<p>This paper focuses on remainder estimates of the magnetic <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2219_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-Hardy inequalities for <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2219_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt;p&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. <i>Firstly</i>, we establish a family of remainder terms involving magnetic gradients of the magnetic <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2219_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-Hardy inequalities, which are also new even for the classical <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2219_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-Hardy inequalities. <i>Secondly</i>, we study another family of remainder terms involving logarithmic terms of the magnetic <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2219_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-Hardy inequalities. <i>Lastly</i>, as a byproduct, we further obtain remainder terms of some other <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2219_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-Hardy-type inequalities by using similar proof of our main results.Furthermore, this paper answers the open question proposed by Cazacu <i>et al.</i> in [Nonlinearity 37:035004, 2024] and can be viewed as a supplementary work of it.</p>

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Remainder Terms of \(L^p\)-Hardy Inequalities with Magnetic Fields: The Case \(1

  • Xiao-Ping Chen,
  • Chun-Lei Tang

摘要

This paper focuses on remainder estimates of the magnetic \(L^p\) L p -Hardy inequalities for \(1<p<2\) 1 < p < 2 . Firstly, we establish a family of remainder terms involving magnetic gradients of the magnetic \(L^p\) L p -Hardy inequalities, which are also new even for the classical \(L^p\) L p -Hardy inequalities. Secondly, we study another family of remainder terms involving logarithmic terms of the magnetic \(L^p\) L p -Hardy inequalities. Lastly, as a byproduct, we further obtain remainder terms of some other \(L^p\) L p -Hardy-type inequalities by using similar proof of our main results.Furthermore, this paper answers the open question proposed by Cazacu et al. in [Nonlinearity 37:035004, 2024] and can be viewed as a supplementary work of it.