Loomis-Whitney inequalities in Heisenberg groups
Abstract
This note concerns Loomis-Whitney inequalities in Heisenberg groups Hn: |K| Πj=12n|πj(K)|n+1n(2n+1), K ⊂ Hn. Here πj, j=1,…,2n, are the vertical Heisenberg projections to the hyperplanes \xj=0\, respectively, and |·| refers to a natural Haar measure on either Hn, or one of the hyperplanes. The Loomis-Whitney inequality in the first Heisenberg group H1 is a direct consequence of known Lp improving properties of the standard Radon transform in R2. 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 H1. The same approach, combined with multilinear interpolation, also yields the following strong type bound: ∫Hn Πj=12n fj(πj(p))\;dp Πj=12n \|fj\|n(2n+1)n+1 for all nonnegative measurable functions f1,…,f2n on R2n. These inequalities and their geometric corollaries are thus ultimately based on planar geometry. Among the applications of Loomis-Whitney inequalities in Hn, we mention the following sharper version of the classical geometric Sobolev inequality in Hn: \|u\|2n+22n+1 Πj=12n\|Xju\|12n, u ∈ BV(Hn), where Xj, j=1,…,2n, are the standard horizontal vector fields in Hn.
Turn this paper into a lesson
ArcXiv compiles a structured reading guide from this paper's metadata: plain-English importance, contributions, prerequisite concepts, which sections to read first, flashcards, and a quiz. Grounded in the abstract, never invented.