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Super-Linear Reverse Hölder Inequalities

Updated 15 January 2026
  • Super-linear reverse Hölder inequalities are quantitative integrability bounds that extend the classical reverse Hölder property with explicit constants and self-improvement effects.
  • They are applied across harmonic analysis, PDEs, high-dimensional probability, and operator theory to refine norm comparisons and establish maximal integrability.
  • Recent advances include sharp constant formulations and extensions to variable exponent, Orlicz, and matrix contexts, underscoring their foundational role in analysis.

Super-linear reverse Hölder inequalities are quantitative integrability bounds that extend the classical reverse Hölder property into the regime of strictly super-linear (i.e., exponent p>1p>1) averages, yielding self-improving integrability and sharp norm-comparisons for functions, measures, weights, operators, and distributions in functional analysis, harmonic analysis, partial differential equations, and high-dimensional probability. This article synthesizes core models, explicit constants, functional and geometric contexts, and rigorous sharpness results drawn from recent research.

1. Core Quantitative Model and Explicit Formulations

Super-linear reverse Hölder inequalities consistently exhibit the following structural form on a measure space (X,μ)(X,\mu), for p>1p>1: $\left( \fint_{Q} f^p\,d\mu \right)^{1/p} \leq C \fint_{Q} f\,d\mu\,,$ where f0f\geq0 is measurable, QQ is a cube (or ball, or rectangle), and CC depends on dimension, underlying quantitative weight characteristic, and other structural data.

Recent advances provide sharp constants and explicit dependence:

  • Muckenhoupt AA_\infty and Strong ApA^*_p Weights: Asymptotically sharp exponents and constants are established so that as the weight approaches uniformity, the integrability exponent blows up, e.g.,

$\left(\fint_Q w^r\right)^{1/r} \leq (w)_{A_\infty}^{1/r'} \left(\frac{r'-1}{r'-1-2^n\big[(w)_{A_\infty}-1\big]}\right)^{1/r} \fint_Q w,$

where (w)A(w)_{A_\infty} is the Fujii–Wilson constant, r<1+1/[2n((w)A1)]r < 1+1/[2^n((w)_{A_\infty}-1)] (Parissis et al., 2016), and analogously

$(\dashint_R w^{1+\varepsilon}d\mu)^{1/(1+\varepsilon)} \leq 2\,\dashint_R w\,d\mu, \quad \text{for } 0 < \varepsilon < 2^{-(p+2)}[w]_{A_p^*}^{-1}$

for strong ApA_p^* weights, with no dimension dependence in the constant (Luque et al., 2015).

  • Variable exponent weights Ap()\mathcal{A}_{p(\cdot)}: For Lebesgue spaces with variable exponent p(x)[1,)p(x)\in [1,\infty), and wAp()w\in A_{p(\cdot)}, there exists r>1r>1 such that

Q1/rpQwχQLrp()Cp()Q1/pQwχQLp(),|Q|^{-1/r p_Q} \|w\chi_Q\|_{L^{rp(\cdot)}} \leq C_{p(\cdot)} |Q|^{-1/p_Q}\|w\chi_Q\|_{L^{p(\cdot)}},

with r=1+1/[C[w]Ap()1+2Cp+/(pp)]r = 1 + 1/[C_* [w]_{A_{p(\cdot)}}^{1+2C_\infty p^+/(p_\infty p^-)}]; the gain ε=r1\varepsilon = r-1 is explicit (Cruz-Uribe et al., 2024).

  • Extremal Sobolev Functions: Sharp reverse Hölder inequalities for extremals of Sobolev constants are quantified, e.g., for uu attaining the optimal Sobolev constant,

uLpKuLq,q>p,\|u\|_{L^p} \geq K\,\|u\|_{L^q}, \quad q > p,

with KK given explicitly in terms of geometric parameters and Sobolev constant (Carroll et al., 2014).

2. Self-Improvement and Structural Mechanisms

A recurring phenomenon in the super-linear regime is quantitative self-improvement: if a reverse Hölder inequality holds with exponent p>1p>1, then there exists ε>0\varepsilon>0 depending only on the underlying constants (dimension, quantitative characteristic) such that the inequality holds for p+εp+\varepsilon. This "Gehring-type" mechanism is now realized with explicit formulas:

  • For flat AA_\infty weights, as (w)A1+(w)_{A_\infty}\to 1^+, the allowed exponent grows arbitrarily large, demonstrating maximal integrability for nearly constant weights (Parissis et al., 2016).
  • In the dyadic setting, the reverse Hölder constant after rearrangement is sharpened via explicit formula c=2nc2n+1c' = 2^n c - 2^n + 1, and maximal LqL^q integrability is characterized as the sharp root p0(p,c)p_0(p,c') of a fixed algebraic equation (Nikolidakis et al., 2014).

A prototypical proof sequence employs:

3. Generalized Weight and Operator Settings

Super-linear reverse Hölder inequalities admit generalization in variable exponent, Orlicz, and operator contexts:

  • Orlicz Scale: For Young functions Φ\Phi with super-linear growth, reverse Hölder inequalities and extrapolation theorems provide additional integrability on the class RHΦRH_{\Phi}, which is properly stronger than AA_\infty and allows refined norm inequalities for Calderón–Zygmund and multilinear singular integral operators (Anderson et al., 2016).
  • Matrix and Operator Norms: In matrix analysis, reverse Hölder inequalities extend to Schatten quasi-norms (0<s<1) and super-linear powers, providing dual variational representations and characterizations of equality (Chayes, 2021). For positive operators in Hilbert spaces, explicit bounds for differences between AtxA^{t}x and (Ax)t(Ax)^t are given in terms of lower moments (reverse Hölder–McCarthy) (Hajmohamadi et al., 2018).

