English

Type and cotype with respect to arbitrary orthonormal systems

Functional Analysis 2016-09-06 v1

Abstract

Let \onk\nz\on_{k \in \nz} be an orthonormal system on some σ\sigma-finite measure space (\Om,p)(\Om,p). We study the notion of cotype with respect to Φ\Phi for an operator TT between two Banach spaces XX and YY, defined by \fcoT:=inf\fco T := \inf cc such that \Tfmm\pl\plc\pll\gmm\mboxforall(xk)X\pl, \Tfmm \pl \le \pl c \pll \gmm \hspace{.7cm}\mbox{for all}\hspace{.7cm} (x_k)\subset X \pl, where (gk)k\nz(g_k)_{k\in \nz} is a sequence of independent and normalized gaussian variables. It is shown that this Φ\Phi-cotype coincides with the usual notion of cotype 22 iff \linebreak \fcoI\linnlog(n+1)\fco {I_{\lin}} \sim \sqrt{\frac{n}{\log (n+1)}} uniformly in nn iff there is a positive η>0\eta>0 such that for all n\nzn \in \nz one can find an orthonormal Ψ=(ψl)1nspan{ϕk\p\pk\nz}\Psi = (\psi_l)_1^n \subset {\rm span}\{ \phi_k \p|\p k \in \nz\} and a sequence of disjoint measurable sets (Al)1n\Om(A_l)_1^n \subset \Om with Al\betψl\rag2dp\pl\plη\mboxforalll=1,...,n\pl. \int\limits_{A_l} \bet \psi_l\rag^2 d p \pl \ge \pl \eta \quad \mbox{for all}\quad l=1,...,n \pl. A similar result holds for the type situation. The study of type and cotype with respect to orthonormal systems of a given length provides the appropriate approach to this result. We intend to give a quite complete picture for orthonormal systems in measure space with few atoms.

Cite

@article{arxiv.math/9401205,
  title  = {Type and cotype with respect to arbitrary orthonormal systems},
  author = {Stefan Geiss and Marius Junge},
  journal= {arXiv preprint arXiv:math/9401205},
  year   = {2016}
}