<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(H_{G,v_0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mrow> <mi>G</mi> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> be the Hardy operator defined on the finite graph <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(G=(V,E)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo>=</mo> <mo stretchy="false">(</mo> <mi>V</mi> <mo>,</mo> <mi>E</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(v_0\in V\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>v</mi> <mn>0</mn> </msub> <mo>∈</mo> <mi>V</mi> </mrow> </math></EquationSource> </InlineEquation>. We obtain the <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\ell ^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-norm estimates for the operator <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H_{G,v_0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mrow> <mi>G</mi> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> in the corresponding strong-type (<i>p</i>,&#xa0;<i>p</i>) for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(0&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> and weak-type (<i>p</i>,&#xa0;<i>p</i>) for <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(0&lt;p\le \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. That is, (i) we obtain the upper and lower bounds for the <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\ell ^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-norm of a general graph <i>G</i> in the range <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(0&lt;p\le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and characterize a special kind of connected graph by the value of the operator norm <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\Vert H_{G,v_0}\Vert _{\ell ^{p}\rightarrow \ell ^{p}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>H</mi> <mrow> <mi>G</mi> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> </mrow> </msub> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> <mo stretchy="false">→</mo> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>; (ii) we obtain sharp constants for <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\Vert H_{G,v_0}\Vert _{\ell ^{p}\rightarrow \ell ^{p}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>H</mi> <mrow> <mi>G</mi> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> </mrow> </msub> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> <mo stretchy="false">→</mo> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> in the range <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(0&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> when <i>G</i> is the complete graph <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(K_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>K</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation>, the star graph <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(S_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> and the path <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(P_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(n\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>; (iii) we compute the weak-type norm <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\Vert H_{G,v_0}\Vert _{\ell ^{p}\rightarrow \ell ^{p,\infty }}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>H</mi> <mrow> <mi>G</mi> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> </mrow> </msub> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> <mo stretchy="false">→</mo> <msup> <mi>ℓ</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>∞</mi> </mrow> </msup> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(0&lt; p\le \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. Finally, we calculate the <i>p</i>-variation inequalities for the operator <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(H_{G,v_0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mrow> <mi>G</mi> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(G=K_{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo>=</mo> <msub> <mi>K</mi> <mi>n</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(G=S_{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo>=</mo> <msub> <mi>S</mi> <mi>n</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(G=P_{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo>=</mo> <msub> <mi>P</mi> <mi>n</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(0&lt;p\le \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Best constants for the Hardy operator on finite graphs

  • Jinjiao Wang,
  • Fayou Zhao

摘要

Let \(H_{G,v_0}\) H G , v 0 be the Hardy operator defined on the finite graph \(G=(V,E)\) G = ( V , E ) and \(v_0\in V\) v 0 V . We obtain the \(\ell ^p\) p -norm estimates for the operator \(H_{G,v_0}\) H G , v 0 in the corresponding strong-type (pp) for \(0<p<\infty \) 0 < p < and weak-type (pp) for \(0<p\le \infty \) 0 < p . That is, (i) we obtain the upper and lower bounds for the \(\ell ^p\) p -norm of a general graph G in the range \(0<p\le 1\) 0 < p 1 and characterize a special kind of connected graph by the value of the operator norm \(\Vert H_{G,v_0}\Vert _{\ell ^{p}\rightarrow \ell ^{p}}\) H G , v 0 p p ; (ii) we obtain sharp constants for \(\Vert H_{G,v_0}\Vert _{\ell ^{p}\rightarrow \ell ^{p}}\) H G , v 0 p p in the range \(0<p<\infty \) 0 < p < when G is the complete graph \(K_n\) K n , the star graph \(S_n\) S n and the path \(P_n\) P n with \(n\ge 2\) n 2 ; (iii) we compute the weak-type norm \(\Vert H_{G,v_0}\Vert _{\ell ^{p}\rightarrow \ell ^{p,\infty }}\) H G , v 0 p p , with \(0< p\le \infty \) 0 < p . Finally, we calculate the p-variation inequalities for the operator \(H_{G,v_0}\) H G , v 0 when \(G=K_{n}\) G = K n , \(G=S_{n}\) G = S n and \(G=P_{n}\) G = P n with \(0<p\le \infty \) 0 < p .