renamed all files for ALICE-INT-2012-040 with corresponding prefix

[u/mrichter/AliRoot.git] / PWGLF / FORWARD / doc / alice-int-2012-040.tex

\documentclass[11pt]{article}
\usepackage{pwglfforward}
\title{%
  {\LARGE EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH}\\%
  {\Large European Organization for Particle Physics}\\[2ex]%
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        {\LARGE\bf Analysing the FMD data for $\dndeta$}%
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        \hfill ALICE--INT--2012--040 v2\\
        \hfill \today%
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\author{Christian Holm
  Christensen\thanks{\texttt{$\langle$cholm@nbi.dk$\rangle$}}\quad\&\quad
  Hans Hjersing Dalsgaard\thanks{\texttt{$\langle$canute@nbi.dk$\rangle$}}\\ 
  Niels Bohr Institute\\
  University of Copenhagen}
\date{}
\begin{document}
\pdfbookmark{Analysing the FMD data for dN/deta}{top}
\maketitle 

\tableofcontents 
\section{Introduction}

This document describes the steps performed in the analysis of the
charged particle multiplicity in the forward pseudo--rapidity regions
with the \FMD{} detector \cite{FWD:2004mz,cholm:2009}. The document
also include a summary (see section \ref{prelim}) of the request for
preliminary figures for the measurement of $\dndeta$ with
SPD\cite{ruben,Aamodt:2010cz}, VZERO\cite{maxime}, and FMD.
%  The primary detector used for this is the \FMD{}

The \FMD{} is organised in 3 \emph{sub--detectors} \FMD{1}, \FMD{2},
and \FMD{3}, each consisting of 1 (\FMD{1}) or 2 (\FMD{2} and~3)
\emph{rings}.  The rings fall into two types: \emph{Inner} or
\emph{outer} rings.  Each ring is in turn azimuthally divided into
\emph{sectors}, and each sector is radially divided into
\emph{strips}.  How many sectors, strips, as well as the $\eta$
coverage is given in \tablename~\ref{tab:fmd:overview}.

\begin{table}[htbp]
  \begin{center}
    \caption{Physical dimensions of Si segments and strips.}
    \label{tab:fmd:overview}
    \vglue0.2cm
    \begin{tabular}{|c|cc|cr@{\space--\space}l|r@{\space--\space}l|}
      \hline
      \textbf{Sub--detector/} &
      \textbf{Azimuthal}&
      \textbf{Radial} &
      $z$ &
      \multicolumn{2}{c|}{\textbf{$r$}} &
      \multicolumn{2}{c|}{\textbf{$\eta$}} \\ 
      \textbf{Ring}&  
      \textbf{sectors} &
      \textbf{strips} & 
      \textbf{[cm]} &
      \multicolumn{2}{c|}{\textbf{range [cm]}} &
      \multicolumn{2}{c|}{\textbf{coverage}} \\
      \hline
      FMD1i & 20& 512& 320  &  4.2& 17.2& 3.68&  5.03\\
      FMD2i & 20& 512&  83.4&  4.2& 17.2& 2.28&  3.68\\
      FMD2o & 40& 256&  75.2& 15.4& 28.4& 1.70&  2.29\\
      FMD3i & 20& 512& -75.2&  4.2& 17.2&-2.29& -1.70\\
      FMD3o & 40& 256& -83.4& 15.4& 28.4&-3.40& -2.01\\
      \hline
    \end{tabular}
  \end{center}
\end{table}

The \FMD{} \ESD{} object contains the scaled energy deposited $\Delta
E/\Delta E_{mip}$ for each of the 51,200 strips.  This is determined
in the reconstruction pass.  The scaling to $\Delta E_{mip}$ is done
using calibration factors extracted in designated pulser runs.  In
these runs, the front-end electronics is pulsed with an increasing
known pulse size, and the conversion factor from ADC counts to $\Delta
E_{mip}$ is determined \cite{cholm:2009}.

The \SPD{} is used for determination of the position of the primary
interaction point except in the case of displaced vertex analysis as
discussed in section \ref{sec:sub:sub:dispvtx}.

The analysis is performed as a two--step process.  
\begin{enumerate}
\item The Event--Summary--Data (\ESD{}) is processed event--by--event
  and passed through a number of algorithms, and
  $\dndetadphi$ for each event is output to an Analysis--Object--Data
  (\AOD{}) tree (see \secref{sec:gen_aod}).
\item The \AOD{} data is read in and the sub--sample of the data under
  investigation is selected (e.g., \INEL{}, \INELONE{}, \NSD{} in p+p data, or
  some centrality class in Pb+Pb data) and the $\dndetadphi$ histogram read for
  those events to build up $\dndeta$ (see \secref{sec:ana_aod}).
\end{enumerate}
The details of each step above will be expanded upon in the
following. 

In Appendix~\ref{app:nomen} is an overview of the nomenclature used in
this document.

\section{Generating $\dndetadphi[i]$ event--by--event}
\label{sec:gen_aod}

When reading in the \ESD{}s and generating the $\dndetadphi$
event--by--event the following steps are taken (in order) for each
event $i$ and FMD ring $r$.
\begin{description}
\item[Event inspection] The global properties of the event is
  determined, including the trigger type and primary interaction
  point\footnote{`Vertex' and `primary interaction point' will be used
    interchangeably in the text, since there is no ambiguity with
    particle production vertex in this analysis.} $z$ coordinate (see
  \secref{sec:sub:event_inspection}).
\item[Sharing filter] The \ESD{} object is read in and corrected for
  sharing.  The result is a new \ESD{} object (see
  \secref{sec:sub:sharing_filter}).
\item[Density calculator] The (possibly un--corrected) \ESD{} object
  is then inspected and an inclusive (primary \emph{and} secondary
  particles), per--ring charged particle density
  $\dndetadphi[incl,r,v,i]$ is made.  This calculation depends in
  general upon the interaction vertex position along the $z$ axis
  $v_z$ (see \secref{sec:sub:density_calculator}).
\item[Corrections] The 5 (one for each FMD ring)
  $\dndetadphi[incl,r,v,i]$ are corrected for secondary production and
  acceptance.  The correction for the secondary particle production is
  highly dependent on the vertex $z$ coordinate.  The result is a
  per--ring, charged primary particle density $\dndetadphi[r,v,i]$
  (see \secref{sec:sub:corrector}).
\item[Histogram collector] Finally, the 5 $\dndetadphi[r,v,i]$ are
  summed into a single $\dndetadphi[v,i]$ histogram, taking care of
  the overlaps between the detector rings.  In principle, this
  histogram is independent of the vertex, except that the
  pseudo--rapidity range, and possible holes in that range, depends on
  $v_z$ --- or rather the bin in which the $v_z$ falls (see
  \secref{sec:sub:hist_collector}).
\end{description}

Each of these steps will be detailed in the following. 

\subsection{Event inspection}
\label{sec:sub:event_inspection}

The first thing to do, is to inspect the event for triggers.  A number
of trigger bits, like \INEL{} (Minimum Bias for Pb+Pb), \INELONE{},
\NSD{}, and so on is then propagated to the \AOD{} output.

Just after the sharing filter (described below) but before any further
processing, the vertex information is queried.  If there is no vertex
information, or if the vertex $z$ coordinate is outside the
pre--defined range, then no further processing of that event takes
place.

\subsubsection{Displaced Vertices}
\label{sec:sub:sub:dispvtx}

The analysis can be set up to run on the `displaced vertices' that
occur during LHC Pb+Pb running. Details on the displaced vertices, and
their selection can be found in the VZERO analysis note \cite{maxime}.

\subsection{Sharing filter}
\label{sec:sub:sharing_filter}

A particle originating from the vertex can, because of its incident
angle on the \FMD{} sensors traverse more than one strip (see
\figref{fig:share_fraction}).  This means that the energy loss of the
particle is distributed over 1 or more strips.  The signal in each
strip should therefore possibly be merged with its neighboring strip
signals to properly reconstruct the energy loss of a single particle.

\begin{figure}[htbp]
  \centering
  \figinput[3cm]{share_fraction}
  \caption{A particle traversing 2 strips and depositing energy in
    each strip. }
  \label{fig:share_fraction}
\end{figure}

The effect is most pronounced in low--flux\footnote{Events with a low
  hit density.} events, like proton--proton collisions or peripheral
Pb--Pb collisions, while in high--flux events the hit density is so
high that most likely each and every strip will be hit and the effect
cancels out on average.

