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Wavelets and Geometric Structure forFunction Spaces
Authors:Qi?Xiang?Yang  author-information"  >  author-information__contact u-icon-before"  >  mailto:Yangqi@public.wh.hb.cn"   title="  Yangqi@public.wh.hb.cn"   itemprop="  email"   data-track="  click"   data-track-action="  Email author"   data-track-label="  "  >Email author
Affiliation:(1) Department of Mathematics, Wuhan University, Wuhan, 430072, P. R. China
Abstract:Abstract With Littlewood–Paley analysis, Peetre and Triebel classified, systematically, almost all the usual function spaces into two classes of spaces: Besov spaces $$
ifmmodeexpandafterdotelseexpandafter.fi{B}^{{s,q}}_{p} {left( {s in R,0 < p,q leqslant infty } right)}
$$ and Triebel–Lizorkin spaces $$
ifmmodeexpandafterdotelseexpandafter.fi{F}^{{s,q}}_{p} {left( {s in R,0 < p < infty ,0 < q leqslant infty } right)}
$$ ; but the structure of dual spaces $$
ifmmodeexpandafterdotelseexpandafter.fi{D}^{{s,q}}_{p} 
$$ of $$
ifmmodeexpandafterdotelseexpandafter.fi{F}^{{s,q}}_{p} {left( {s in R,0 < p leqslant 1 leqslant q leqslant infty } right)}
$$ is very different from that of Besov spaces or that of Triebel–Lizorkin spaces, and their structure cannot be analysed easily in the Littlewood–Paley analysis. Our main goal is to characterize $$
ifmmodeexpandafterdotelseexpandafter.fi{D}^{{s,q}}_{p} {left( {s in R,0 < p = 1 leqslant q leqslant infty } right)}
$$ in tent spaces with wavelets. By the way, some applications are given: (i) Triebel–Lizorkin spaces for p = ∞ defined by Littlewood–Paley analysis cannot serve as the dual spaces of Triebel–Lizorkin spaces for p = 1; (ii) Some inclusion relations among these above spaces and some relations among $$
ifmmodeexpandafterdotelseexpandafter.fi{B}^{{0,q}}_{1} ,{kern 1pt} {kern 1pt} ifmmodeexpandafterdotelseexpandafter.fi{F}^{{0,q}}_{1} 
$$ and L 1 are studied. Supported by NNSF of China (Grant No. 10001027)
Keywords:Triebel–  Lizorkin spaces  Dual spaces  Wavelets
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