<p>The inverse power potential <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(U(r)=r^{-1/s}, 0&lt;s&lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>U</mi> <mrow> <mo stretchy="false">(</mo> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>r</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mi>s</mi> </mrow> </msup> <mo>,</mo> <mn>0</mn> <mo>&lt;</mo> <mi>s</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> generates the Boltzmann kernel <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(B^{s}=|v-v_*|^{1-4s} b_s(\theta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>B</mi> <mi>s</mi> </msup> <mo>=</mo> <mmultiscripts> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo>-</mo> <mmultiscripts> <mi>v</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mo stretchy="false">|</mo> </mrow> <mrow /> <mrow> <mn>1</mn> <mo>-</mo> <mn>4</mn> <mi>s</mi> </mrow> </mmultiscripts> <msub> <mi>b</mi> <mi>s</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>θ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with an angular singularity as <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\theta \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>θ</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Jang et al. [<CitationRef CitationID="CR7">7</CitationRef>] proved the limit <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(B^{s}\rightarrow \frac{1}{4}|v-v_*|\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>B</mi> <mi>s</mi> </msup> <mo stretchy="false">→</mo> <mfrac> <mn>1</mn> <mn>4</mn> </mfrac> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo>-</mo> <mmultiscripts> <mi>v</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mo stretchy="false">|</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(s\rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, as well as weak convergence of solutions, but without a rate. In this work we establish the sharp estimate <Equation ID="Equ162"> <EquationSource Format="TEX">\( |b_s(\theta )-\tfrac{1}{4}| \le C\, s\,\theta ^{-2-2s}. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mrow> <mo stretchy="false">|</mo> </mrow> <msub> <mi>b</mi> <mi>s</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>θ</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mstyle displaystyle="false" scriptlevel="0"> <mfrac> <mn>1</mn> <mn>4</mn> </mfrac> </mstyle> <mrow> <mo stretchy="false">|</mo> <mo>≤</mo> <mi>C</mi> <mspace width="0.166667em" /> <mi>s</mi> <mspace width="0.166667em" /> </mrow> <msup> <mi>θ</mi> <mrow> <mo>-</mo> <mn>2</mn> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </msup> <mo>.</mo> </mrow> </math></EquationSource> </Equation>In particular, this sharp estimate yields the <i>optimal</i> <i>O</i>(<i>s</i>) convergence rate for solutions of the homogeneous Boltzmann equation with large initial data in suitable Sobolev spaces; i.e., for any <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(t\in [0,T]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, we have <Equation ID="Equ163"> <EquationSource Format="TEX">\(\begin{aligned} f^s(t)=f^0(t)+O(s), \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mi>f</mi> <mi>s</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>f</mi> <mn>0</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>O</mi> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>quantified by the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(L^1_k\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>L</mi> <mi>k</mi> <mn>1</mn> </msubsup> </math></EquationSource> </InlineEquation> norm for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(k\ge 2.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>≥</mo> <mn>2</mn> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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Optimal Convergence Estimate of the Limit from Inverse Power Potential to Hard Sphere Boltzmann Equation

  • Zheng-Nan Hu,
  • Jin Woo Jang,
  • Zheng-An Yao,
  • Yu-Long Zhou

摘要

The inverse power potential \(U(r)=r^{-1/s}, 0<s<1\) U ( r ) = r - 1 / s , 0 < s < 1 generates the Boltzmann kernel \(B^{s}=|v-v_*|^{1-4s} b_s(\theta )\) B s = | v - v | 1 - 4 s b s ( θ ) with an angular singularity as \(\theta \rightarrow 0\) θ 0 . Jang et al. [7] proved the limit \(B^{s}\rightarrow \frac{1}{4}|v-v_*|\) B s 1 4 | v - v | as \(s\rightarrow 0\) s 0 , as well as weak convergence of solutions, but without a rate. In this work we establish the sharp estimate \( |b_s(\theta )-\tfrac{1}{4}| \le C\, s\,\theta ^{-2-2s}. \) | b s ( θ ) - 1 4 | C s θ - 2 - 2 s . In particular, this sharp estimate yields the optimal O(s) convergence rate for solutions of the homogeneous Boltzmann equation with large initial data in suitable Sobolev spaces; i.e., for any \(t\in [0,T]\) t [ 0 , T ] , we have \(\begin{aligned} f^s(t)=f^0(t)+O(s), \end{aligned}\) f s ( t ) = f 0 ( t ) + O ( s ) , quantified by the \(L^1_k\) L k 1 norm for \(k\ge 2.\) k 2 .