English

On directional Whitney inequality

Numerical Analysis 2021-04-08 v2 Numerical Analysis Classical Analysis and ODEs

Abstract

This paper studies a new Whitney type inequality on a compact domain ΩRd\Omega\subset {\mathbb{R}}^d that takes the form infQΠr1d(E)fQpC(p,r,Ω)ωEr(f,diam(Ω))p,  rN,  0<p,\inf_{Q\in \Pi_{r-1}^d({\mathcal{E}})} \|f-Q\|_p \leq C(p,r,\Omega) \omega_{{\mathcal{E}}}^r(f,{\rm diam}(\Omega))_p,\ \ r\in {\mathbb{N}},\ \ 0<p\leq \infty, where ωEr(f,t)p\omega_{{\mathcal{E}}}^r(f, t)_p denotes the rr-th order directional modulus of smoothness of fLp(Ω)f\in L^p(\Omega) along a finite set of directions ESd1{\mathcal{E}}\subset {\mathbb{S}^{d-1}} such that span(E)=Rd{\rm span}({\mathcal{E}})={\mathbb{R}}^d, Πr1d(E):={gC(Ω): ωEr(g,diam(Ω))p=0}\Pi_{r-1}^d({\mathcal{E}}):=\{g\in C(\Omega):\ \omega^r_{\mathcal{E}} (g, {\rm diam} (\Omega))_p=0\}. We prove that there does not exist a universal finite set of directions E{\mathcal{E}} for which this inequality holds on every convex body ΩRd\Omega\subset {\mathbb{R}}^d, but for every connected C2C^2-domain ΩRd\Omega\subset {\mathbb{R}}^d, one can choose E{\mathcal{E}} to be an arbitrary set of dd independent directions. We also study the smallest number Nd(Ω)N{\mathcal{N}}_d(\Omega)\in{\mathbb{N}} for which there exists a set of Nd(Ω){\mathcal{N}}_d(\Omega) directions E{\mathcal{E}} such that span(E)=Rd{\rm span}({\mathcal{E}})={\mathbb{R}}^d and the directional Whitney inequality holds on Ω\Omega for all rNr\in{\mathbb{N}} and p>0p>0. It is proved that Nd(Ω)=d{\mathcal{N}}_d(\Omega)=d for every connected C2C^2-domain ΩRd\Omega\subset {\mathbb{R}}^d, for d=2d=2 and every planar convex body ΩR2\Omega\subset {\mathbb{R}}^2, and for d3d\ge 3 and every almost smooth convex body ΩRd\Omega\subset {\mathbb{R}}^d. [See the pre-print for the complete abstract - not included here due to arXiv limitations.]

Keywords

Cite

@article{arxiv.2010.08374,
  title  = {On directional Whitney inequality},
  author = {Feng Dai and Andriy Prymak},
  journal= {arXiv preprint arXiv:2010.08374},
  year   = {2021}
}

Comments

the material in this article is based heavily on a part of arXiv:1910.11719

R2 v1 2026-06-23T19:24:11.729Z