Since the particles travel more or less in straight lines toward the
\FMD{} sensors, the sharing effect is predominantly in the $r$ or
\emph{strip} direction.  Only neighbouring strips in a given sector are
therefore investigated for this effect.  

Algorithm~\ref{algo:sharing} is applied to the signals in a given
sector.

\begin{algorithm}[htpb]
  \belowpdfbookmark{Algorithm 1}{algo:sharing}
  \SetKwData{usedThis}{current strip used}
  \SetKwData{usedPrev}{previous strip used}
  \SetKwData{Output}{output}
  \SetKwData{Input}{input}
  \SetKwData{Nstr}{\# strips}
  \SetKwData{Signal}{current}
  \SetKwData{Eta}{$\eta$}
  \SetKwData{prevE}{previous strip signal} 
  \SetKwData{nextE}{next strip signal} 
  \SetKwData{lowFlux}{low flux flag} 
  \SetKwFunction{SignalInStrip}{SignalInStrip}
  \SetKwFunction{MultiplicityOfStrip}{MultiplicityOfStrip}
  \usedThis $\leftarrow$ false\;
  \usedPrev $\leftarrow$ false\;
  \For{$t\leftarrow1$ \KwTo \Nstr}{ 
    \Output${}_t\leftarrow 0$\;
    \Signal $\leftarrow$ \SignalInStrip($t$)\;

    \uIf{\Signal is not valid}{ 
      \Output${}_t \leftarrow$ invalid\;
    }
    \uElseIf{\Signal is 0}{ 
      \Output${}_t \leftarrow$ 0\;
    }
    \Else{
      \Eta$\leftarrow$ $\eta$ of \Input${}_t$\;
      \prevE$\leftarrow$ 0\;
      \nextE$\leftarrow$ 0\;
      \lIf{$t \ne 1$}{ 
        \prevE$\leftarrow$ \SignalInStrip($t-1$)\;
      }
      \lIf{$t \ne $\Nstr}{ 
        \nextE$\leftarrow$ \SignalInStrip($t+1$)\;
      }
      \Output${}_t\leftarrow$
      \MultiplicityOfStrip(\Signal,\Eta,\prevE,\nextE,\\
      \hfill\lowFlux,$t$,\usedPrev,\usedThis)\;
    }   
  }
  \caption{Sharing correction}
  \label{algo:sharing}
\end{algorithm}

Here the function \FuncSty{SignalInStrip}($t$) returns the properly
path--length corrected signal in strip $t$.  The function
\FuncSty{MultiplicityOfStrip} is where the real processing takes
place (see page \pageref{func:MultiplicityOfStrip}). 

\begin{function}[htbp]
  \belowpdfbookmark{MultiplicityOfStrip}{func:MultiplicityOfStrip}
  \caption{MultiplicityOfStrip(\DataSty{current},$\eta$,\DataSty{previous},\DataSty{next},\DataSty{low
      flux flag},\DataSty{previous signal used},\DataSty{this signal
      used})} 
  \label{func:MultiplicityOfStrip}
  \SetKwData{Current}{current} 
  \SetKwData{Next}{next} 
  \SetKwData{Previous}{previous} 
  \SetKwData{lowFlux}{low flux flag}
  \SetKwData{usedPrev}{previous signal used}
  \SetKwData{usedThis}{this signal used}
  \SetKwData{lowCut}{low cut}
  \SetKwData{total}{Total}
  \SetKwData{highCut}{high cut}
  \SetKwData{Eta}{$\eta$}  
  \SetKwFunction{GetHighCut}{GetHighCut}
  \If{\Current is very large or \Current $<$ \lowCut} {
    \usedThis $\leftarrow$ false\;
    \usedPrev $\leftarrow$ false\;
    \Return{0}
  }
  \If{\usedThis}{ 
    \usedThis $\leftarrow$ false\;
    \usedPrev $\leftarrow$ true\;
    \Return{0}
  }
  \highCut $\leftarrow$ \GetHighCut($t$,\Eta)\;
  %\If{\Current $<$ \Next and \Next $>$ \highCut and \lowFlux set}{ 
  %  \usedThis $\leftarrow$ false\;
  %  \usedPrev $\leftarrow$ false\;
  %  \Return{0}
  %}
  \total $\leftarrow$ \Current\;
  \lIf{\lowCut $<$ \Previous $<$ \highCut and not \usedPrev}{ 
    \total $\leftarrow$ \total + \Previous\;
  }
  \If{\lowCut $<$ \Next $<$ \highCut}{ 
    \total $\leftarrow$ \total + \Next\;  
    \usedThis $\leftarrow$ true\;
  }
  \eIf{\total $>$ 0}{ 
    \usedPrev $\leftarrow$ true\;
    \Return{\total}
  }{
    \usedPrev $\leftarrow$ false\;
    \usedThis $\leftarrow$ false\;
    \Return{0}
  }
\end{function}
Here, the function \FuncSty{GetHighCut} (see below) evaluates a fit to the energy
distribution in the specified $\eta$ bin (see also
\secref{sec:sub:density_calculator}).  It returns
$$
\Delta_{mp} - 2 w
$$
where $\Delta_{mp}$ is the most probable energy loss, and $w$ is the
width of the Landau distribution.  

The \KwSty{if} in line 5, says that if the previous strip was merged
with current one, and the signal of the current strip was added to
that, then the current signal is set to 0, and we mark it as used for
the next iteration (\DataSty{previous signal used}$\leftarrow$true).

% The \KwSty{if} in line 10 checks if the current signal is smaller than
% the next signal, if the next signal is larger than the upper cut
% defined above, and if we have a low--flux event\footnote{Note, that in
%   the current implementation there are never any low--flux events.}.
% If that condition is met, then the current signal is the smaller of
% two possible candidates for merging, and it should be merged into the
% next signal.  Note, that this \emph{only} applies in low--flux events.

In line 11, % 15, 
we test if the previous signal lies between our low and
high cuts, and if it has not been marked as being used.  If so, we add
it to our current signal.  

The next \KwSty{if} on line 12 % 16 
checks if the next signal is within our
cut bounds.  If so, we add that signal to the current signal and mark
it as used for the next iteration (\DataSty{this signal
  used}$\leftarrow$true).  It will then be put to zero on the next
iteration by the condition on line 6.

Finally, if our signal is still larger than 0, we return the signal
and mark this signal as used (\DataSty{previous signal
  used}$\leftarrow$true) so that it will not be used in the next
iteration. Otherwise, we mark the current signal and the next signal
as unused and return a 0. 


\subsection{Density calculator}
\label{sec:sub:density_calculator}

The density calculator loops over all the strip signals in the sharing
corrected\footnote{The sharing correction can be disabled, in which
  case the density calculator uses the input \ESD{} signals.} \ESD{}
and calculates the inclusive (primary + secondary) charged particle
density in pre--defined $\etaphi$ bins.

\subsubsection{Inclusive number of charged particles: Energy Fits} 
\label{sec:sub:sub:eloss_fits}

