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On $L^p$-Hardy inequalities for magnetic $p$-Laplacians

Yi C. Huang, Xinhang Tong

TL;DR

The paper addresses remainder terms in $L^p$ Hardy inequalities for magnetic $p$-Laplacians and identifies the sharp constant in a key algebraic inequality. It introduces an integral representation $R_p$ that yields a precise expression for $C_p(x,y)/|y|^p$ and reduces the problem to a one-variable minimization over $k=x/|y|$. For $p\ge2$ the sharp constant $c_p$ is positive and given by $c_p=(p-1)(1-k_0)^p+pk_0(1-k_0)^{p-1}+k_0^p$ with $k_0=r_0/(1+r_0)$ where $r_0$ solves $r^{p-1}-(p-1)r-(p-2)=0$, while for $1<p<2$ one has $c_p=0$. The paper also provides the explicit value $c_3=2- obreak\sqrt{2}$ and sketches the proofs of these claims, including equality cases when $x=\lambda y$.

Abstract

In this paper we revisit the remainder terms of $L^p$-Hardy inequalities for magnetic $p$-Laplacians. In particular, we will give an integral representation of the sharp constant for a crucial algebraic inequality established by C. Cazacu, D. Krejčiřík, N. Lam, and A. Laptev.

On $L^p$-Hardy inequalities for magnetic $p$-Laplacians

TL;DR

The paper addresses remainder terms in Hardy inequalities for magnetic -Laplacians and identifies the sharp constant in a key algebraic inequality. It introduces an integral representation that yields a precise expression for and reduces the problem to a one-variable minimization over . For the sharp constant is positive and given by with where solves , while for one has . The paper also provides the explicit value and sketches the proofs of these claims, including equality cases when .

Abstract

In this paper we revisit the remainder terms of -Hardy inequalities for magnetic -Laplacians. In particular, we will give an integral representation of the sharp constant for a crucial algebraic inequality established by C. Cazacu, D. Krejčiřík, N. Lam, and A. Laptev.

Paper Structure

This paper contains 2 sections, 3 theorems, 36 equations.

Key Result

Theorem 2

Let $2 \leq p < d$ and $B$ be a smooth and closed magnetic field with $B \neq 0$. Then there exists a constant $c_{p} > 0$ such that for any vector field $A$ with $dA = B$, and for any $u \in \mathcal{D}(h_{A,p})$, The constant $c_p$ is given by

Theorems & Definitions (9)

  • Definition 1
  • Theorem 2: Cazacu2024, Theorem 1.2
  • Theorem 3
  • Remark 4
  • Remark 5
  • Theorem 6
  • Remark 7
  • proof : Proof of Theorem \ref{['exrep']}
  • proof : Proof of Theorem \ref{['solution']}