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\begin{document}

\section{Sharpening the physics case for charm physics at SuperB}

\subsection{Executive summary}
F.M.Vidal

\subsection{Theoretical Introduction}
I.Bigi: about  2 pages.

\subsection{Review of D Mixing at the Upsilon and at Threshold}
D.Asner: 
\begin{itemize}
\item
  comparison with other charm physics experiments (BES,CLEO,
etc.), 
\item
  evaluation of possibilities at threshold vs Upsilon running:
threshold will give a model independent way of determine the strong
phase. 
\item
 At threshold  time dependent CPV measurement can also be done since 
 $\sigma (t) ~ \tau_D$).
\end{itemize}

\subsection{CPV}

  \subsubsection{CPV in Mixing at the Upsilon and at Threshold }
  F.Martinez Vidal, A.Oyanguren: Semileptonic and adronc decays at
  threshold and Upsilon.

  \subsubsection{CPV in interference between mixing and decays}
  G.Simi: decays into CP egenstates
\begin{itemize}
\item
  contact BaBar authors: Chavez,
  Carlos A.; Coleman, Jonathon; Cowan, Ray; Flood, Kevin; Lockman,
  William; Petersen, Brian). 
\item
  Golden mode is D->KK ( can use D->pipi,
  Ksrho, while KsPhi can have ~10\% contribution from f0
  resonance). 
\item
  This is to be done at Y4S.
\end{itemize}

  \subsubsection{CPV in decay}
  A.Palano[TBC]: double cabibbo suppressed decays.

  \subsubsection{T odd correlations}
  A.Palano: $D->K K\pi\pi$ angular correlations.

\subsection{Mixing and CPV in 3 body decays}
N.Neri, G.Batignani: threshold vs Upsilon for Dalitz model systematics,
feasibility of the model independent measurement.
\begin{itemize}
\item
Need to understand how to keep under control the dalitz model systematic.
\item
CPV measurement can be competitive with D->KK. 
\item
Systematic errors in this analysis are different from other analysis
(like lietime ratio)
\item 
take the current babar dalitz model, generate toy MC event, count
number of events in the various bins, then estimate the sensitivity on
strong phase



\end{itemize}

\end{document}
