\begin{sidewaystable*}[!htp]
\begin{center}
\begin{tabular}{|c|c|c|cccc|} 
\hline 
Data  & Time resolution & Mistag & $\sigma(x)$ & $\sigma(y)$ & $\sigma(\phi)$ & $\sigma(|q/p|)$ \\ 
\hline
LB $\Psi(3770)$               & Perfect               & 0   & 0.00076 & 0.00044 & 0.077 & 0.031 \\
LB $\Psi(3770)$ large mixing  & Perfect               & 0   & 0.00059 & 0.00043 & 0.007 & 0.003 \\
LB $\Psi(3770)$ no CPV        & Perfect               & 0   & 0.00081 & 0.00027 & 0     & 0 \\
LB $\Psi(3770)$               & HB TG (0.25/0.20~ps)  & 0   & 0.00098 & 0.00046 & 0.077 & 0.034 \\
LB $\Psi(3770)$               & IB TG (0.40/0.28~ps)  & 0   & 0.00100 & 0.00051 & 0.078 & 0.035 \\
LB $\Psi(3770)$               & LB TG (0.66/0.39~ps)  & 0   & 0.00104 & 0.00054 & 0.103 & 0.037 \\
LB $\Psi(3770)$               & VLB TG (1.27/0.76~ps) & 0   & 0.00107 & 0.00067 & 0.149 & 0.061 \\
HB $\Psi(3770)$               & HB TG (0.25/0.20~ps)  & 0   & 0.00118 & 0.00056 & 0.093 & 0.041 \\  % taken from LB Psi HB TG scaling by relative geo efficiency, eff_0.3/eff_0.91=0.66/0.45=1.467
IB $\Psi(3770)$               & IB TG (0.40/0.28~ps)  & 0   & 0.00108 & 0.00054 & 0.084 & 0.037 \\  % taken from LB Psi IB TG scaling by relative geo efficiency, eff_0.56/eff_0.91=0.66/0.57=1.158
LB $\Psi(3770)$               & Perfect               & 2\% & 0.00210 & 0.00062 & 0.119 & 0.097 \\
\hline
$\Upsilon(4S)$                & Perfect               & 0   & 0.00021 & 0.00007 & 0.012 & 0.005 \\
$\Upsilon(4S)$ large mixing   & Perfect               & 0   & 0.00010 & 0.00008 & 0.001 & 0.001 \\
$\Upsilon(4S)$ no CPV         & Perfect               & 0   & 0.00012 & 0.00004 & 0     & 0 \\
$\Upsilon(4S)$                & TG (0.17/0.10~ps)     & 0   & 0.00017 & 0.00008 & 0.014 & 0.005 \\
$\Upsilon(4S)$                & Perfect               & 2\% & 0.00030 & 0.00011 & 0.019 & 0.014 \\
\hline 
\end{tabular} 
\caption{Estimated sensitivities for the mixing and CP violating parameters as determined from combined fits to all two-body double tags available at 
$\Psi(3770)$ and $\Upsilon$, using the expected number of events and proper time resolution as a function of the reconstructed decays from Table~\ref{tab:final_states_list2}.
``LB $\Psi(3770)$'', ``IB $\Psi(3770)$'' and ``HB $\Psi(3770)$'' data refer to the low ($\beta\gamma=0.238$), intermediate ($\beta\gamma=0.56$) and
high ($\beta\gamma=0.91$) boost number of events, given in the 3rd, 4th and 5th columns, respectively, in Table~\ref{tab:final_states_list2}. According
to Figure~\ref{fig:eff_vs_bg_kpikpi}, the expected number of events is approximately stable for $\beta\gamma$ in the range between 0.15 and 0.3.
``HB TG'', ``IB TG'', ``LB TG'' and ``VLB TG'' refer to the high ($\beta\gamma=0.91$), intermediate ($\beta\gamma=0.56$), low ($\beta\gamma=0.3$) 
and very low ($\beta\gamma=0.15$) triple Gaussian proper time resolution at $\Psi(3770)$ as estimated from FastSim and reported in 
Figure~\ref{fig:aveDeltaTErr_vs_bg_kpikpi}. The numbers in parenthesis are the total and core rms resolutions.
The ``large mixing'' configuration has been generated with $x$ and $y$ values 10 times larger than the nominal (HFAG) values.
%
The reported (rms) sensitivities for the mixing and CP violating parameters have been scaled to the complete expected SuperB data
by scaling by $\sqrt{10}$ and $\sqrt{200}$ the rms results from the Toy Monte Carlo experiments.
} 
\label{tab:final_sensitivities} 
\end{center}
\end{sidewaystable*} 
