<p>A notable feature of the anomalous sub-solution equation is its solution’s algebraic decay over extended time periods, a phenomenon commonly associated with Mittag-Leffler type stability. For power-nonlinear sub-diffusion models with variable coefficients, we prove Mittag-Leffler stability under natural decay assumptions on the source functions, with decay rate <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="188" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert u(t)\Vert _{L^{s}(\Omega )}=O( t^{-(\alpha +\beta )/\gamma } )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mi>s</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>=</mo> <mi>O</mi> <mrow> <mo stretchy="false">(</mo> <msup> <mi>t</mi> <mrow> <mo>-</mo> <mo stretchy="false">(</mo> <mi>α</mi> <mo>+</mo> <mi>β</mi> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mi>γ</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq2.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> are positive constants, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="95" /> </InlineMediaObject> <EquationSource Format="TEX">\(\beta \in (-\alpha ,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mo>-</mo> <mi>α</mi> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\in (1,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. We then develop a structure-preserving algorithm for these models. For the complete monotonicity-preserving (<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{C}\mathcal{M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">C</mi> <mi mathvariant="script">M</mi> </mrow> </math></EquationSource> </InlineEquation>-preserving) schemes developed by Li and Wang (Commun. Math. Sci., 19(5):1301-1336, 2021), we show they satisfy the discrete comparison principle for time-fractional differential equations with variable coefficients. By carefully constructing the fine the discrete supersolutions and subsolutions, we obtain the numerical solution’s long-time optimal decay rate <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq8.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="177" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert u_{n}\Vert _{L^{s}(\Omega )}=O( t_n^{-(\alpha +\beta )/\gamma } )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>u</mi> <mi>n</mi> </msub> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mi>s</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>=</mo> <mi>O</mi> <mrow> <mo stretchy="false">(</mo> <msubsup> <mi>t</mi> <mi>n</mi> <mrow> <mo>-</mo> <mo stretchy="false">(</mo> <mi>α</mi> <mo>+</mo> <mi>β</mi> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mi>γ</mi> </mrow> </msubsup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10915_2025_2812_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(t_{n}\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>t</mi> <mi>n</mi> </msub> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, which aligns perfectly with the theoretical decay rate. Finally, we validate our analysis through numerical experiments.</p>

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Mittag-Leffler Stability of Complete Monotonicity-Preserving Schemes for Sub-Diffusion Equations with Time-Dependent Coefficients

  • Wen Dong,
  • Dongling Wang

摘要

A notable feature of the anomalous sub-solution equation is its solution’s algebraic decay over extended time periods, a phenomenon commonly associated with Mittag-Leffler type stability. For power-nonlinear sub-diffusion models with variable coefficients, we prove Mittag-Leffler stability under natural decay assumptions on the source functions, with decay rate \(\Vert u(t)\Vert _{L^{s}(\Omega )}=O( t^{-(\alpha +\beta )/\gamma } )\) u ( t ) L s ( Ω ) = O ( t - ( α + β ) / γ ) as \(t\rightarrow \infty \) t , where \(\alpha \) α , \(\gamma \) γ are positive constants, \(\beta \in (-\alpha ,\infty )\) β ( - α , ) and \(s\in (1,\infty )\) s ( 1 , ) . We then develop a structure-preserving algorithm for these models. For the complete monotonicity-preserving ( \(\mathcal{C}\mathcal{M}\) C M -preserving) schemes developed by Li and Wang (Commun. Math. Sci., 19(5):1301-1336, 2021), we show they satisfy the discrete comparison principle for time-fractional differential equations with variable coefficients. By carefully constructing the fine the discrete supersolutions and subsolutions, we obtain the numerical solution’s long-time optimal decay rate \(\Vert u_{n}\Vert _{L^{s}(\Omega )}=O( t_n^{-(\alpha +\beta )/\gamma } )\) u n L s ( Ω ) = O ( t n - ( α + β ) / γ ) as \(t_{n}\rightarrow \infty \) t n , which aligns perfectly with the theoretical decay rate. Finally, we validate our analysis through numerical experiments.