%&latex209
\documentstyle[amssymb,amsfonts]{amsart}

% \usepackage{amsmath}
% \usepackage{amsthm}
% \usepackage{amsfonts}
% \usepackage{amssymb}


% \newcommand*{\Rd}{\ensuremath{\mathbb{R}}}                  % reals
\newcommand{\norm}[1]{ \left|  #1 \right| }
\newcommand{\Ecal}{{\cal E}}
\newcommand{\Tcal}{{\cal T}}
\newcommand{\ifof}{\Leftrightarrow}
\newcommand{\Norm}[1]{ \left\| #1 \right\| }
\renewcommand{\Re}{{\mbox{Re}}}
\def\be#1{\begin{equation} \label{#1}}
\def\bs{\begin{split}}
\def\bi{\begin{itemize}}
\def\ei{\end{itemize}}
\def\es{\end{split}}
\def\ba{\begin{align}}
\def\bas{\begin{align*}}
\def\ea{\end{align}}
\def\eas{\end{align*}}
\def\grad{\nabla}
\def\R{{\mbox{\bf R}}}
\def\Q{{\mbox{\bf Q}}}
\def\T{{\mbox{\bf T}}}
\def\m{m}
\def\dist{{\mbox{\rm dist}}}
\def\diam{{\mbox{\rm diam}}}
\def\supp{{\mbox{\rm supp}}}
\def\B{{\cal B}}
\def\C{{\cal C}}
\def\Qcal{{\cal Q}}
\def\K{{\mbox{\bf K}}}
\def\D{{\mbox{\bf D}}}
\def\Z{{\mbox{\bf Z}}}
\def\eps{\varepsilon}
\def\pp{{p^\prime}}
\def\ppt{{\tilde p^\prime}}
\def\np{{n^\prime}}
\def\qp{{q^\prime}}
\def\lp{{l^\prime}}
\def\Qp{{Q^\prime}}
\def\PT{{\prod_{t=1}^2}}
\def\qpt{{\tilde q^\prime}}
\def\kp{{k^\prime}}
\def\mP{{m^\prime}}
\def\x{{\underline{x}}}
\newcommand{\qtil}{{\tildeq}}
\newcommand{\ktil}{{\tilde{k}}}
\newcommand{\ptil}{{\tilde{p}}}
\newcommand{\uxi}{{\overline{\xi}}}
% \def\lesssim{<_\sim}
\def\emph#1{{\it #1}}
\def\textbf#1{{\bf #1}}
\newenvironment{proof}{\noindent {\bf Proof} }{\endprf\par}
\def \endprf{\hfill  {\vrule height6pt width6pt depth0pt}\medskip}

% \swapnumbers
% \pagestyle{headings}

\theoremstyle{plain}
  \newtheorem{theorem}[subsection]{Theorem}
  \newtheorem{proposition}[subsection]{Proposition}
  \newtheorem{lemma}[subsection]{Lemma}
  \newtheorem{corollary}[subsection]{Corollary}
  \newtheorem{conjecture}[subsection]{Conjecture}
  \newtheorem{problem}[subsection]{Problem}

\theoremstyle{remark}
  \newtheorem{remark}[subsection]{Remark}
  \newtheorem{remarks}[subsection]{Remarks}

\theoremstyle{definition}
  \newtheorem{definition}[subsection]{Definition}

\include{psfig}

\begin{document}

\title[$L^p$ non-invertibility]{$L^p$ non-invertibility of frame operators}

\author{Terence Tao}
\address{Department of Mathematics, UCLA, Los Angeles, CA 90024}
\email{tao@@math.ucla.edu}

\subjclass{42B}
\begin{abstract}
We give an example of an operator of the form 
$$ T f = \sum_{j,k} \langle f, \Psi_{j,k} \rangle \Psi_{j,k},$$
where $\Psi$ is a pseudo-wavelet,
which is bounded and invertible on $L^2$ but not on $L^p$ for any specified $1 < p < 2$.  
\end{abstract}

\maketitle

\section{Introduction}

Fix $1 < p < 2$.  Let $\psi$ be a smooth compactly supported mother wavelet (the exact choice of which is unimportant), and let
$$ \psi_{j,k}(x) = 2^{-j/2} \psi(2^{-j}x-k)$$
be the associated orthonormal basis of $L^2$.  Define
$$ \Psi = \psi_{0,0} - \alpha \psi_{-1,0}$$
where $0 < \alpha < 1$ is given by
$$ \alpha = 2^{\frac{1}{2} - \frac{1}{p}}.$$
Note that
$$ \| \psi_{j,k} \|_p = \alpha^{-j} \| \psi_{0,0} \|_p.$$
Also, if we define
$$ \Psi_{j,k}(x) = 2^{-j/2} \Psi(2^{-j}x-k)$$
then we have
$$ \Psi_{j,k} = \psi_{j,k} - \alpha \psi_{j-1,2k}.$$
Clearly
$$ (1-\alpha) \|f\|_2 \leq (\sum_{j,k} |\langle f, \Psi_{j,k} \rangle|^2)^{1/2} \leq (1+\alpha) \|f\|_2$$
so the $\Psi_{j,k}$ form a frame.

Let $N$ be a large integer and define
$$ f = \sum_{i=0}^N \alpha^i \psi_{i,0}.$$
From the Littlewood-Paley theory for $\psi$ we have
$$ \|f\|_p \sim \| (\sum_{i=0}^N \alpha^{2i} |\psi_{i,0}|^2)^{1/2} \|_p
\sim N^{1/p}$$
as an easy calculation shows.

On the other hand, we have
$$ \langle f, \Psi_{0,0} \rangle = 1$$
$$ \langle f, \Psi_{N+1,0} \rangle = -\alpha^{N+1}$$
and that $\langle f, \Psi_{j,k} \rangle = 0$ for all other $\Psi_{j,k}$.  Thus
$$ \sum_{j,k} \langle f, \Psi_{j,k} \rangle \Psi_{j,k} = \Psi_{0,0} - \alpha^{N+1} \Psi_{N+1,0}.$$
Thus
$$ \| \sum_{j,k} \langle f, \Psi_{j,k} \rangle \Psi_{j,k} \|_p \lesssim 1.$$
Thus we see that the operator
$$ f \mapsto \sum_{j,k} \langle f, \Psi_{j,k} \rangle \Psi_{j,k}$$
is not invertible on $L^p$, even though it is invertible on $L^2$.
(In particular, the inverse of this operator is not a Calder\'on-Zygmund operator).

The author thanks Amos Ron for discussions which originated this problem, and for pointing out some errors in the original version of this note.

%\begin{thebibliography}{10}
%\end{thebibliography}

\end{document}
\endinput

