Abstract <p>In this work we focus on two-species reaction-diffusion system involving two reaction processes <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="115" /> </InlineMediaObject> <EquationSource Format="TEX">\(A + A \to (\emptyset ,A)\)</EquationSource> <!--PhysPNLt2570008Hnatic-m1--> </InlineEquation>, and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq2.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="90" /> </InlineMediaObject> <EquationSource Format="TEX">\(A + B \to A\)</EquationSource> <!--PhysPNLt2570008Hnatic-m2--> </InlineEquation>. Reactants are subject to diffusive spreading with arbitrary diffusion constants. Such a system was studied earlier at and below its upper critical dimension <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\({{d}_{{\text{c}}}} = 2\)</EquationSource> <!--PhysPNLt2570008Hnatic-m3--> </InlineEquation> in [2, 3], and recently also in the presence of long-range spreading with fractional Laplace operator <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq4.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="90" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\partial }^{\sigma }} \equiv {{\partial }^{{2(1 - \alpha )}}}\)</EquationSource> <!--PhysPNLt2570008Hnatic-m4--> </InlineEquation> [5–7]. In the latter case, however, only long-range limit was explored (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \gg \epsilon \)</EquationSource> <!--PhysPNLt2570008Hnatic-m5--> </InlineEquation>), where <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="137" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon = {{d}_{{\text{c}}}} - d = 2 - d\)</EquationSource> <!--PhysPNLt2570008Hnatic-m6--> </InlineEquation>. Here, our aim is to investigate the hybrid regime in which parameters α and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <!--PhysPNLt2570008Hnatic-m7--> </InlineEquation> are of the same order, i.e. <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10093_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha = O(\epsilon )\)</EquationSource> <!--PhysPNLt2570008Hnatic-m8--> </InlineEquation>. Our primary theoretical tool is field-theoretic perturbative renormalization group augmented with the approach of Honkonen and Nalimov [8]. The model is renormalized to all orders of perturbation theory, stable long-time asymptotic regimes are identified and time-decay exponent of respective particle densities is calculated.</p>

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Renormalization Group Analysis of Two-Species Reaction-Diffusion System: Crossover between Long-Range and Short-Range Spreading

  • M. Hnatič,
  • M. Kecer,
  • T. Lučivjanský

摘要

Abstract

In this work we focus on two-species reaction-diffusion system involving two reaction processes \(A + A \to (\emptyset ,A)\) , and \(A + B \to A\) . Reactants are subject to diffusive spreading with arbitrary diffusion constants. Such a system was studied earlier at and below its upper critical dimension \({{d}_{{\text{c}}}} = 2\) in [2, 3], and recently also in the presence of long-range spreading with fractional Laplace operator \({{\partial }^{\sigma }} \equiv {{\partial }^{{2(1 - \alpha )}}}\) [5–7]. In the latter case, however, only long-range limit was explored ( \(\alpha \gg \epsilon \) ), where \(\epsilon = {{d}_{{\text{c}}}} - d = 2 - d\) . Here, our aim is to investigate the hybrid regime in which parameters α and \(\epsilon \) are of the same order, i.e. \(\alpha = O(\epsilon )\) . Our primary theoretical tool is field-theoretic perturbative renormalization group augmented with the approach of Honkonen and Nalimov [8]. The model is renormalized to all orders of perturbation theory, stable long-time asymptotic regimes are identified and time-decay exponent of respective particle densities is calculated.