<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(G=(V,E)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo>=</mo> <mo stretchy="false">(</mo> <mi>V</mi> <mo>,</mo> <mi>E</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> be a locally finite connected graph. We develop the first eigenvalue method on <i>G</i> introduced in 1963 by Kaplan [<CitationRef CitationID="CR22">22</CitationRef>] on Euclidean space, the discrete Phragmén-Lindelöf principle of parabolic equations and upper and lower solutions method on <i>G</i>. Using these methods, we establish the estimates and asymptotic behaviour of the life span of solutions to a semilinear heat equation with initial data <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\lambda \psi (x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mi>ψ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for different scales of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> on <i>G</i> under some different conditions. Our results are different from the continuous case, which is related to the structure of the graph <i>G</i>.</p>

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The life span of solution of a semilinear parabolic equation on locally finite graphs

  • Yuanyang Hu,
  • Mingxin Wang

摘要

Let \(G=(V,E)\) G = ( V , E ) be a locally finite connected graph. We develop the first eigenvalue method on G introduced in 1963 by Kaplan [22] on Euclidean space, the discrete Phragmén-Lindelöf principle of parabolic equations and upper and lower solutions method on G. Using these methods, we establish the estimates and asymptotic behaviour of the life span of solutions to a semilinear heat equation with initial data \(\lambda \psi (x)\) λ ψ ( x ) for different scales of \(\lambda \) λ on G under some different conditions. Our results are different from the continuous case, which is related to the structure of the graph G.