<p>We consider positive radial decreasing blow-up solutions of the semilinear heat equation <Equation ID="Equ131"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_Equ131.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="314" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} u_t-\Delta u=f(u):=e^{u}L(e^{u}),\quad x\in \Omega ,\ t&gt;0, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>=</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>:</mo> <mo>=</mo> <msup> <mi>e</mi> <mi>u</mi> </msup> <mi>L</mi> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mi>u</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="4pt" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega =\mathbb {R}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>=</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega =B_R\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>=</mo> <msub> <mi>B</mi> <mi>R</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> and <i>L</i> is a slowly varying function (which includes for instance logarithms and their powers and iterates, as well as some strongly oscillating unbounded functions). We characterize the asymptotic blow-up behavior and obtain the sharp, global blow-up profile in the scale of the original variables (<i>x</i>,&#xa0;<i>t</i>). Namely, assuming for instance <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_t\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, we have <Equation ID="Equ132"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_Equ132.gif" Format="GIF" Height="44" Rendition="HTML" Resolution="72" Type="Linedraw" Width="611" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} u(x,t)\!=\!G^{-1}\bigg (T\!-\!t\!+\!\frac{1}{8}\frac{|x|^2}{|\log |x||}\bigg )\!+\!o(1)\ \ \hbox { as } (x,t)\!\rightarrow \! (0,T),\quad \hbox { where } G(X)\!=\!\int _{X}^{\infty } \frac{ds}{f(s)}. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="-0.166667em" /> <mo>=</mo> <mspace width="-0.166667em" /> <msup> <mi>G</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">(</mo> </mrow> <mi>T</mi> <mspace width="-0.166667em" /> <mo>-</mo> <mspace width="-0.166667em" /> <mi>t</mi> <mspace width="-0.166667em" /> <mo>+</mo> <mspace width="-0.166667em" /> <mfrac> <mn>1</mn> <mn>8</mn> </mfrac> <mfrac> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mrow> <mo stretchy="false">|</mo> <mo>log</mo> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> <mo stretchy="false">|</mo> </mrow> </mfrac> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">)</mo> </mrow> <mspace width="-0.166667em" /> <mo>+</mo> <mspace width="-0.166667em" /> <mi>o</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="0.333333em" /> <mtext>as</mtext> <mspace width="0.333333em" /> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="-0.166667em" /> <mo stretchy="false">→</mo> <mspace width="-0.166667em" /> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>where</mtext> <mspace width="0.333333em" /> <mi>G</mi> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="-0.166667em" /> <mo>=</mo> <mspace width="-0.166667em" /> <msubsup> <mo>∫</mo> <mrow> <mi>X</mi> </mrow> <mi>∞</mi> </msubsup> <mfrac> <mrow> <mi mathvariant="italic">ds</mi> </mrow> <mrow> <mi>f</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> </mfrac> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>This estimate in particular provides the sharp final space profile and the refined space-time profile. For exponentially growing nonlinearities, such results were up to now available only in the scale invariant case <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="72" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(u)=e^u\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>e</mi> <mi>u</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>. Moreover, this displays a universal structure of the global blow-up profile, given by the resolvent <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(G^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>G</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> </InlineEquation> of the ODE composed with a fixed time-space building block, which is robust with respect to the factor <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10884_2025_10447_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(L(e^u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mi>u</mi> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Refined Blow-up Behavior for Reaction-Diffusion Equations with Non Scale Invariant Exponential Nonlinearities

  • Loth Damagui Chabi

摘要

We consider positive radial decreasing blow-up solutions of the semilinear heat equation \(\begin{aligned} u_t-\Delta u=f(u):=e^{u}L(e^{u}),\quad x\in \Omega ,\ t>0, \end{aligned}\) u t - Δ u = f ( u ) : = e u L ( e u ) , x Ω , t > 0 , where \(\Omega =\mathbb {R}^n\) Ω = R n or \(\Omega =B_R\) Ω = B R and L is a slowly varying function (which includes for instance logarithms and their powers and iterates, as well as some strongly oscillating unbounded functions). We characterize the asymptotic blow-up behavior and obtain the sharp, global blow-up profile in the scale of the original variables (xt). Namely, assuming for instance \(u_t\ge 0\) u t 0 , we have \(\begin{aligned} u(x,t)\!=\!G^{-1}\bigg (T\!-\!t\!+\!\frac{1}{8}\frac{|x|^2}{|\log |x||}\bigg )\!+\!o(1)\ \ \hbox { as } (x,t)\!\rightarrow \! (0,T),\quad \hbox { where } G(X)\!=\!\int _{X}^{\infty } \frac{ds}{f(s)}. \end{aligned}\) u ( x , t ) = G - 1 ( T - t + 1 8 | x | 2 | log | x | | ) + o ( 1 ) as ( x , t ) ( 0 , T ) , where G ( X ) = X ds f ( s ) . This estimate in particular provides the sharp final space profile and the refined space-time profile. For exponentially growing nonlinearities, such results were up to now available only in the scale invariant case \(f(u)=e^u\) f ( u ) = e u . Moreover, this displays a universal structure of the global blow-up profile, given by the resolvent \(G^{-1}\) G - 1 of the ODE composed with a fixed time-space building block, which is robust with respect to the factor \(L(e^u)\) L ( e u ) .