<p>We consider heat semigroups of the form <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\text{exp}(t(\Delta-\lambda\mathbf{1}_{\Omega_{0}}))\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mtext>exp</mtext> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">(</mo> <mi mathvariant="normal">Δ</mi> <mo>−</mo> <mi>λ</mi> <msub> <mrow> <mn mathvariant="bold">1</mn> </mrow> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </msub> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> on bounded domains. These singularly perturbed equations arise in certain models of diffusion limited chemical reactions. Using variants of Moser’s iteration scheme, we show sub-exponential decay in the strong coupling limit, i.e., as λ ↗ ∞, in compact subdomains of the “obstacle”, Ω<sub>0</sub>.</p>

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A note on Moser iteration and the large coupling limit

  • Ikemefuna Agbanusi

摘要

We consider heat semigroups of the form \(\text{exp}(t(\Delta-\lambda\mathbf{1}_{\Omega_{0}}))\) exp ( t ( Δ λ 1 Ω 0 ) ) on bounded domains. These singularly perturbed equations arise in certain models of diffusion limited chemical reactions. Using variants of Moser’s iteration scheme, we show sub-exponential decay in the strong coupling limit, i.e., as λ ↗ ∞, in compact subdomains of the “obstacle”, Ω0.