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Some quasilinear minimization problems involving Hardy potentials

Published 14 Jun 2026 in math.AP | (2606.15849v1)

Abstract: In this note, we consider several quasiliniear minimization problems involving various Hardy type potentials for functions in W<sup>1,p(Ω)W<sup>{1,p}(Ω) with weighted mean zero. We prove that the strict inequality for the infimum yields the existence of a minimizer.

Authors (2)

Summary

  • The paper proves positivity of weighted mean-zero Hardy constants and attainment below the universal Hardy threshold for point and submanifold singularities, as well as critical logarithmic weights.
  • The authors combine Cherrier-type Hardy refinements with the Valeriola–Willem gradient Brezis–Lieb theorem to recover compactness and establish strong convergence of minimizing sequences.
  • The strict gap condition is verified for selected balls using coordinate-function test cases, while the method remains limited to subcritical dimensions, admissible geometries, and domains without a general gap criterion.

Setting and motivation

The paper studies quasilinear minimization problems of Hardy type on a smooth bounded domain ΩRN\Omega \subset \mathbb{R}^N with 0Ω0 \in \Omega. The classical W01,pW^{1,p}_0-Hardy inequality asserts that the best constant

Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p

is positive, independent of Ω\Omega, and never attained in W01,p(Ω)W^{1,p}_0(\Omega) for $1 < p < N$. This non-attainability is a manifestation of the lack of compactness in the embedding W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx). The authors' strategy, following Chabrowski–Peral–Ruf for the case p=2p=2 (2606.15849), is to restore compactness by restricting to the closed subspace

Xp={uW1,p(Ω):Ωuxpdx=0},X_p = \left\{ u \in W^{1,p}(\Omega) : \int_\Omega \frac{u}{|x|^p}\,dx = 0 \right\},

i.e., functions with weighted mean zero, and minimizing the Rayleigh quotient over 0Ω0 \in \Omega0:

0Ω0 \in \Omega1

The same program is carried out in two further settings: the geometric Hardy inequality of Barbatis–Filippas–Tertikas with potential 0Ω0 \in \Omega2 attached to a submanifold 0Ω0 \in \Omega3 of codimension 0Ω0 \in \Omega4 satisfying the condition 0Ω0 \in \Omega5 weakly, and the critical logarithmic Hardy inequality for 0Ω0 \in \Omega6, where the weight is 0Ω0 \in \Omega7.

Main results

The three theorems share a common structure. For 0Ω0 \in \Omega8 (with 0Ω0 \in \Omega9 covering the point singularity), W01,pW^{1,p}_00; moreover, if the strict inequality

W01,pW^{1,p}_01

holds, then the infimum is attained by a non-zero function in W01,pW^{1,p}_02. Analogously, for the critical exponent,

W01,pW^{1,p}_03

implies attainability of W01,pW^{1,p}_04 on W01,pW^{1,p}_05. The positivity statements hold unconditionally; only the attainment requires the strict gap below the universal constant. Theorem 2 extends the earlier work of Sano–Takahashi from W01,pW^{1,p}_06 to all W01,pW^{1,p}_07.

The strictness assumption is essential: it is used precisely at the points where the contradiction arguments would otherwise yield only the trivial inequality W01,pW^{1,p}_08. Whether the gap condition holds depends on the geometry of W01,pW^{1,p}_09; the paper does not characterize when it fails.

Analytic framework

Two ingredients drive the proofs. First, the authors establish Cherrier-type refinements of the Hardy inequalities valid on all of Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p0 (not merely Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p1): for every Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p2 there exists Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p3 such that

Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p4

with an analogous inequality for the critical logarithmic weight. These follow by cutting off with a test function Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p5 near Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p6 and applying the elementary inequality Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p7; the lower-order term absorbs the error away from the singularity.

