\chapter{The \LHCb experiment}
\label{chap:MoreStuff}

\chapterquote{There, sir! that is the perfection of vessels!}
{Jules Verne, 1828--1905}

\section{The \LHC}
The Large Hadron Collider (\LHC) at \CERN is a new hadron collider,
located in the same tunnel as the Large Electron-Positron collider 
(\LEP)~\cite{Brianti:2004qq}. Where \LEP's chief task was the use 
of \unit{90--207}{\GeV} \epluseminus collisions to establish the 
precision physics of electroweak unification\dots

\begin{figure}
  \includegraphics[width=\largefigwidth]{ckmfitter-alpha-combined}
  \caption[CKM Fitter constraints on \alphaCKM.]%
  {CKM Fitter constraints on \alphaCKM from combined \BToPiPi, 
    \BToRhoPi and \BToRhoRho decay analyses.}
  \label{fig:CKMFitter}
\end{figure}

\section{The \LHCb experiment}
\label{sec:LHCbInDetail}

Since both \bhadron{s} are preferentially produced in the same direction 
and are forward-boosted along the beam-pipe, the detector is not required 
to have full $4\pi$ solid-angle coverage. \LHCb takes advantage of this 
by using a wedge-shaped single-arm detector with angular acceptance 
\unit{10-300}{\mrad} in the horizontal (bending) plane~\cite{Amato:1998xt}.

\vspace{1cm}

\begin{center}
{\hspace{1mm}\Large\vdots\hspace{1cm}}
\end{center}

\vspace{1cm}

The detector is illustrated in \FigureRef{fig:LHCbCrossSection}, showing 
the overall scale of the experiment and the surrounding cavern structure.

\begin{sidewaysfigure}
  %\begin{center}
  \includegraphics[width=0.8\textheight]{lhcb-detector-cross-section}
  \caption[Cross-section view of \LHCb, cut in the non-bending $y-z$ plane]%
    {Cross-section view of \LHCb, cut in the non-bending $y-z$ plane.}
  \label{fig:LHCbCrossSection}
  %\end{center}
\end{sidewaysfigure}

The single-sided detector design was chosen in preference to a two-armed
design since the detector dimensions are restricted by the layout of the 
IP8 (ex-Delphi) cavern in which \LHCb is located. Using all the available 
space for a single-arm spectrometer more than compensates in performance 
for the \about{50\percent} drop in luminosity.

\section{The \Cerenkov mechanism}
A Huygens construction in terms of spherical shells of probability for photon
emission as the particle progresses along its track shows an effective
``shock-front'' of \Cerenkov emission. This corresponds to an emission cone of
opening angle \thetaCerenkov around the momentum vector for each point on the
track,
%
\begin{subequations}
  \label{eq:cosThetaCk}
  \begin{equation}
    \cos\,\thetaCerenkov  &= \frac{1}{n \beta} + 
                             \frac{\hbar k}{2p}%
                             \parenths{ 1 - \frac{1}{n^2} } \\
                          &\,\sim \frac{1}{n \beta}%
    \label{eq:cosThetaCkApprox}
  \end{equation}
\end{subequations}
%
where $\beta \equiv v/c$, the relativistic velocity fraction,

\section{Trigger system}
\label{sec:triggers}
An overview of the \LHCb trigger characteristics broken down by level
is shown in \Table~\ref{tab:TriggerDetails}:

\begin{table}
  \begin{tabular}{lllll}
                & L0              & L1              & HLT             \\
    \midrule
    Input rate  & \unit{40}{\MHz} & \unit{1}{\MHz}  & \unit{40}{\kHz} \\
    Output rate & \unit{1}{\MHz}  & \unit{40}{\kHz} & \unit{2}{\kHz}  \\
    Location    & On detector     & Counting room   & Counting room   \\
  \end{tabular}
  \caption{Characteristics of the trigger levels and offline analysis.}
  \label{tab:TriggerDetails}
\end{table}