The number charged particles in a strip $\mult[,t]$ is calculated
using multiple Landau-like distributions fitted to the energy loss
spectrum of all strips in a given $\eta$ bin.
\begin{align}
  \Delta_{i,mp} &= i (\Delta_{1,mp}+ \xi_1 \log(i))\nonumber\\
  \xi_i         &= i\xi_1\nonumber\\
  \sigma_i      &= \sqrt{i}\sigma_1\nonumber\\
  \mult[,t]     &= \frac{\sum_i^{N_{max}}
    i\,a_i\,F(\Delta_t;\Delta_{i,mp},\xi_i,\sigma_i)}{
    \sum_i^{N_{max}}\,a_i\,F(\Delta_t;\Delta_{i,mp},\xi_i,\sigma_i)}\quad,
\end{align}
where $F(x;\Delta_{mp},\xi,\sigma)$ is the evaluation of the Landau
distribution $f_L$ with most probable value $\Delta_{mp}$ and width
$\xi$, folded with a Gaussian distribution with spread $\sigma$ at the
energy loss $x$ \cite{nim:b1:16,phyrev:a28:615}.
\begin{align}
  \label{eq:energy_response}
  F(x;\Delta_{mp},\xi,\sigma) = \frac{1}{\sigma \sqrt{2 \pi}}
  \int_{-\infty}^{+\infty} d\Delta' f_{L}(x;\Delta',\xi)
  \exp{-\frac{(\Delta_{mp}-\Delta')^2}{2\sigma^2}}\quad,
\end{align}
where $\Delta_{1,mp}$, $\xi_1$, and $\sigma_1$ are the parameters for
the first MIP peak, $a_1=1$, and $a_i$ is the relative weight of the
$i$-fold MIP peak.  The parameters $\Delta_{1,mp}, \xi_1,
\sigma_1, \mathbf{a} = \left(a_2, \ldots a_{N_{max}}\right)$ are
obtained by fitting 
$$
F_j(x;C,\Delta_{mp},\xi,\sigma,\mathbf{a}) = C 
\sum_{i=1}^{j} a_i F(x;\Delta_{i,mp},\xi_{i},\sigma_i) 
$$
for increasing $j$ to the energy loss spectra in separate $\eta$ bins.
The fit procedure is stopped when for $j+1$: (the default values for
each value are included below) 
\begin{itemize}
\item the reduced $\chi^2$ exceeds a certain threshold (usually 20), or
\item the relative error $\delta p/p$ of any parameter of the fit
  exceeds a certain threshold (usually 0.12), or 
\item when the weight $a_j+1$ is smaller than some number (typically
  $10^{-5}$). 
\end{itemize}
$N_{max}$ is then set to $j$.  Examples of the result of these fits
are given in \figref{fig:eloss_fits} in Appendix~\ref{app:eloss_fits}.
\subsubsection{Inclusive number of charged particles: Poisson Approach} 
\label{sec:sub:sub:poisson}
Another approach to the calculation of the number of charged particles
is using Poisson statistics. This is the default choice because it is
less sensitive to the stability of the fits required for the energy
fits method. 
Assume that in a region of the FMD % where
$\mult$ 
%is azimuthally uniform in $\eta$ intervals it 
is
distributed according to a Poisson distribution. This means that the
probability of $\mult=n$ becomes:
\begin{equation}
P(n) = \frac{\mu^n e^{-\mu}}{n!} \label{eq:PoissonDef}
\end{equation}
In particular the measured occupancy, $\mu_{meas}$, is the probability
of any number of hits, thus using \eqref{eq:PoissonDef} :
\begin{equation}
\mu_{meas} = 1 - P(0) = 1 - e^{-\mu } 
%\Rightarrow \mu = \ln
%(1 - \mu_{meas})^{-1} \label{eq:PoissonDef2}
\end{equation}
which implies:
\begin{equation}
\mu = \ln
(1 - \mu_{meas})^{-1} \label{eq:PoissonDef2}
\end{equation}
The mean number of particles in a hit strip becomes:
\begin{eqnarray}
C &=& \frac{\sum_{n>0} n P(n>0)}{\sum_{n>0} P(n>0)} \nonumber \\
  &=& \frac{e^{-\mu}}{1-e^{-\mu}} \mu  \sum \frac{\mu^n}{n!} 
  \nonumber \\
  &=& \frac{e^{-\mu}}{1-e^{-\mu}} \mu e^{\mu} \nonumber \\
  &=& \frac{\mu}{1-e^{-\mu}}
\end{eqnarray}
%While $\mu$ can be calculated analytically for practical purposes we
With $\mu$ defined in \eqref{eq:PoissonDef2} this calculation is
carried out per event in
regions of the FMD each containing 256 strips\footnote{Note that this means that the same factor is used for each of the 256 strips.}. %Defining
%$\mu_{meas}^{region}$ to be the measured occupancy
 In such a region,
$\mult$ for a hit strip ($N_{hits} \equiv 1$) in that region becomes:
\begin{equation}
\mult = N_{hits} \times C = 1 \times C = C
\end{equation}
Where C is calculated using $\mu_{meas}^{region}$.

The Poisson method and the energy fits method have been compared in
\cite{hhd:2009} where it is found that the two methods are in good
agreement. The residual difference between the methods contributes to
the systematic error.

\subsubsection{Azimuthal Acceptance}

Before the signal $\mult[,t]$ can be added to the $\etaphi$
bin in one of the 5 per--ring histograms, it needs to be corrected for
the $\varphi$ acceptance of the strip.

The sensors of the \FMD{} are not perfect arc--segments --- the two
top corners are cut off to allow the largest possible sensor on a 6''
Si-wafer.   This means, however, that the strips in these outer
regions do not fully cover $2\pi$ in azimuth, and there is therefore a
need to correct for this limited acceptance.  

The acceptance correction is only applicable where the strip length
does not cover the full sector.  This is the case for the outer strips
in both the inner and outer type rings.  The acceptance correction is
then simply 
\begin{align}
  \label{eq:acc_corr}
  \Corners{} &= \frac{l_t}{\Delta\varphi}\quad
\end{align}
where $l_t$ is the strip length in radians at constant $r$, and
$\Delta\varphi$ is $2\pi$ divided by the number of sectors in the
ring (20 for inner type rings, and 40 for outer type rings). 

Note, that this correction is a hardware--related correction, and does
not depend on the properties of the collision (e.g., primary vertex
location). 

The final $\etaphi$ content of the 5 output vertex dependent,
per--ring histograms of the inclusive charged particle density is then
given by
\begin{align}
  \label{eq:density}
  \dndetadphi[incl,r,v,i\etaphi] &= \sum_t^{t\in\etaphi}
  \mult[,t]\,\Corners{}
\end{align}
where $t$ runs over the strips in the $\etaphi$ bin. 

\subsection{Corrections}
\label{sec:sub:corrector}

The corrections code receives the five vertex dependent,
per--ring histograms of the inclusive charged particle density
$\dndetadphi[incl,r,v,i]$ from the density calculator and applies
two corrections 

\subsubsection{Secondary correction}
%%
%%                hHits_FMD<d><r>_vtx<v> 
%% hCorrection = -----------------------
%%                hPrimary_FMD_<r>_vtx<v>
%%
%% where 
%% - hPrimary_FMD_<r>_vtx<vtx> is 2D of eta,phi for all primary ch
%%   particles
%% - hHits_FMD<d><r>_vtx<v>  is 2D of eta,phi for all track-refs that
%%   hit the FMD - The 2D version of hMCHits_nocuts_FMD<d><r>_vtx<v>
%%   used below. 
This is a 2 dimensional histogram generated from simulations, as the
ratio of primary particles to the total number of particles that fall
within an $\etaphi$ bin for a given vertex bin

\begin{align}
  \label{eq:secondary}
  \SecMap{} &=
  \frac{\sum_i^{\NV[,v]}\mult[,\text{primary},i]\etaphi}{
    \sum_i^{\NV[,v]}\mult[,\text{\FMD{}},i]\etaphi}\quad,
\end{align}
where $\NV[,v]$ is the number of events with a valid trigger and a
vertex in bin $v$, and $\mult[,\FMD{},i]$ is the total number of
charged particles that hit the \FMD{} in event $i$ in the specified
$\etaphi$ bin and $\mult[,\text{primary},i]$ is number of
primary charged particles in event $i$ within the specified
$\etaphi$ bin.

$\mult[,\text{primary}]\etaphi$ is given by summing over the
charged particles labelled as primaries \emph{at the time of the
  collision} as defined in the simulation code.  That is, it is the
number of primaries within the $\etaphi$ bin at the collision
point --- not at the \FMD{}.

$\SecMap$ varies from $\approx 1.5$ for the most forward bins to
$\approx 3$ for the more central bins. Figure \ref{secondaries} shows
the $\dndeta$ of secondaries from various sources assessed with MC
simulations to give an idea of the magnitude of the effects of
secondaries.
\begin{figure}[]
  \centering
  \figinput[\textwidth]{secondary_origin}
  \caption{$\dndeta$ for secondaries and primaries in the FMD. The
    same plot for the SPD inner layer is included for comparison.}
  \label{secondaries}
\end{figure} 
 
%For pp, different event
%generators were used and found to give compatible results within
%3--5\%.   
For pp, at least some millions of events must be
accumulated to reach satisfactory statistics.  For Pb--Pb where the
general hit density is larger, reasonable statistics can be achieved
with less simulated data.   

\subsubsection{Acceptance due to dead channels}

Some of the strips in the \FMD{} have been marked up as \emph{dead},
meaning that they are not used in the reconstruction or analysis.
This leaves holes in the acceptance of each defined $\etaphi$
which need to be corrected for.  

Dead channels are marked specially in the \ESD{}s with the flag
\textit{Invalid Multiplicity}.  This is used in the analysis to build
up and event--by--event acceptance correction in each $\etaphi$
bin by calculating the ratio
\begin{align}
  \label{eq:dead_channels} 
  \DeadCh{} &= 
  \frac{\sum_t^{t\in\etaphi}\left\{\begin{array}{cl}
        1 & \text{if not dead}\\
        0 & \text{otherwise}
      \end{array}\right.}{\sum_t^{t\in\etaphi} 1}\quad,
\end{align}
where $t$ runs over the strips in the $\etaphi$ bin.  This correction
is obviously $v_z$ dependent since the $\etaphi$ bin to which a strip $t$
corresponds to depends on its  position relative to the primary vertex.

