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We prove sharp L p → L q estimates for averaging operators along general polynomial curves in two and three dimensions. These operators are translation-invariant, given by convolution with the so-called affine arclength measure of the curve and we obtain universal bounds over the class of curves given by polynomials of bounded degree. Our method relies on a geometric inequality for general vector polynomials together with a combinatorial argument due to M. Christ. Almost sharp Lorentz space estimates are obtained as well.
We prove sharp L p → L q estimates for averaging operators along general polynomial curves in two and three dimensions. These operators are translation-invariant, given by convolution with the so-called affine arclength measure of the curve and we obtain universal bounds over the class of curves given by polynomials of bounded degree. Our method relies on a geometric inequality for general vector polynomials together with a combinatorial argument due to M. Christ. Almost sharp Lorentz space estimates are obtained as well.
This note concerns Loomis–Whitney inequalities in Heisenberg groups $$\mathbb {H}^n$$ H n : $$\begin{aligned} |K| \lesssim \prod _{j=1}^{2n}|\pi _j(K)|^{\frac{n+1}{n(2n+1)}}, \qquad K \subset \mathbb {H}^n. \end{aligned}$$ | K | ≲ ∏ j = 1 2 n | π j ( K ) | n + 1 n ( 2 n + 1 ) , K ⊂ H n . Here $$\pi _{j}$$ π j , $$j=1,\ldots ,2n$$ j = 1 , … , 2 n , are the vertical Heisenberg projections to the hyperplanes $$\{x_j=0\}$$ { x j = 0 } , respectively, and $$|\cdot |$$ | · | refers to a natural Haar measure on either $$\mathbb {H}^n$$ H n , or one of the hyperplanes. The Loomis–Whitney inequality in the first Heisenberg group $$\mathbb {H}^1$$ H 1 is a direct consequence of known $$L^p$$ L p improving properties of the standard Radon transform in $$\mathbb {R}^2$$ R 2 . In this note, we show how the Loomis–Whitney inequalities in higher dimensional Heisenberg groups can be deduced by an elementary inductive argument from the inequality in $$\mathbb {H}^1$$ H 1 . The same approach, combined with multilinear interpolation, also yields the following strong type bound: $$\begin{aligned} \int _{\mathbb {H}^n} \prod _{j=1}^{2n} f_j(\pi _j(p))\;dp\lesssim \prod _{j=1}^{2n} \Vert f_j\Vert _{\frac{n(2n+1)}{n+1}} \end{aligned}$$ ∫ H n ∏ j = 1 2 n f j ( π j ( p ) ) d p ≲ ∏ j = 1 2 n ‖ f j ‖ n ( 2 n + 1 ) n + 1 for all nonnegative measurable functions $$f_1,\ldots ,f_{2n}$$ f 1 , … , f 2 n on $$\mathbb {R}^{2n}$$ R 2 n . These inequalities and their geometric corollaries are thus ultimately based on planar geometry. Among the applications of Loomis–Whitney inequalities in $$\mathbb {H}^n$$ H n , we mention the following sharper version of the classical geometric Sobolev inequality in $$\mathbb {H}^n$$ H n : $$\begin{aligned} \Vert u\Vert _{\frac{2n+2}{2n+1}} \lesssim \prod _{j=1}^{2n}\Vert X_ju\Vert ^{\frac{1}{2n}}, \qquad u \in BV(\mathbb {H}^n), \end{aligned}$$ ‖ u ‖ 2 n + 2 2 n + 1 ≲ ∏ j = 1 2 n ‖ X j u ‖ 1 2 n , u ∈ B V ( H n ) , where $$X_j$$ X j , $$j=1,\ldots ,2n$$ j = 1 , … , 2 n , are the standard horizontal vector fields in $$\mathbb {H}^n$$ H n . Finally, we also establish an extension of the Loomis–Whitney inequality in $$\mathbb {H}^n$$ H n , where the Heisenberg vertical coordinate projections $$\pi _1,\ldots ,\pi _{2n}$$ π 1 , … , π 2 n are replaced by more general families of mappings that allow us to apply the same inductive approach based on the $$L^{3/2}$$ L 3 / 2 -$$L^3$$ L 3 boundedness of an operator in the plane.
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