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Patrick Janot edited Measurements at the Z pole.tex
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\subsection{Measurements with TeraZ}
With a continuous luminosity of $5\times 10^{35} \cms$ per IP at a centre-of-mass of
90 91 GeV, TLEP is a
Z-factory Z factory able to deliver $7\times 10^{11}$ visible Z decays for one year of running, with very clean experimental conditions, centre-of-mass energy known to a fraction of
MeV MeV, and the possibility of longitudinally polarized
beams. This allows beams, with which the following experiments
to can be carried
out. out:
\begin{itemize}
\item
A precise a high-statistics line-shape scan of the Z
resonance resonance, allowing
a precise determination of the Z mass and width;
\item
High high statistics data collection at the Z
peak; peak, towards the measurement of the Z partial widths, the determination of the number of light neutrinos, and the detection of rare decays;
\item
Data high-statistics data taking with
longitudinally polarized beams. longitudinally-polarized beams, enable a precise determination of the weak mixing angle.
\end{itemize}
An extensive description of Electroweak measurements performed at LEP and SLC in 1988-1998 can be found
in~\cite{ements_on_the_Z_resonance_2006}. in Ref.~\cite{ements_on_the_Z_resonance_2006}. It is beyond the scope of this article to revisit all the measurements to establish the improvements brought about by TLEP, and we limit ourselves to a few key measurements. The typical improvement in statistics over the LEP experiments being a factor $10^5$ (a factor 300 reduction in statistical errors!) it is clear that a detailed consideration of systematic errors will be essential before a precise conclusion will be drawn on the achievable precisions. In addition, uncertainties in the theoretical interpretation will need to be revisited, this implying a significant new program of calculations of higher order Electroweak corrections.