Alternatively, pre--made acceptance factors can be used.  These are
made from the off-line conditions database (\OCDB{}).

The 5 output vertex dependent, per--ring histograms of the primary
charged particle density is then given by
\begin{align}
  \dndetadphi[r,v,i\etaphi] &=
  \SecMap{} \frac{1}{\DeadCh{}}\dndetadphi[incl,r,v,i\etaphi]
\end{align}

\subsection{Histogram collector}
\label{sec:sub:hist_collector}

The histogram collector collects the information from the 5 vertex
dependent, per--ring histograms of the primary charged particle
density $\dndetadphi[r,v,i]$ into a single vertex dependent histogram
of the charged particle density $\dndetadphi[v,i]$.  

To do this, it first calculates, for each vertex bin, the $\eta$ bin
range to use for each ring.  It investigates the secondary correction
maps $\SecMap{}$ to find the edges of each map.  The edges are given
by the $\eta$ range where $\SecMap{}$ is larger than some
threshold\footnote{Typically $t_s\approx 0.1$.}  $t_s$. The code
applies safety margin of a number of bins, $N_{cut}$\footnote{Typically
  $N_{cut}=1$.}, to ensure that the data selected does not have too
large corrections associated with it.

It then loops over the bins in the defined $\eta$ range and sums the
contributions from each of the 5 histograms.  In the $\eta$ ranges
where two rings overlap, the collector calculates the average and adds
the errors in quadrature\footnote{While not explicitly checked, it was
  found that the histograms agrees within error bars in the
  overlapping region}.

The output vertex dependent histogram of the primary
charged particle density is then given by
\begin{align}
  \label{eq:superhist}
  \dndetadphi[v,i\etaphi] &=
  \frac{1}{N_{r\in\etaphi}}\sum_{r}^{r\in\etaphi}  
  \dndetadphi[r,v,i\etaphi]\\
  \delta\left[\dndetadphi[v,i\etaphi]\right] &=
  \frac{1}{N_{r\in\etaphi}}\sqrt{\sum_{r}^{r\in\etaphi}   
    \delta\left[\dndetadphi[r,v,i\etaphi]\right]^2}
  \quad,
\end{align}
where $N_{r\in\etaphi}$ is the number of overlapping histograms
in the given $\etaphi$ bin. 

The histogram collector stores the found $\eta$ ranges in the
underflow bin of the histogram produced.  The content of the overflow
bins are 
\begin{align}
  \label{eq:overflow}
  I_{v,i}(\eta) &= 
  \frac{1}{N_{r\in(\eta)}}
  \sum_{r}^{r\in(\eta)} \left\{\begin{array}{cl} 
      0 & \eta \text{\ bin not selected}\\ 
      1 & \eta \text{\ bin selected}
      \end{array}\right.\quad,
\end{align}
where $N_{r\in(\eta)}$ is the number of overlapping histograms in the
given $\eta$ bin.  The subscript $v$ indicates that the content
depends on the current vertex bin of event $i$.

\section{Building the final $\dndeta$}
\label{sec:ana_aod}

To build the final $\dndeta$ distribution it is enough to sum
\eqref{eq:superhist} and \eqref{eq:overflow} over all accepted
events, $\NA$, and correct for the acceptance $I(\eta)$ 
\begin{align}
  \dndetadphi[\etaphi] &= \sum_i^{\NA}\dndetadphi[i,v\etaphi]\\ 
  I(\eta) &= \sum_i^{\NA}I_{i,v}(\eta)\quad.
\end{align}
Note, that $I(\eta)\le\NA$.  

We then need to normalise to the total number of events $N_X$, given
by 
\begin{align}
  \N{X}{} &= \frac{1}{\epsilon_X}\left[\NA + \alpha(\NnotV -
    \beta)\right]  \label{eq:fulleventnorm}\\
  & = \frac{1}{\epsilon_X}\left[\NA + \frac{\NA}{\NV}(\NT-\NV{} -
    \beta)\right]\nonumber \\
  & =\frac{1}{\epsilon_X}\NA\left[1+\frac{1}{\epsilon_V}-1-
    \frac{\beta}{\NV}\right]\nonumber\\ 
  & = \frac{1}{\epsilon_X}\frac{1}{\epsilon_V}\NA
  \left(1-\frac{\beta}{\NT{}}\right)\nonumber
\end{align}
where
\begin{description}
\item[$\epsilon_X$]  is the trigger efficiency for type
  $X\in[\text{\INEL},\text{\INELONE},\text{\NSD} for p+p data and MB
  for Pb+Pb data]$
\item[$\epsilon_V=\frac{\NV{}}{\NT{}}$] is the vertex efficiency
  evaluated over the data.
\item[$\NA$] is the number of events with a trigger \emph{and} a valid
  vertex in the selected range
\item[$\NV{}$] is the number of events with a trigger \emph{and} a valid
  vertex. 
\item[$\NT$] is the number of events with a trigger.
\item[$\NnotV{}=\NT-\NV{}$] is the number of events with a trigger
  \emph{but no} valid vertex
\item[$\alpha=\frac{\NA}{\NV}$] is the fraction of accepted events of
  the total number of events with a trigger and valid vertex.  
\item[$\beta=\N{a}{}+\N{c}{}-\N{e}{}$] is the number of background
  events \emph{with} a valid off-line trigger. This formula is the
  simplest case of one bunch crossing per trigger/background
  class. For more complicated collision setups the fractions in the
  formula change.
\end{description}
The two terms under the parenthesis in \eqref{eq:fulleventnorm} refers
to the observed number of event $\NA$, and the events missed because
of no vertex reconstruction.  Note, for $\beta\ll\NT{}$
\eqref{eq:fulleventnorm} reduces to the simpler expression
$$
\N{X}{} = \frac1{\epsilon_X}\frac1{\epsilon_V}\NA{}
$$
The trigger efficiency $\epsilon_X$ for a given trigger type $X$ is
evaluated from simulations as
\begin{align}
  \epsilon_X = \frac{\N{X\wedge \text{T}}{}}{\N{X}{}}\quad,
\end{align}
that is, the ratio of number of events of type $X$ with a
corresponding trigger to the number of events of type $X$. 

The final event--normalised charged particle density then becomes 
\begin{align}
  \frac{1}{N}\frac{dN_{\text{ch}}}{d\eta} &= 
  \frac{1}{\N{X}{}} \int_0^{2\pi} d\varphi
  \frac{\dndetadphi[\etaphi]}{I(\eta)}
  \label{eq:eventnormdndeta}
\end{align}

If the trigger $X$ introduces a bias on the measured number of events,
then \eqref{eq:eventnormdndeta} need to be modified to 
\begin{align}
  \frac{1}{N}\frac{dN_{\text{ch}}}{d\eta} &= 
  \frac{1}{\N{X}{}} \int_0^{2\pi} d\varphi
  \frac{\frac{1}{B\etaphi}\dndetadphi[\etaphi]}{I(\eta)}
  \label{eq:eventnormdndeta2}\quad,
\end{align}
where $B\etaphi$ is the bias correction.  This is typically
calculated from simulations using the expression 
\begin{align}
  B\etaphi = \frac{\frac{1}{\N{X\wedge
        \text{T}}{}}\sum_i^{\N{X\wedge \text{T}}{}}
    \mult[,\text{primary}]\etaphi}{\frac{1}{\N{X}{}}\sum_i^{\N{X}{}}
    \mult[,\text{primary}]\etaphi}
\end{align}

