<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10959_2025_1450_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\{X_t\}_{t\ge 0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">{</mo> <msub> <mi>X</mi> <mi>t</mi> </msub> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>t</mi> <mo>≥</mo> <mn>0</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> be a <i>d</i>-dimensional critical or subcritical super-Brownian motion started from the Lebesgue measure. Denote by <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10959_2025_1450_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="335" /> </InlineMediaObject> <EquationSource Format="TEX">\(R_t:=\sup \{u&gt;0: X_t(\{x\in \mathbb {R}^d:|x|&lt; u\})=0\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>R</mi> <mi>t</mi> </msub> <mrow> <mo>:</mo> <mo>=</mo> <mo movablelimits="true">sup</mo> <mo stretchy="false">{</mo> <mi>u</mi> <mo>&gt;</mo> <mn>0</mn> <mo>:</mo> </mrow> <msub> <mi>X</mi> <mi>t</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mo stretchy="false">{</mo> <mi>x</mi> </mrow> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mrow> <mo>:</mo> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> <mo>&lt;</mo> <mi>u</mi> <mo stretchy="false">}</mo> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> <mo stretchy="false">}</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> the radius of the largest empty ball centred at the origin of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10959_2025_1450_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(X_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>X</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>. This article shows that <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10959_2025_1450_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(R_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> will converge in law after suitable renormalization as <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10959_2025_1450_Article_IEq5.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. Our results indicate that the renormalization scale of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10959_2025_1450_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(R_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> not only depends on the dimension but also depends on whether the branching mechanism has finite variance and is critical or not, which completes our previous results for the critical super-Brownian with quadratic branching mechanism (Zhang and Xiong in Bernoulli 30:72–87, 2024) and reveals some new phase transitions.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

On the Empty Balls of Critical and Subcritical Super-Brownian Motions with General Branching Mechanisms

  • Shuxiong Zhang,
  • Jiawei Liu,
  • Jie Xiong

摘要

Let \(\{X_t\}_{t\ge 0}\) { X t } t 0 be a d-dimensional critical or subcritical super-Brownian motion started from the Lebesgue measure. Denote by \(R_t:=\sup \{u>0: X_t(\{x\in \mathbb {R}^d:|x|< u\})=0\}\) R t : = sup { u > 0 : X t ( { x R d : | x | < u } ) = 0 } the radius of the largest empty ball centred at the origin of \(X_t\) X t . This article shows that \(R_t\) R t will converge in law after suitable renormalization as \(t\rightarrow \infty \) t . Our results indicate that the renormalization scale of \(R_t\) R t not only depends on the dimension but also depends on whether the branching mechanism has finite variance and is critical or not, which completes our previous results for the critical super-Brownian with quadratic branching mechanism (Zhang and Xiong in Bernoulli 30:72–87, 2024) and reveals some new phase transitions.