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The key is a chamber lifting: fix a closed Weyl chamber $\mathcal C$ and set $Uf(x)=(f(\sigma_1x),\dots,f(\sigma_{|G|}x))$ for $x\in\mathcal C$. This identifies $L^p(\mathbb{R}^N,d\omega)$ with $L^p(\mathcal C,d\omega;\ell_{|G|}^p)$. Under this lifting, the orbit singularity becomes the ordinary diagonal on $\mathcal C$ and the commutator becomes a finite matrix singular integral on $\mathcal C$. We construct it via heat-scale regularizations, prove component $T1$ testing for chamber indicators, and then apply scalar Calderón--Zygmund theory to obtain the $L^p$ bounds.
| Comments: | 51 pages |
| Subjects: | Classical Analysis and ODEs (math.CA) |
| MSC classes: | 42B35 |
| Cite as: | arXiv:2605.25808 [math.CA] |
| (or arXiv:2605.25808v1 [math.CA] for this version) | |
| https://doi.org/10.48550/arXiv.2605.25808 arXiv-issued DOI via DataCite (pending registration) |
From: Liangchuan Wu [view email]
[v1]
Mon, 25 May 2026 13:01:43 UTC (46 KB)
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