\section{Systematic Errors} \label{fmdsysterror} 
\begin{table} 
\centering
\begin{tabular}{|c|c|c|}
\hline
 Effect & Magnitude in Pb+Pb analysis & Magnitude in p+p
 analysis \\
\hline
 Variation of the cuts in sec. \ref{sec:sub:sharing_filter} & 2\%   &  3\% \\
\hline
Calculation of $\mult$ & 3\%   &  4\% \\
\hline
 Material budget   & 7 \%  & 7 \%  \\
\hline
 Generator    & 2\%  & 2\%   \\
\hline
Vertex and trigger bias    & N/A  &  3\%  \\
\hline
 Centrality   & 1\% --6\%   & N/A  \\
\hline
 Normalization   & N/A  &  1.3\% - 3\% \\
\hline
\hline
Total in quadrature & 8.2\% -- 10.1\% & 9.4 \% -- 9.8\% \\
\hline
\end{tabular}
\caption[Systematic Errors in the FMD]{The table summarizes the
  systematic errors in the FMD including the total systematic error
  obtained by addition in quadrature.} \label{systerrors} 
\end{table}
The systematic errors on the $\dndeta$ measurement are discussed in detail in 
\cite{hhd:2009}. The results for the systematic errors in p+p and
Pb+Pb data are shown in table \ref{systerrors}. A short summary of the elements of the table is given here:
\begin{itemize}
\item The variations of the cuts in section \ref{sec:sub:sharing_filter} are carried out by re--running the analysis with different cuts and taking the observed differences as the contribution to the systematic error.
\item To assess the error on the calculation of the multiplcity the two methods for counting particles (see section \ref{sec:sub:density_calculator}) are compared.
\item The systematic error on the material budget description was found from simulations with $\pm 10 \%$ increased density.
\item Several event generators were used to assess the error from the particular choice of generator in the analysis. The same procedure was used to assess the error from the MC dependent part of the correction for trigger and vertex bias (p+p only). 
\item The systematic error on the centrality selection was obtained from variations of the different methods for measuring centrality. 
\end{itemize}

\section{Using the per--event $\dndetadphi[i,v]$ histogram for other
  analysis} 

\subsection{Multiplicity distribution} 

To build the multiplicity distribution for a given $\eta$ range
$[\eta_1,\eta_2]$, one needs to find the total multiplicity in that
$\eta$ range for each event. To do so, one should sum the
$\dndetadphi[i,v]$ histogram over all $\varphi$ and in the selected
$\eta$ range.
\begin{align}
  n'_{i[\eta_1,\eta_2]}, &= \int_{\eta_1}^{\eta_2}d\eta\int_0^{2\pi}d\varphi
  \dndetadphi[i,v]\quad.\nonumber
\end{align}
However, $n'_i$ is not corrected for the coverage in $\eta$ for the
particular vertex range $v$.  One therefor needs to correct for the
number of missing bins in the range $[\eta_1,\eta_2]$.  Suppose
$[\eta_1,\eta_2]$ covers $N_{[\eta_1,\eta_2]}$ $\eta$ bins, then the acceptance
correction is given by 
\begin{align}
  A_{i,[\eta_1,\eta_2]} = \frac{N_{[\eta_1,\eta_2]}}{\int_{\eta_1}^{\eta_2}d\eta\,
    I_{i,v}(\eta)}\quad.\nonumber
\end{align}
The per--event multiplicity is then given by 
\begin{align}
  n_{i,[\eta_1,\eta_2]} &= A_{i,[\eta_1,\eta_2]}\,n'_{i,[\eta_1,\eta_2]}\nonumber\\
  &= \frac{N_{[\eta_1,\eta_2]}}{\int_{\eta_1}^{\eta_2}\eta
    I_{i,v}(\eta)} \int_{\eta_1}^{\eta_2}d\eta\int_0^{2\pi}d\varphi
  \dndetadphi[i,v]
  \label{eq:event_n}
\end{align}

\subsection{Forward--Backward correlations} 

To do forward--backward correlations, one need to calculate
$n_{i,[\eta_1,\eta_2]}$ as shown in \eqref{eq:event_n} in two bins
$n_{i,[\eta_1,\eta_2]}$ and $n_{i,[-\eta_2,-\eta_1]}$ \textit{e.g.},
$n_{i,f}=n_{i,[-3,-1]}$ and $n_{i,b}=n_{i,[1,3]}$. 

\clearpage
\section{Some results}

%% \figurename{}s \ref{fig:1} to \ref{fig:3} shows some results.
Figures below show some examples \cite{hhd:2009}.  Note these are not
finalised plots.
\begin{figure}[]
  \centering
  \figinput[\textwidth]{results_ppdndeta}
  \caption{$\dndeta$ for pp for \INEL{} events at
    $\sqrt{s}=\GeV{900}$, $\sqrt{s}=\TeV{2.76}$, and $\sqrt{s}=\TeV{7}$
    $\cm{-10}\le v_z\le\cm{10}$, rebinned by a factor 5 \cite{hhd:2009}. 
    % Middle panel
    % shows the ratio of ALICE data to UA5, and the bottom panel shows
    % the ratio of the right (positive) side to the left (negative) side
    % of the forward $\dndeta$.
  }
  \label{fig:1}
\end{figure} 
\begin{figure}[]
  \centering
  \figinput[\textwidth]{results_PbPbdndeta}
  \caption{$\dndeta$ for Pb+Pb for Minimum Bias events at
    $\sqrt{s_{NN}}=\TeV{2.76}$ $\cm{-10}\le v_z\le\cm{10}$, rebinned by a
    factor 5 in 10 centrality intervals \cite{hhd:2009}. 
% Middle panel
%    shows the ratio of ALICE data to UA5, and the bottom panel shows
%    the ratio of the right (positive) side to the left (negative) side
%    of the forward $\dndeta$.
}
  \label{fig:2}
\end{figure} 


\clearpage

\section{Analysis for QM 2012 and Paper} \label{prelim}
\subsection{Analysis}

Following the development of the displaced vertex technique for VZERO
\cite{maxime} it was decided also to attempt such an analysis with the
FMD using exactly the same event selection and centrality selection as
the VZERO analysis.

The analysis described in this note was used successfully on these
special events. Three detectors contribute to this measurement: SPD
with tracklets covering $-2<\eta<2$ \cite{ruben,Aamodt:2010cz}, VZERO
covering $-3<\eta<-1.25$ and $1.25<\eta<5.25$, and FMD covering
$-5<\eta<-1.25$ and $1.25<\eta<5.5$. The extended coverage of the
VZERO and FMD comes from the positions of the displaced vertices. The
full pseudorapidity coverage of the combined measurement is
$-5<\eta<5.5$.

To combine the measurements the individual measurements were weighted
by their systematic error before a weighted average was taken to form
the final $\dndeta$. The systematic error is calculated as an average
in quadrature with a contribution from the residual difference between
the measurements.

Due to the nature of the ZDCvsZEM centrality determination (see
\cite{maxime} for details) the centrality selection of the measurement
with SPD, VZERO, and FMD is limited to $30\%$ central collisions. The
centrality bins considered are thus $0-5\%$, $5-10\%$, $10-20\%$, and
$20-30\%$.

The selected vertices with full pseudorapidity coverage for FMD in
this analysis are $\cm{112.5}$, $\cm{150}$, $\cm{187.5}$, $\cm{225}$,
$\cm{262.5}$, $\cm{300}$. For vertices $v_z > \cm{300}$ and $v_z <
\cm{112.5}$ a cut is imposed in pseudorapidity to only accept data
with $|\eta| > 4$ to avoid regions in ALICE known to have issues with
the material budget description.

\subsection{Analysis Performance}

This section includes some plots to assess the validity of the
analysis. This includes comparisons between the measurements used
(SPD, VZERO, and FMD) and $\dndphi$ from the FMD.

Figure \ref{coverage} shows the pseudorapidity coverage of the FMD
when using FMD1 and FMD2I as a function of vertex with displaced
vertices.
\begin{figure}[hbp]
  \centering
  \figinput[\textwidth]{performance_coverage}
  \caption{Pseudorapidity coverage of the FMD as a function of vertex
    with displaced vertices.}
  \label{coverage}
\end{figure} 

Figure \ref{spdfmdvzero} shows the results of the measurements of the
SPD, VZERO, and FMD. It is seen that there is good agreement between
the three different measurements albeit residual differences of up to
$6 \%$ remain.
\begin{figure}[hbp]
   \centering
  \figinput[\textwidth]{performance_spdfmdvzero}
  \caption{$\dndeta$ measured with nominal vertices with the SPD and
    displaced vertices with VZERO and FMD. It is seen that there is
    good agreement between the measurements.}
  \label{spdfmdvzero}
\end{figure} 

