Search arXiv⌕ Search

arXiv · 2610.36293

A fractional modular Poincaré--Wirtinger-type inequality in Sobolev spaces with variable exponents

Abstract

Let $Ω\subset\mathbb{R}^n$ be a bounded Lipschitz domain and let $p:Ω\to[1,\infty)$ be a measurable, essentially bounded exponent; no regularity of $p$ -- in particular, no log-Hölder continuity -- is assumed. For a general non-negative measurable kernel $\mathcal{K}(x,y)$ admitting a radial bounding function $κ(x,r)$ in the second variable, we establish the fractional modular Poincaré--Wirtinger-type inequality $$ \iint_{Ω\timesΩ}\mathcal{K}(x,y)\,|u(x)-u(y)|^{p(x)} d y\, d x \leqslant C\int_Ωc(x)\left(\int_Ω \frac{|\nabla u(z)|^{p(x)}}{|z-x|^{n-1+θ}}\, d z\right) d x, $$ valid for every $u\in W^{1,1}(Ω)$, in particular every $u\in W^{1,p(\cdot)}(Ω)$, and every $θ\in[0,1)$. Here $$ c(x)=\int_0^{D}r^{n+p(x)-2+θ}κ(x,r)\,d r, $$ $D$ is the diameter of any fixed ball containing $\overlineΩ$, and the constant $C$ depends only on $n,p^+,θ$ and the fixed domain $Ω$. For the fractional kernel $\mathcal{K}(x,y)=|x-y|^{-n-λp(x)}$ we obtain a variable-exponent Gagliardo-modular estimate. The proof replaces the starshaped chain decompositions used there by a combination of a Morrey-type estimate on starshaped domains, a positive-kernel proof of weighted Poincaré inequalities, and one reflection extension for the weights $|z-x|^{-(n-1+θ)}$. The constants are uniform down to exponent $1$, and the inequalities are understood in the extended nonnegative sense when either side is infinite.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Giovanni Di Fratta, Alberto Fiorenza, Leon Happ. 2026-10-26. A fractional modular Poincaré--Wirtinger-type inequality in Sobolev spaces with variable exponents. https://arxiv.org/abs/2610.36293

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Local rigidity of conformally Euclidean metrics for the anisotropic Helmholtz equation at fixed energy

We prove local rigidity of smooth conformally Euclidean metrics $g_0$ on smooth compact domains $M\subset\mathbb{R}^n$, $n\ge3$, for the anisotropic Helmholtz equation $(-Δ_g -k^2)u =0$ at a fixed energy $k^2>0$ which is not a Dirichlet eigenvalue of $-Δ_{g_0}$ in $M$. Any smooth metric sufficiently close to $g_0$ in $H^s(M)$, with integer $s>n/2+1$, and having the same Dirichlet-to-Neumann map, is its pullback by a smooth diffeomorphism fixing the boundary pointwise. The proof uses a Helmholtz embedding to fix the gauge and a compactness argument together with a characterization of the kernel of the linearization.

math.AP↗

A self-contained proof of the variational characterization of the principal eigenvalue of $-Δ+q$ under general Robin boundary conditions of non-classical type

In this paper, we are going to deliver a completely self-contained proof of the variational characterization of the principal eigenvalue of $-Δ+q$ in $Ω$ under Robin boundary conditions of non-classical type, $\frac{\partial u}{\partial n}+β(x)u=0$ on $\partialΩ$, where $β(x)$ is allowed to change sign on $\partialΩ$. The classical case occurs in the very special case when $β\geq 0$ on $\partialΩ$.

math.AP↗

Large data global strong solutions to the quantum Navier-Stokes equations with degenerate viscosity

This work is devoted to study the Cauchy problem for the quantum Navier-Stokes equations in $\mathbb R^N$, $N=2,3$, with density dependent viscosities $μ(ρ)=ρ,λ(ρ)=0$, quantum capillarity $κ(ρ)=1/ρ$, which was derived by Dunn and Serrin (see Arch. Ration. Mech. Anal. 88(2):95-133, 1985) as a phase transition model. For arbitrarily large initial data satisfying suitable regularity and decay assumptions, with density positive at every finite point and vanishing at infinity, we prove the existence and uniqueness of global strong solutions without symmetry assumptions. The admissible pressure range is $γ\ge 1$ in two dimensions and $1\leγ< 8/3$ in three dimensions. On every finite time interval, the density remains pointwise comparable to its initial profile, and both the effective velocity and the logarithmic density gradient remain bounded. The central estimates require no uniform positive lower bound for the density. When $γ>1$, a suitable combination of the density and effective velocity equations allows the maximum principle to yield an $L^\infty$ bound for the effective velocity using only an upper bound for the density. We then introduce the relative density with respect to a fixed profile determined by the initial data. In the isothermal case $γ=1$, we combine estimates for this relative density with a scalar inequality involving the effective velocity and the logarithmic density to close the coupled estimates and obtain the effective velocity bound. Combining the relative-density bounds with weighted gradient estimates and localized De Giorgi iteration, we control the logarithmic density gradient and close the higher-order estimates.

math.AP↗