\section{Induction Linacs}
The muons drift first to spread out in time. The induction linacs then
decelerate the early particles and accelerate the later ones. Three
induction linacs are used with lengths of 100, 80 and 80~m, in a system
that reduces distortion in the phase space of the rotated muon bunch
and allows the induction linacs to operate with unipolar pulses. One
additional feature of this design is that the 1.25~T transport
solenoids are placed inside of the induction cores to avoid saturation
of the ferrites. The induction linac units are similar to those
being built for the DARHT project~\cite{CPR:indref1}; technical details
are discussed in Chapter~\ref{IND:LINAC}.

Figure~\ref{CPR:indfg1} shows the pulse shapes of three induction
linacs and Fig.~\ref{CPR:indfg2} depicts a cross section of two units
of the induction linac. The gaps in the solenoidal focusing, which lead to the periodicity described in Section~\ref{DandPR:drift}, are apparent.
\begin{figure}[!hbt]
\begin{center}
%\hskip.2in
\input{ind2-new.fig}
\caption[Pulse shapes of the induction linacs]{Pulse shapes of the three induction linacs.}
\label{CPR:indfg1}
\end{center}
\end{figure}

\begin{figure}[!hbt]
\begin{center}
\includegraphics[width=5in]{../template/report/ps-and-eps/induction.eps}
\caption{Cross section of two induction units.}
\label{CPR:indfg2}
\end{center}
\end{figure}