Figure \ref{ratiofmdvzero} shows the ratios of the measurements of FMD
and VZERO to the combined measurement and to the SPD measurement. It
is seen that the residual differences are small and there is good
agreement between the three different measurements.
\begin{figure}
  \centering
  \begin{minipage}{0.5\linewidth}
    \centering
    \figinput[\textwidth]{performance_ratio_tocombined}
  \end{minipage}%
  \begin{minipage}{0.5\linewidth}
    \centering
    \figinput[\textwidth]{performance_ratio_tospd}
  \end{minipage}%
  \caption{Left: Ratio of FMD and VZERO measurements to the combined
    $\dndeta$ measured with SPD, VZERO and FMD. Right: Ratios of FMD
    and VZERO measurement to SPD measurement in regions of
    overlap. It is worth pointing out that the residual differences
    can come from the fact that the VZERO analysis uses SPD for
    absolute calibration while the FMD analysis does not. This means that the
    centrality determination for displaced vertices will affect the
    FMD analysis the most because the VZERO analysis has an additional
  constraint from the SPD analysis that uses the ZDCvsZEM centrality
  at midrapidity where it can be crosschecked with other means of
  centrality determination. Such a crosscheck is not possible elsewhere.}
  \label{ratiofmdvzero}
\end{figure} 

Since $\dndeta$ is an average taken over $\varphi$ it is instructive
to consider $\dndphi$ to check that these distributions are flat as
they should be. Figure \ref{dndphi_pos} shows examples of the
$\dndphi$ distributions for FMD1. Figure \ref{dndphi_neg} shows
examples from FMD2 (inner ring). The two low points at $\varphi \sim
5.5$ in Figure \ref{dndphi_neg} are understood as coming from two
dying chips in FMD2I. They are considered dead in the final analysis
and corrected for. It is seen that the trends are quite flat within
$\sim 5\%$ as expected. The same trend is observed for all the
distributions.

\begin{figure}
  \centering
  \figinput[\textwidth]{performance_dndphi_fmd1}
  \caption{Examples of $\dndphi$ from FMD1 (positive
    pseudorapidities). The distributions are essentially flat.}
  \label{dndphi_pos}
\end{figure} 

\begin{figure}
  \centering
  \figinput[\textwidth]{performance_dndphi_fmd2}
  \caption{Examples of $\dndphi$ from FMD2I (negative
    pseudorapidities). The two low points at $\varphi \sim 5.5$ are
    understood as the result of two dying chips in FMD2I. They are
    considered dead in the final analysis and corrected for
    accordingly. Apart from these points, the distributions are
    essentially flat.}
  \label{dndphi_neg}
\end{figure} 

Figure \ref{pervertex} shows the analysis performed for each
vertex. The material budget effects for vertices $<\cm{112.5}$ are
clearly seen.

\begin{figure}
  \centering
  \figinput[0.8\textwidth]{performance_pervertex_negfield}
  \figinput[0.8\textwidth]{performance_pervertex_posfield}
%\end{minipage}%
  \caption{Top: Analysis per vertex for negative field data. Bottom:
    Analysis per vertex for positive field data. In the two plots the
    vertices where the full coverage is used are shown in blue. For
    the red and green points there a cut is applied for the
    pseudorapidity so that only points with $|\eta|>4$ are used in the
    analysis.}
\label{pervertex}
\end{figure} 

Figure \ref{leftright} shows the ratio of the postive and negative
pseudorapidities for the FMD. It is seen that there are discrepancies
of up to $\sim 5 \%$.
\begin{figure}
  \centering
  \figinput[0.7\textwidth]{performance_ratio_leftright}
  \caption{Ratios of the positive and negative pseudorapidities for
    the FMD (ratio is negative over positive). The grey band indicates
    the combined systematic error for FMD1I and FMD2I assuming
    excluding all contributions from event selection and material
    budget (i.e. the minimum systematic error between FMD1I and
    FMD2I).}  \label{leftright}
\end{figure} 

\subsection{Results}

This section summarizes the final results of the analysis and includes
the figures for approval.

Figure \ref{combineddndeta} shows the combined $\dndeta$ from SPD,
VZERO, and FMD in the full pseudorapidity range of $-5<\eta<5.5$.

\begin{figure}
  \centering
  \figinput[\textwidth]{results_PbPbdndeta_sat}
  \caption{Request for ALICE preliminary: Combined $\dndeta$ measured
    with SPD, VZERO and FMD. The VZERO and FMD measurements are made
    with displaced vertices and the SPD measurement is made at the
    nominal vertex. The fits are fits to a function $f(\eta) = A\exp
    (\frac{\eta -a_1}{2 a_2^2}) - B\exp (\frac{\eta -b_1}{2 b_{2}^2})$
    i.e. a Gaussian centered on $ \eta = 0$ subtracted from a similar
    Gaussian.}
  \label{combineddndeta}
\end{figure} 

Figure \ref{dndetaoverNpart} shows $dN/d\eta/(N_{part}/2)$ based on
figure \ref{combineddndeta} and data taken from \cite{Aamodt:2010cz}.
\begin{figure}
  \centering
  \figinput[\textwidth]{results_PbPbnpart_sat}
  \caption{Request for ALICE preliminary: The $dN/d\eta/(N_{part}/2)$
    measured with SPD, VZERO and FMD. The VZERO and FMD measurements
    are made with displaced vertices and the SPD measurement is made
    at the nominal vertex. The values of $N_{part}$ and the
    measurement at $-0.5<\eta<0.5$ taken from \cite{Aamodt:2010cz}.}
  \label{dndetaoverNpart}
\end{figure} 

Using figure \ref{dndetaoverNpart}, figure \ref{RatiodndetaoverNpart}
is constructed. It shows the ratios of $dN/d\eta/(N_{part}/2)$ in the
following $\eta$ bins: $0.5<\eta<1.5$, $1.5<\eta<2.5$, $2.5<\eta<3.5$,
$3.5<\eta<4.5$, and $4.5<\eta<5.5$ to the published
$dN/d\eta/(N_{part}/2)$ at $-0.5<\eta<0.5$. These ratios are found to
be flat for all pseudorapidity intervals.

\begin{figure}
  \centering
  \figinput[\textwidth]{results_PbPbnpart_ratio}
  \caption{Request for ALICE preliminary: Ratios of
    $dN/d\eta/(N_{part}/2)$ at $0.5<\eta<1.5$, $1.5<\eta<2.5$,
    $2.5<\eta<3.5$, $3.5<\eta<4.5$, and $4.5<\eta<5.5$ to the
    published $dN/d\eta/(N_{part}/2)$ at $-0.5<\eta<0.5$. The ratios
    are found to be flat for all the pseudorapidity intervals.}
  \label{RatiodndetaoverNpart}
\end{figure} 

With the analysis presented in figure \ref{combineddndeta} it is also
possible to study longitudinal scaling from LHC to RHIC
energies. Figure \ref{longscaling} shows $\dndeta$ as a function of
$y'=\eta-y_{beam}$ from Figure \ref{combineddndeta} and results from
the BRAHMS\cite{Bearden:2001qq} and PHOBOS\cite{Alver:2010ck}
experiments at RHIC. From the figure it is seen that with the wide
coverage of the SPD, VZERO, and FMD measurement it is indeed likely
that longitudinal scaling exist from RHIC to LHC energies.

\begin{figure}
  \centering
  \figinput[\textwidth]{results_PbPblongscaling_sat}
  \caption{Request for ALICE preliminary: Study of Longitudinal
    scaling. $\dndeta$ as a function of $y'=\eta-y_{beam}$ from Figure
    \ref{combineddndeta} and the BRAHMS\cite{Bearden:2001qq} and
    PHOBOS\cite{Alver:2010ck} experiments at RHIC. The fits are the
    function from figure \ref{combineddndeta} and a straight line
    ending in $\eta=y_{beam}$. From the figure it seems likely that
    longitudinal scaling exists from RHIC to LHC energies.}
  \label{longscaling}
\end{figure} 

Finally the total number of produced charged particles,
$N_{ch}=\int^{y_{beam}}_{-y_{beam}}\dndeta d\eta$, has
been calculated from the fits in Figure \ref{combineddndeta}. The
obtained values of $N_{ch}$ versus $N_{part}$ are shown in figure
\ref{totalNch}. The systematic errors on $N_{ch}$ have been assessed
by the procedure of varying fit functions discussed in \cite{maxime}.

\begin{figure}
  \centering
  \figinput[\textwidth]{results_PbPbtotalnch_sat}
  \caption{Request for ALICE preliminary: Total number of charged
    particles, $N_{ch}=\int^{y_{beam}}_{-y_{beam}}\dndeta d\eta$,
    obtained from the fitted function in figure
    \ref{combineddndeta}. The systematic errors on this plot were
    assessed by variation of the fit function as described in \cite{maxime}.}
  \label{totalNch}
\end{figure} 

