<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="223" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_{\varepsilon } = \textbf{D}^* g(\varvec{x}/\varepsilon ) \textbf{D} + \varepsilon ^{-2} p({\varvec{x}}/\varepsilon ),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>A</mi> <mi>ε</mi> </msub> <mo>=</mo> <msup> <mi mathvariant="bold">D</mi> <mo>∗</mo> </msup> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="bold-italic">x</mi> </mrow> <mo stretchy="false">/</mo> <mi>ε</mi> <mo stretchy="false">)</mo> </mrow> <mi mathvariant="bold">D</mi> <mo>+</mo> <msup> <mi>ε</mi> <mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>p</mi> <mrow> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="bold-italic">x</mi> </mrow> <mo stretchy="false">/</mo> <mi>ε</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq2.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, be a second-order elliptic differential operator in <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_2(\mathbb {R}^d)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>L</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with periodic coefficients. For small <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation>, the behavior of the semigroup <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{- A_{\varepsilon } t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mo>-</mo> <msub> <mi>A</mi> <mi>ε</mi> </msub> <mi>t</mi> </mrow> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq6.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(t&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, cut by the spectral projection of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation> into the interval <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="92" /> </InlineMediaObject> <EquationSource Format="TEX">\([\varepsilon ^{-2} \lambda _{+},+\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <msup> <mi>ε</mi> <mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> <msub> <mi>λ</mi> <mo>+</mo> </msub> <mo>,</mo> <mo>+</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is studied. Here, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon ^{-2} \lambda _{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ε</mi> <mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> <msub> <mi>λ</mi> <mo>+</mo> </msub> </mrow> </math></EquationSource> </InlineEquation> is the right edge of the spectral gap for <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation>. An approximation for the “cut semigroup” in the operator norm on <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_2(\mathbb {R}^d)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>L</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with error <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="TEX">\(O(\varepsilon )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <mo stretchy="false">(</mo> <mi>ε</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is obtained together with a more accurate approximation with corrector taken into account with error <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq13.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(O(\varepsilon ^2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <mo stretchy="false">(</mo> <msup> <mi>ε</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> (after singling out the factor <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq14.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{-t \lambda _{+} / \varepsilon ^2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <msub> <mi>λ</mi> <mo>+</mo> </msub> <mo stretchy="false">/</mo> <msup> <mi>ε</mi> <mn>2</mn> </msup> </mrow> </msup> </math></EquationSource> </InlineEquation>). The results are applied to homogenization of the Cauchy problem <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq15.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="98" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial _t v_\varepsilon = - A_\varepsilon v_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <msub> <mi>v</mi> <mi>ε</mi> </msub> <mo>=</mo> <mo>-</mo> <msub> <mi>A</mi> <mi>ε</mi> </msub> <msub> <mi>v</mi> <mi>ε</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq16.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(v_\varepsilon \vert _{t=0} = f_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>v</mi> <mi>ε</mi> </msub> <msub> <mrow> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>t</mi> <mo>=</mo> <mn>0</mn> </mrow> </msub> <mo>=</mo> <msub> <mi>f</mi> <mi>ε</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, with initial data <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7998_Article_IEq17.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(f_\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>f</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation> from a special class. Bibliography: 24 titles.</p>

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HOMOGENIZATION OF MULTIDIMENSIONAL PARABOLIC EQUATIONS WITH PERIODIC COEFFICIENTS AT THE EDGE OF INNER GAP

  • A. A. Mishulovich

摘要

Let \(A_{\varepsilon } = \textbf{D}^* g(\varvec{x}/\varepsilon ) \textbf{D} + \varepsilon ^{-2} p({\varvec{x}}/\varepsilon ),\) A ε = D g ( x / ε ) D + ε - 2 p ( x / ε ) , \(\varepsilon >0\) ε > 0 , be a second-order elliptic differential operator in \(L_2(\mathbb {R}^d)\) L 2 ( R d ) with periodic coefficients. For small \(\varepsilon \) ε , the behavior of the semigroup \(e^{- A_{\varepsilon } t}\) e - A ε t , \(t>0\) t > 0 , cut by the spectral projection of \(A_{\varepsilon }\) A ε into the interval \([\varepsilon ^{-2} \lambda _{+},+\infty )\) [ ε - 2 λ + , + ) is studied. Here, \(\varepsilon ^{-2} \lambda _{+}\) ε - 2 λ + is the right edge of the spectral gap for \(A_{\varepsilon }\) A ε . An approximation for the “cut semigroup” in the operator norm on \(L_2(\mathbb {R}^d)\) L 2 ( R d ) with error \(O(\varepsilon )\) O ( ε ) is obtained together with a more accurate approximation with corrector taken into account with error \(O(\varepsilon ^2)\) O ( ε 2 ) (after singling out the factor \(e^{-t \lambda _{+} / \varepsilon ^2}\) e - t λ + / ε 2 ). The results are applied to homogenization of the Cauchy problem \(\partial _t v_\varepsilon = - A_\varepsilon v_\varepsilon \) t v ε = - A ε v ε , \(v_\varepsilon \vert _{t=0} = f_\varepsilon \) v ε | t = 0 = f ε , with initial data \(f_\varepsilon \) f ε from a special class. Bibliography: 24 titles.