<p>In the context of Hardy inequalities for the fractional Laplacian <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((-\Delta _{\mathbb {N}})^{\sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">N</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mi>σ</mi> </msup> </math></EquationSource> </InlineEquation> on the discrete half-line <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">N</mi> </math></EquationSource> </InlineEquation>, we provide an optimal Hardy-weight <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(W^{\textrm{op}}_{\sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>W</mi> <mi>σ</mi> <mtext>op</mtext> </msubsup> </math></EquationSource> </InlineEquation> for exponents <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\sigma \in \left( 0,1\right] \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo>∈</mo> <mfenced close="]" open="("> <mn>0</mn> <mo>,</mo> <mn>1</mn> </mfenced> </mrow> </math></EquationSource> </InlineEquation>. As a consequence, we provide an estimate of the sharp constant in the fractional Hardy inequality with the classical Hardy-weight <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(n^{-2\sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>n</mi> <mrow> <mo>-</mo> <mn>2</mn> <mi>σ</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathbb {N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">N</mi> </math></EquationSource> </InlineEquation>. It turns out that for <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\sigma =1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> the Hardy-weight <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(W^{\textrm{op}}_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>W</mi> <mn>1</mn> <mtext>op</mtext> </msubsup> </math></EquationSource> </InlineEquation> is pointwise larger than the optimal Hardy-weight obtained by Keller–Pinchover–Pogorzelski near infinity. As an application of our main result, we obtain unique continuation results at infinity for the solutions of some fractional Schrödinger equation.</p>

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An optimal fractional Hardy inequality on the discrete half-line

  • Ujjal Das,
  • Rubén de la Fuente-Fernández

摘要

In the context of Hardy inequalities for the fractional Laplacian \((-\Delta _{\mathbb {N}})^{\sigma }\) ( - Δ N ) σ on the discrete half-line \(\mathbb {N}\) N , we provide an optimal Hardy-weight \(W^{\textrm{op}}_{\sigma }\) W σ op for exponents \(\sigma \in \left( 0,1\right] \) σ 0 , 1 . As a consequence, we provide an estimate of the sharp constant in the fractional Hardy inequality with the classical Hardy-weight \(n^{-2\sigma }\) n - 2 σ on \(\mathbb {N}\) N . It turns out that for \(\sigma =1\) σ = 1 the Hardy-weight \(W^{\textrm{op}}_{1}\) W 1 op is pointwise larger than the optimal Hardy-weight obtained by Keller–Pinchover–Pogorzelski near infinity. As an application of our main result, we obtain unique continuation results at infinity for the solutions of some fractional Schrödinger equation.