\subsection{Comparison to old Preliminary}

At QM 2011 figures were approved for preliminary status and
shown. Roughly six months later it was found that the execution of the
FMD analysis had a flaw\footnote{A boolean variable was wrong in a
  configuration macro for FMD.} which caused the results to be lower
than what they should be. The top panel of Figure
\ref{prelimcomparison} shows a comparison between the distribution in
Figure \ref{combineddndeta} and the preliminary (ALI-PREL-2536) shown
at QM 2011. The top panel shows the same comparison with the proper
FMD distribution instead of the incorrect one. It is clear that the
agreement observed between VZERO, SPD, and FMD at QM 2011 does not
hold with the FMD analysis run properly for nominal vertices.

\begin{figure}
  \centering
  \begin{minipage}{0.5\linewidth}
    \centering
    \figinput[\textwidth]{oldprelim_wrong}
  \end{minipage}%
  \begin{minipage}{0.5\linewidth}
    \centering
    \figinput[\textwidth]{oldprelim_right}
  \end{minipage}%
  \caption{Left: Comparison of new combined $\dndeta$ to the data
    shown at QM 2011. Right: The same comparison with the properly run
    FMD analysis at nominal vertices (`FMD Hits'). The difference is
    clearly seen around $|\eta| \sim 2$.}
  \label{prelimcomparison}
\end{figure} 

\subsection{Summary of Systematic Errors}

Table \ref{combinedsyst} shows the various sources of systematic
errors for the combined measurement of VZERO, SPD, and FMD collected
from Table \ref{fmdsysterror}, \cite{maxime}, and
\cite{ruben,Aamodt:2010cz}. The `common' section of the table refers
to source of systematic errors identified as common in the different
measurements. These errors were evaluated for the displaced vertices
analysis in the following way:
\begin{itemize}
\item Centrality errors come from variation in the parameters used in
  the scaling of the ZEM signal (see \cite{maxime}).
\item Material budget errors were estimated by analyzing a simulation
  and adding a weight of $0.9$ or $1.1$ to all physical processes
  except decays for all secondary particles. This approach was used in
  the absence of suitable ALICE simulation productions.
\item $p_T$ weights were developed to assess the effect of the
  difference in $p_T$ spectra measured by ALICE and in the HIJING
  generator.
\end{itemize}

\begin{table} 
  \centering
  \begin{tabular}{|c|c|}
    \hline
    Source of Error & Magnitude   \\
    \hline
    Common   &   \\
    \hline
    Centrality  & 1-4\%    \\
    \hline
    $p_T$ weights (FMD+VZERO)  & 2\%   \\
    \hline
    % Strangeness Enhancement  & 1\%    \\
    % \hline
    Material budget(FMD+VZERO)  & 4\%    \\
    \hline
    Generator  & 2\%    \\
    \hline
    SPD   &   \\
    \hline
    Background Subtraction & 0.1\%-2\%    \\
    \hline
    Particle Mix & 1\%   \\
    \hline
    Weak Decays & 1 \%   \\
    \hline
    Extrapolation to zero $p$ & 2\%    \\
    \hline
    VZERO &   \\
    \hline
    Fluctuation between rings & 3\%   \\
    \hline
    Normalization & 3\%-4\%   \\
    \hline
    FMD  &  \\
    \hline
    Variation of Cuts    &  2\%  \\
    \hline
    Calculation of Multiplicity    &  3\%  \\
    \hline
  \end{tabular}
  \caption[Combined Systematic Errors]{The table summarizes the
    systematic errors in the SPD\cite{ruben,Aamodt:2010cz},
    VZERO\cite{maxime}, and FMD\cite{hhd:2009}.} \label{combinedsyst}  
\end{table}

The errors are obtained using variation of the quantities studied in
MC simulations. In particular the studies of the dependence on the
material budget are carried out with special MC simulations where the
material density of ALICE is increased.

\subsection{Technical Details}

Here, the technical aspects of the analysis are described. The SPD
analysis was done on run 137366, reconstruction pass 2 while the FMD
and VZERO analysis were carried out on a total of 126 runs (46 with
negative field and 80 with positive field) to obtain the necessary
statistics for the displaced vertices. These runs were selected to be
of good quality for VZERO, SPD, FMD, and ZDC. These data were also
from pass 2 reconstruction.

The AliRoot version for SPD is: \textbf{v5-03-24-AN}, for VZERO:
\textbf{v5-03-28-AN}, and for FMD: \textbf{v5-03-26-AN}.

For the analysis of the displaced vertices presented here the
production LHC12c2 was used (the simulation was done with an anchor
run for each field polarity). This production includes the latest
version (as of July 2012) of the ALICE geometry and alignment.

There is a twiki page for the paper using this analysis:
\url{https://twiki.cern.ch/twiki/bin/viewauth/ALICE/PWGLFGeoPbPbdNdeta}.
\clearpage
%% \currentpdfbookmark{Appendices}{Appendices}
\appendix 
\section{Nomenclature} 
\label{app:nomen}

\begin{table}[hbp]
  \centering
  \begin{tabular}[t]{|lp{.8\textwidth}|}
    \hline 
    \textbf{Symbol}&\textbf{Description}\\
    \hline 
    \INEL & In--elastic event\\ 
    \INELONE & In--elastic event with at least one tracklet in the
    \SPD{} in the region $-1\le\eta\le1$\\ 
    \NSD{} & Non--single--diffractive event.  Single diffractive
    events are events where one of the incident collision systems
    (proton or nucleus) is excited and radiates particles, but there
    is no other processes taking place\\ 
    \hline
    $\NT{}$ & Number of events with a valid trigger\\
    $\NV{}$ & Number of events with a valid trigger \emph{and} a valid
    vertex.\\  
    $\NA{}$ & Number of events with a valid trigger
    \emph{and} a valid vertex \emph{within} the selected vertex range.\\ 
    $\N{a,c,ac,e}{}$ & Number of events with background triggers $A$,
    $B$, $AC$, or $E$, \emph{and} a valid off-line trigger of the
    considered type.   Background triggers are typically flagged with
    the trigger words \texttt{CINT1-A},  \texttt{CINT1-C},
    \texttt{CINT1-AC}, \texttt{CINT1-E}, or similar.\\
    \hline
    $\mult{}$ & Charged particle multiplicity\\ 
    $\mult[,\text{primary}]$ & Primary charged particle multiplicity
    as given by simulations\\ 
    $\mult[,\text{\FMD{}}]$ & Number of charged particles that hit the
    \FMD{} as given by simulations\\ 
    $\mult[,t]$ & Number of charged particles in an \FMD{} strip as
    given by evaluating the energy response functions $F$\\ 
    \hline
    $F$ & Energy response function (see \eqref{eq:energy_response})\\
    $\Delta_{mp}$ & Most probably energy loss\\ 
    $\xi$ & `Width' parameter of a Landau distribution\\
    $\sigma$ & Variance of a Gaussian distribution\\ 
    $a_i$ & Relative weight of the $i$--fold MIP peak in the energy
    loss spectra.\\ 
    \hline
    $\Corners{}$ & Azimuthal acceptance of strip $t$\\ 
    $\SecMap{}$ & Secondary particle correction factor in $\etaphi$
    for a given vertex bin $v$\\  
    $\DeadCh{}$ & Acceptance in $\etaphi$ for a given vertex bin $v$\\ 
    \hline
    $\dndetadphi[incl,r,v,i]$ & Inclusive (primary \emph{and}
    secondary) charge particle density in event $i$ with vertex $v$,
    for \FMD{} ring $r$.\\ 
    $\dndetadphi[r,v,i]$ & Primary charged particle
    density in event $i$ with vertex $v$ for \FMD{} ring $r$. \\
    $\dndetadphi[v,i]$ & Primary charged particle density in event $i$
    with vertex $v$\\  
    $I_{v,i}(\eta)$ & $\eta$ acceptance of event $i$ with vertex $v$\\ 
    $I(\eta)$ & Integrated $\eta$ acceptance over $\NA$ events.
    Note, that this has a value of $\NA$ for $(\eta)$ bins where we
    have full coverage\\ 
    \hline 
    $X_t$ & Value $X$ for strip number $t$ (0-511 for inner rings,
    0-255 for outer rings)\\ 
    $X_r$ & Value $X$ for ring $r$ (where rings are \FMD{1i},
    \FMD{2i}, \FMD{2o}, \FMD{3o}, and \FMD{3i} in decreasing $\eta$
    coverage).\\ 
    $X_v$ & Value $X$ for vertex bin $v$ (typically 10 bins from -10cm
    to +10cm)\\ 
    $X_i$ & Value $X$ for event $i$\\
    \hline
  \end{tabular}
  \caption{Nomenclature used in this document}
  \label{tab:nomenclature}
\end{table}
\clearpage


