<p>We consider the local times of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((1 + \beta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>+</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-stable <i>d</i>-dimensional super-Brownian motion with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(0&lt; \beta &lt; 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>β</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. It is known from Sugitani (J Math Soc Jpn 41(3):437–462, 1989) that for <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\beta = 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, the local time is differentiable for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(d=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. For <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(0&lt; \beta &lt; 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>β</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, Mytnik and Perkins (Ann Probab 31(3): 1413–1440, 2003) proved that the local time, denoted by <i>L</i>(<i>t</i>,&#xa0;<i>x</i>), is jointly continuous for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(d = 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, while it is locally unbounded in <i>x</i> for <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(d \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> where it exists. This paper strengthens the results of Mytnik and Perkins for <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(d=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> by showing that the local time <i>L</i>(<i>t</i>,&#xa0;<i>x</i>) is continuously differentiable in the spatial parameter <i>x</i>. Moreover, we give a representation of the spatial derivative, denoted by <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\frac{\partial }{\partial x}L(t, x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfrac> <mi>∂</mi> <mrow> <mi>∂</mi> <mi>x</mi> </mrow> </mfrac> <mi>L</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and further prove that the derivative is locally <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-Hölder continuous in <i>x</i> for any index <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\gamma \in (0, \frac{\beta }{1+\beta })\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mi>β</mi> <mrow> <mn>1</mn> <mo>+</mo> <mi>β</mi> </mrow> </mfrac> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>.</p>

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On the Differentiability of Local Times of (\(1+\beta \))-Stable Super-Brownian Motion

  • Ziyi Chen,
  • Jieliang Hong

摘要

We consider the local times of \((1 + \beta )\) ( 1 + β ) -stable d-dimensional super-Brownian motion with \(0< \beta < 1\) 0 < β < 1 . It is known from Sugitani (J Math Soc Jpn 41(3):437–462, 1989) that for \(\beta = 1\) β = 1 , the local time is differentiable for \(d=1\) d = 1 . For \(0< \beta < 1\) 0 < β < 1 , Mytnik and Perkins (Ann Probab 31(3): 1413–1440, 2003) proved that the local time, denoted by L(tx), is jointly continuous for \(d = 1\) d = 1 , while it is locally unbounded in x for \(d \ge 2\) d 2 where it exists. This paper strengthens the results of Mytnik and Perkins for \(d=1\) d = 1 by showing that the local time L(tx) is continuously differentiable in the spatial parameter x. Moreover, we give a representation of the spatial derivative, denoted by \(\frac{\partial }{\partial x}L(t, x)\) x L ( t , x ) , and further prove that the derivative is locally \(\gamma \) γ -Hölder continuous in x for any index \(\gamma \in (0, \frac{\beta }{1+\beta })\) γ ( 0 , β 1 + β ) .