<p>We study a monostable reaction-diffusion equation of the form <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(u_t=du_{xx}+f(u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <mi>d</mi> <msub> <mi>u</mi> <mrow> <mi mathvariant="italic">xx</mi> </mrow> </msub> <mo>+</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> over a semi-infinite spatial domain <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\([g(t),\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, with <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(x=g(t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>=</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> the free boundary whose evolution is governed by equations derived from a “preferred population density” principle, which postulates that the species with population density <i>u</i>(<i>t</i>,&#xa0;<i>x</i>) and population range <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\([g(t),\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> maintains a certain density <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation> at the habitat edge <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(x=g(t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>=</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In the “high-density” regime, where <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation> exceeds the carrying capacity of the favourable environment represented by a monostable function <i>f</i>(<i>u</i>), it is known; see [6] for the case of a bounded population range [g(t), h(t)], that for large time, the front retreats as time advances. In this work, the unboundedness of the population range <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\([g(t),\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> allows us to prove that, as time <i>t</i> converges to infinity, the free boundary <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(x=g(t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>=</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> converges to <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>∞</mi> </math></EquationSource> </InlineEquation> with a constant asymptotic speed <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(c(\delta )&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo stretchy="false">(</mo> <mi>δ</mi> <mo stretchy="false">)</mo> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> determined by an associated semi-wave problem, and the population density <i>u</i>(<i>t</i>,&#xa0;<i>x</i>) has the property that <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(u(t,x+g(t))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mi>x</mi> <mo>+</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> converges uniformly to <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(q^*_{c(\delta )}(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>q</mi> <mrow> <mi>c</mi> <mo stretchy="false">(</mo> <mi>δ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∗</mo> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, the semi-wave profile function associated with the speed <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(c(\delta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo stretchy="false">(</mo> <mi>δ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. It turns out that in this retreating front situation considered here, some key techniques developed for advancing fronts in related free boundary models do not work anymore. This difficulty is overcome here by a “touching method", which uses a family of lower and upper solutions constructed from semi-waves of some carefully designed auxiliary problems to touch the solution <i>u</i>(<i>t</i>,&#xa0;<i>x</i>) at the retreating front <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(x=g(t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>=</mo> <mi>g</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, thereby generating a setting where the comparison principle can be used to obtain the desired estimates for <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(g'(t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>g</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <i>u</i>(<i>t</i>,&#xa0;<i>x</i>). We believe this method will find applications elsewhere.</p>

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Convergence to a receding wave in a monostable free boundary problem

  • Hongkai Cao,
  • Yihong Du,
  • Wenjie Ni

摘要

We study a monostable reaction-diffusion equation of the form \(u_t=du_{xx}+f(u)\) u t = d u xx + f ( u ) over a semi-infinite spatial domain \([g(t),\infty )\) [ g ( t ) , ) , with \(x=g(t)\) x = g ( t ) the free boundary whose evolution is governed by equations derived from a “preferred population density” principle, which postulates that the species with population density u(tx) and population range \([g(t),\infty )\) [ g ( t ) , ) maintains a certain density \(\delta \) δ at the habitat edge \(x=g(t)\) x = g ( t ) . In the “high-density” regime, where \(\delta \) δ exceeds the carrying capacity of the favourable environment represented by a monostable function f(u), it is known; see [6] for the case of a bounded population range [g(t), h(t)], that for large time, the front retreats as time advances. In this work, the unboundedness of the population range \([g(t),\infty )\) [ g ( t ) , ) allows us to prove that, as time t converges to infinity, the free boundary \(x=g(t)\) x = g ( t ) converges to \(\infty \) with a constant asymptotic speed \(c(\delta )>0\) c ( δ ) > 0 determined by an associated semi-wave problem, and the population density u(tx) has the property that \(u(t,x+g(t))\) u ( t , x + g ( t ) ) converges uniformly to \(q^*_{c(\delta )}(x)\) q c ( δ ) ( x ) , the semi-wave profile function associated with the speed \(c(\delta )\) c ( δ ) . It turns out that in this retreating front situation considered here, some key techniques developed for advancing fronts in related free boundary models do not work anymore. This difficulty is overcome here by a “touching method", which uses a family of lower and upper solutions constructed from semi-waves of some carefully designed auxiliary problems to touch the solution u(tx) at the retreating front \(x=g(t)\) x = g ( t ) , thereby generating a setting where the comparison principle can be used to obtain the desired estimates for \(g'(t)\) g ( t ) and u(tx). We believe this method will find applications elsewhere.