\section{Second pass example code}
\label{app:exa_pass2}
\lstset{basicstyle=\small\ttfamily,% 
  keywordstyle=\color[rgb]{0.627,0.125,0.941}\bfseries,% 
  identifierstyle=\color[rgb]{0.133,0.545,0.133}\itshape,%
  commentstyle=\color[rgb]{0.698,0.133,0.133},%
  stringstyle=\color[rgb]{0.737,0.561,0.561},
  emph={TH2D,TH1D,TFile,TTree,AliAODForwardMult},emphstyle=\color{blue},%
  emph={[2]dndeta,sum,norm},emphstyle={[2]\bfseries\underbar},%
  emph={[3]file,tree,mult,nV,nBg,nA,nT,i,gSystem},emphstyle={[3]},%
  language=c++,%
}
\begin{lstlisting}[caption={Example 2\textsuperscript{nd} pass code to
    do $\dndeta$},label={lst:example},frame=single,captionpos=b]
void Analyse(int mask=AliAODForwardMult::kInel,
             float vzLow=-10, float vzHigh=10, float trigEff=1)
{ 
  gSystem->Load("libANALYSIS.so");      // Load analysis libraries
  gSystem->Load("libANALYSISalice.so"); // General ALICE stuff
  gSystem->Load("libPWGLFforward2.so");  // Forward analysis code

  int                nT      = 0;              // # of ev. w/trigger
  int                nV      = 0;              // # of ev. w/trigger&vertex
  int                nA      = 0;              // # of accepted ev.
  int                nBg     = 0;              // # of background ev
  TH2D*              sum     = 0;              // Summed hist
  AliAODForwardMult* mult    = 0;              // AOD object
  TFile*             file    = TFile::Open("AliAODs.root","READ");
  TTree*             tree    = static_cast<TTree*>(file->Get("aodTree"));
  tree->SetBranchAddress("Forward", &forward); // Set the address

  for (int i = 0; i < tree->GetEntries(); i++) { 
    // Read the i'th event 
    tree->GetEntry(i);

    // Create sum histogram on first event - to match binning to input
    if (!sum) 
      sum = static_cast<TH2D*>(mult->GetHistogram()->Clone("d2ndetadphi"));
    
    // Calculate beta=A+C-E
    if (mult->IsTriggerBits(mask|AliAODForwardMult::kA))    nBg++;
    if (mult->IsTriggerBits(mask|AliAODForwardMult::kC))    nBg++;
    if (mult->IsTriggerBits(mask|AliAODForwardMult::kE))    nBg--;

    // Other trigger/event requirements could be defined 
    if (!mult->IsTriggerBits(mask)) continue; 
    nT++;

    // Check if we have vertex and select vertex range (in centimeters) 
    if (!mult->HasIpZ()) continue;
    nV++;
    
    if (!mult->InRange(vzLow, vzHigh) continue; 
    nA++;

    // Add contribution from this event
    sum->Add(&(mult->GetHistogram()));
  }

  // Get acceptance normalisation from underflow bins 
  TH1D* norm   = sum->ProjectionX("norm", 0, 0, "");
  // Project onto eta axis - _ignoring_underflow_bins_!
  TH1D* dndeta = sum->ProjectionX("dndeta", 1, -1, "e");
  // Normalize to the acceptance, and scale by the vertex efficiency 
  dndeta->Divide(norm);
  dndeta->Scale(trigEff * nT/nV / (1 - nBg/nT), "width");
  // And draw the result
  dndeta->Draw();
}
\end{lstlisting}

\section{$\Delta E$ fits} 
\label{app:eloss_fits}

\begin{figure}[htbp]
  \centering
  \figinput[\textwidth]{eloss_fits}
  \caption{Summary of energy loss fits in each $\eta$ bin (see also
    \secref{sec:sub:sub:eloss_fits}).
    \newline
    On the left side: Top panel shows the
    reduced $\chi^2$, second from the top shows the found
    scaling constant, 3\textsuperscript{rd} from the top is
    the most probable energy loss $\Delta_{mp}$, 4\textsuperscript{th}
    shows the width parameter $\xi$ of the Landau, and the
    5\textsuperscript{th} is the Gaussian width $\sigma$.
    $\Delta_{mp}$, $\xi$, and $\sigma$ have units of $\Delta E/\Delta
    E_{mip}$. 
    \newline
    On the right: The top panel shows the maximum number of
    multi--particle signals that where fitted, and the 4 bottom panels
    shows the weights $a_2,a_3,a_4,$ and $a_5$ for 2, 3, 4, and 5
    particle responses.}
  \label{fig:eloss_fits}
\end{figure}

\clearpage
\currentpdfbookmark{References}{References}
\begin{thebibliography}{99}
\bibitem{FWD:2004mz} \ALICE{} Collaboration, Bearden, I.~G.\
  \textit{et al} \textit{ALICE technical design report on forward
    detectors: FMD, T0 and V0}, \CERN{}, 2004, CERN-LHCC-2004-025
\bibitem{cholm:2009} Christensen, C.~H., \textit{The ALICE Forward
    Multiplicity Detector --- From Design to Installation},
  Ph.D.~thesis, University of Copenhagen, 2009,
  \url{http://www.nbi.dk/~cholm/}.
\bibitem{maxime} Guilbaud, M. \textit{et al}, \textit{Measurement of
    the charged-particle multiplicity density at forward rapidity with
    ALICE VZERO detector in central Pb-Pb collision at
    $\sqrt{s_{NN}}=\TeV{2.76}$}, ALICE internal note, 2012,
  \url{https://aliceinfo.cern.ch/Notes/node/17/}.
\bibitem{nim:b1:16}
%% \bibitem{Hancock:1983ry}
  S.~Hancock, F.~James, J.~Movchet {\it et al.}, ``Energy Loss
  Distributions For Single Particles And Several Particles In A Thin
  Silicon Absorber,'' Nucl.\ Instrum.\ Meth.\ \textbf{B1} (1984) 16,
  \url{http://cdsweb.cern.ch/record/147286/files/cer-000058451.pdf}.
\bibitem{phyrev:a28:615} 
  %% \bibitem{Hancock:1983fp}
  S.~Hancock, F.~James, J.~Movchet {\it et al.}, ``Energy Loss And
  Energy Straggling Of Protons And Pions In The Momentum Range
  0.7-gev/c To 115-gev/c,'' Phys.\ Rev.\ \textbf{A28} (1983) 615,
  \url{http://cdsweb.cern.ch/record/145395/files/PhysRevA.28.615.pdf}.
\bibitem{hhd:2009} Dalsgaard, H.~H., \textit{Pseudorapidity Densities
    in p+p and Pb+Pb collisions at LHC measured with the ALICE
    experiment}, Ph.D.~thesis, University of Copenhagen, 2011,
  \url{http://www.nbi.dk/~canute/thesis.pdf}.
\bibitem{ruben} Shahoyan, R. \textit{Determination of $\dndeta$ in
    Pb-Pb collision at 2.76 A TeV with SPD tracklets}, ALICE internal
  note 2012, \url{https://aliceinfo.cern.ch/Notes/node/59/}.
\bibitem{Aamodt:2010cz} K.~Aamodt {\it et al.}  [ALICE Collaboration],
  %``Centrality dependence of the charged-particle multiplicity
  %density at mid-rapidity in Pb-Pb collisions at sqrt(sNN) = 2.76
  %TeV,''
  Phys.\ Rev.\ Lett.\  {\bf 106} (2011) 032301
  [arXiv:1012.1657 [nucl-ex]].
  %%CITATION = ARXIV:1012.1657;%%
\bibitem{Bearden:2001qq} I.~G.~Bearden {\it et al.}  [BRAHMS
  Collaboration],
  %``Pseudorapidity distributions of charged particles from Au+Au
  %collisions at the maximum RHIC energy,''
  Phys.\ Rev.\ Lett.\ {\bf 88} (2002) 202301 [nucl-ex/0112001].
  %%CITATION = NUCL-EX/0112001;%%
\bibitem{Alver:2010ck} B.~Alver {\it et al.}  [PHOBOS Collaboration],
  % ``Phobos results on charged particle multiplicity and
  % pseudorapidity distributions in Au+Au, Cu+Cu, d+Au, and p+p
  % collisions at ultra-relativistic energies,''
  Phys.\ Rev.\ C {\bf 83} (2011) 024913 [arXiv:1011.1940 [nucl-ex]].
  %%CITATION = ARXIV:1011.1940;%%
\end{thebibliography}
\end{document}

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