Second, since the Brezis–Lieb identity for gradients generally fails for weakly convergent sequences in Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p8 when Hp=(Npp)pH_p = \left(\frac{N-p}{p}\right)^p9, the authors invoke a theorem of Valeriola–Willem: if a weakly convergent sequence satisfies the scalar condition

Ω\Omega0

where Ω\Omega1 for Ω\Omega2 and Ω\Omega3 otherwise, then Ω\Omega4 a.e., the Brezis–Lieb identity holds for the gradient, and Ω\Omega5 strongly in Ω\Omega6 for Ω\Omega7.

The core of each proof is verifying this scalar condition for a minimizing Palais–Smale sequence produced by the Ekeland variational principle on the constraint manifold Ω\Omega8. Testing the approximate Euler–Lagrange equation against Ω\Omega9, where W01,p(Ω)W^{1,p}_0(\Omega)0 normalizes W01,p(Ω)W^{1,p}_0(\Omega)1 into the constraint subspace, decomposes the expression into four terms; these vanish respectively by strong convergence of the Lagrange multipliers W01,p(Ω)W^{1,p}_0(\Omega)2 in the dual space, dominated convergence (using that W01,p(Ω)W^{1,p}_0(\Omega)3 when W01,p(Ω)W^{1,p}_0(\Omega)4), boundedness of the weighted W01,p(Ω)W^{1,p}_0(\Omega)5 norms, and weak convergence of W01,p(Ω)W^{1,p}_0(\Omega)6 to zero in W01,p(Ω)W^{1,p}_0(\Omega)7. With the Brezis–Lieb identity in hand, two contradiction steps show that the weak limit W01,p(Ω)W^{1,p}_0(\Omega)8 is non-trivial and saturates the constraint W01,p(Ω)W^{1,p}_0(\Omega)9, hence attains the infimum.

An implication worth noting: because the argument relies on $1 < p < N$0, the supercritical regime $1 < p < N$1 is outside the scope of the method as presented.

Verification of the gap condition

The paper provides concrete sufficient conditions under which the strict inequality holds, using the coordinate function $1 < p < N$2 as a test function.

For balls $1 < p < N$3 and $1 < p < N$4, symmetry gives $1 < p < N$5, and Hölder's inequality yields $1 < p < N$6. Hence the gap condition holds whenever $1 < p < N$7. For $1 < p < N$8, the estimate $1 < p < N$9 suffices, which holds for fixed W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)0 once W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)1 — true for large W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)2 since the ratio diverges as W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)3.

In the critical case, testing with W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)4 gives W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)5 as W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)6, via an asymptotic expansion of W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)7 obtained through integration by parts and l'Hôpital's rule. Thus the gap condition is satisfied for "fat" balls with W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)8 close to W01,p(Ω)Lp(Ω,xpdx)W^{1,p}_0(\Omega) \hookrightarrow L^p(\Omega, |x|^{-p}\,dx)9. These verifications are restricted to balls; no general geometric criterion on p=2p=20 is given.

Limitations and open questions

Several restrictions are inherent to the treatment. The attainment results are conditional on the strict gap p=2p=21, and the paper offers no characterization of domains or manifolds for which the gap fails — nor examples showing non-attainment when equality holds. The sufficient conditions for the gap are established only for balls, leaving the question open for general domains. The manifold hypothesis (K) excludes configurations where p=2p=22 changes sign, and the supercritical range p=2p=23 is not addressed. Finally, whether the minimizers exhibit specific qualitative behavior (regularity up to the singularity, asymptotic profiles analogous to those known in the linear case) is not investigated here.

Conclusion

The paper establishes positivity and conditional attainability of weighted-mean-zero Hardy constants in three quasilinear settings — point singularities, submanifold singularities, and the critical logarithmic weight — by combining Cherrier-type global Hardy inequalities with the Valeriola–Willem Brezis–Lieb machinery for gradients. The contribution is a systematic extension of techniques previously available for p=2p=24 to the full quasilinear range p=2p=25, together with explicit ball-domain regimes in which the required spectral gap provably holds.

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