4. Nonlinear PDEs and Harmonic Analysis Applications

Super-linear reverse Hölder inequalities are fundamental in establishing higher integrability for gradients in nonlinear PDEs:

  • Trudinger Equation: For solutions u0u\geq0 of the doubly-nonlinear equation, a covering and reverse Hölder iteration yields

uLp(1+ε)(Q)CuLp(2Q),\|\nabla u\|_{L^{p(1+\varepsilon)}(Q)} \leq C\,\|\nabla u\|_{L^p(2Q)},

where ε\varepsilon and CC depend only on structure constants, without upper bounds on pp (Saari et al., 2019).

  • Riesz Transforms and Metric Spaces: On doubling metric measure spaces, super-linear reverse Hölder inequalities (q>1q>1) for weights or gradients are central to extending LpL^p-boundedness for Riesz transforms and related operators, with explicit quantitative control via the self-improvement mechanism (Gehring lemma) (Bernicot et al., 2015).

5. Probability, Gaussian Measures, and Extremal Distributions

Super-linear reverse Hölder phenomena govern discrete and continuous moment inequalities in high-dimensional probability:

  • Log-Concave Distributions: For centred log-concave XX, sharp LpL_p-L1L_1 and mixed LpL_p-LqL_q reverse Hölder inequalities are determined by a universal family of two-sided exponential laws, with a phase transition at p02.9414p_0\approx2.9414 (Melbourne et al., 2 May 2025).

XpΓ(p+1)1/pΓ(q+1)1/qXq\|X\|_p \geq \frac{\Gamma(p+1)^{1/p}}{\Gamma(q+1)^{1/q}}\|X\|_q

for 1<p1qp0-1<p\leq1\leq q\leq p_0, with sharp attainment on the Laplace and exponential distributions.

  • Correlated Gaussians and Functional Inequalities: For block covariance matrices TT and exponents pi>1p_i>1, a matrix criterion TPT\succeq P yields

Ei=1mfi(Xi)i=1m(Efi(Xi)pi)1/pi\mathbb{E}\prod_{i=1}^m f_i(X_i) \geq \prod_{i=1}^m (\mathbb{E}f_i(X_i)^{p_i})^{1/p_i}

with equality for exponential-linear test functions. This unifies reverse hypercontractivity, Prekopa–Leindler, and Young inequalities (Chen et al., 2013).

6. Sharpness, Optimality, and Limiting Cases

Recent advances emphasize sharp constants, characterization of equality, and limiting cases:

  • For AA_\infty and A1A_1 weights, both the range of allowed exponents and multiplicative constants have been shown to be best possible via explicit extremizers (Parissis et al., 2016, Luque et al., 2015).
  • The continuous improvement as the underlying weight or operator becomes "flatter" or more regular is quantified; in particular, as the characteristic tends to its minimal value, the integrability exponent diverges.
  • Reverse Hölder inequalities for extremal Sobolev functions attain equality only for balls (Carroll et al., 2014), and in probabilistic and operator settings, extremizers are explicit.

7. Summary Table: Explicit Super-linear RHI Models

Context/class Inequality (core model) Quantitative range/constant
Classical ApA_p/AA_\infty $\left(\fint_Q w^r\right)^{1/r} \leq C\,\fint_Q w$ r<1+1/[2n((w)A1)]r < 1+1/[2^n((w)_{A_\infty}-1)] (Parissis et al., 2016)
Dyadic cubes in [0,1]n[0,1]^n 1QQφpc(1QQφ)p\frac{1}{|Q|}\int_Q \varphi^p \leq c\,(\frac{1}{|Q|}\int_Q \varphi)^p c=2nc2n+1c' = 2^n c - 2^n + 1, explicit p0(p,c)p_0(p,c') (Nikolidakis et al., 2014)
Variable exponent weights Q1/rpQwχQLrp()CQ1/pQwχQLp()|Q|^{-1/rp_Q}\|w\chi_Q\|_{L^{rp(\cdot)}} \leq C\,|Q|^{-1/p_Q}\|w\chi_Q\|_{L^{p(\cdot)}} r=1+1/[quantitative characteristic]r = 1 + 1/[\text{quantitative characteristic}] (Cruz-Uribe et al., 2024)
Sobolev extremals uLpKuLq\|u\|_{L^p} \geq K\,\|u\|_{L^q} KK explicit from geometry, only balls attain equality (Carroll et al., 2014)
Log-concave XX Xp[Γ(p+1)1/p/Γ(q+1)1/q]Xq\|X\|_p \geq [\Gamma(p+1)^{1/p}/\Gamma(q+1)^{1/q}]\|X\|_q p1qp02.94p\leq1\leq q\leq p_0 \approx 2.94 (Melbourne et al., 2 May 2025)

8. Further Directions and Open Problems

Current research continues to refine constants and exponents, extend reverse Hölder theory to nonlinear growth (Orlicz, p()p(\cdot)), matrix-valued weights, non-doubling and product measures, and to applications in sharp weighted norm inequalities for singular integrals. Optimizing constants in variable exponent reverse Hölder remains open (Cruz-Uribe et al., 2024). Extending sharp RHI to sign-changing or vector-valued solutions in nonlinear PDE theory is also unresolved (Saari et al., 2019).

Super-linear reverse Hölder inequalities thus constitute a foundational, highly quantitative framework with far-reaching consequences in analysis, probability, and operator theory.

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