEX">\( {\partial _t} - \mathrm{{div}}\left( {A\left( {x/\varepsilon ,t/{\varepsilon ^\ell }} \right) \nabla } \right) ,\;0&lt; \varepsilon ,\ell &lt; \infty , \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mo>-</mo> <mi mathvariant="normal">div</mi> <mfenced close=")" open="("> <mrow> <mi>A</mi> <mfenced close=")" open="("> <mrow> <mi>x</mi> <mo stretchy="false">/</mo> <mi>ε</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">/</mo> <msup> <mi>ε</mi> <mi>ℓ</mi> </msup> </mrow> </mfenced> <mi mathvariant="normal">∇</mi> </mrow> </mfenced> <mo>,</mo> <mspace width="0.277778em" /> <mn>0</mn> <mo>&lt;</mo> <mi>ε</mi> <mo>,</mo> <mi>ℓ</mi> <mo>&lt;</mo> <mi>∞</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> of which the large-scale Lipschitz estimate down to <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2962_Article_IEq3.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon +\varepsilon ^{\ell /2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>+</mo> <msup> <mi>ε</mi> <mrow> <mi>ℓ</mi> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> was recently established by the Geng and Shen (Arch Ration Mech Anal 236:145–188, 2020). Due to the non-self-similar structure, the full-scale estimates do not follow directly from the large-scale estimates and the blow-up argument. As a byproduct, we also derive the convergence rates for the corresponding initial-Dirichlet problems, which extend the results in the aforementioned literature to more general settings.</p>

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Homogenization of locally periodic parabolic operators with non-self-similar scales

  • Jun Geng,
  • Weisheng Niu

摘要

We investigate quantitative estimates in homogenization of the locally periodic parabolic operator with multiscales \( {\partial _t} - \mathrm{{div}}\left( {A\left( {x,t,x/\varepsilon ,t/{\kappa ^2}} \right) \nabla } \right) ,\;\varepsilon> 0,{\hspace{0.55542pt}} \kappa > 0. \) t - div A x , t , x / ε , t / κ 2 , ε > 0 , κ > 0 . Under proper assumptions, we establish the full-scale interior and boundary Lipschitz estimates. These results are new even for the case \(\kappa =\varepsilon \) κ = ε , and for the periodic operators \( {\partial _t} - \mathrm{{div}}\left( {A\left( {x/\varepsilon ,t/{\varepsilon ^\ell }} \right) \nabla } \right) ,\;0< \varepsilon ,\ell < \infty , \) t - div A x / ε , t / ε , 0 < ε , < , of which the large-scale Lipschitz estimate down to \(\varepsilon +\varepsilon ^{\ell /2}\) ε + ε / 2 was recently established by the Geng and Shen (Arch Ration Mech Anal 236:145–188, 2020). Due to the non-self-similar structure, the full-scale estimates do not follow directly from the large-scale estimates and the blow-up argument. As a byproduct, we also derive the convergence rates for the corresponding initial-Dirichlet problems, which extend the results in the aforementioned literature to more general settings.