]> git.uio.no Git - u/mrichter/AliRoot.git/commitdiff
renamed all files for ALICE-INT-2012-040 with corresponding prefix
authorcholm <cholm@f7af4fe6-9843-0410-8265-dc069ae4e863>
Tue, 16 Jul 2013 22:29:53 +0000 (22:29 +0000)
committercholm <cholm@f7af4fe6-9843-0410-8265-dc069ae4e863>
Tue, 16 Jul 2013 22:29:53 +0000 (22:29 +0000)
24 files changed:
PWGLF/FORWARD/doc/alice-int-2012-040-eloss_fits.png [moved from PWGLF/FORWARD/doc/eloss_fits.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-fmd_logo_v2.png [moved from PWGLF/FORWARD/doc/fmd_logo_v2.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-oldprelim_right.png [moved from PWGLF/FORWARD/doc/oldprelim_right.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-oldprelim_wrong.png [moved from PWGLF/FORWARD/doc/oldprelim_wrong.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_coverage.png [moved from PWGLF/FORWARD/doc/performance_coverage.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_dndphi_fmd1.png [moved from PWGLF/FORWARD/doc/performance_dndphi_fmd1.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_dndphi_fmd2.png [moved from PWGLF/FORWARD/doc/performance_dndphi_fmd2.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_pervertex_negfield.png [moved from PWGLF/FORWARD/doc/performance_pervertex_negfield.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_pervertex_posfield.png [moved from PWGLF/FORWARD/doc/performance_pervertex_posfield.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_ratio_leftright.png [moved from PWGLF/FORWARD/doc/performance_ratio_leftright.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_ratio_tocombined.png [moved from PWGLF/FORWARD/doc/performance_ratio_tocombined.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_ratio_tospd.png [moved from PWGLF/FORWARD/doc/performance_ratio_tospd.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-performance_spdfmdvzero.png [moved from PWGLF/FORWARD/doc/performance_spdfmdvzero.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_PbPbdndeta.pdf [moved from PWGLF/FORWARD/doc/results_PbPbdndeta.pdf with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_PbPbdndeta_sat.png [moved from PWGLF/FORWARD/doc/results_PbPbdndeta_sat.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_PbPblongscaling_sat.jpg [moved from PWGLF/FORWARD/doc/results_PbPblongscaling_sat.jpg with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_PbPbnpart_ratio.png [moved from PWGLF/FORWARD/doc/results_PbPbnpart_ratio.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_PbPbnpart_sat.png [moved from PWGLF/FORWARD/doc/results_PbPbnpart_sat.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_PbPbtotalnch_sat.png [moved from PWGLF/FORWARD/doc/results_PbPbtotalnch_sat.png with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-results_ppdndeta.pdf [moved from PWGLF/FORWARD/doc/results_ppdndeta.pdf with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-secondary_origin.pdf [moved from PWGLF/FORWARD/doc/secondary_origin.pdf with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040-share_fraction.pdf [moved from PWGLF/FORWARD/doc/share_fraction.pdf with 100% similarity]
PWGLF/FORWARD/doc/alice-int-2012-040.tex [moved from PWGLF/FORWARD/doc/doc.tex with 97% similarity]
PWGLF/FORWARD/doc/pwglfforward.sty

similarity index 97%
rename from PWGLF/FORWARD/doc/doc.tex
rename to PWGLF/FORWARD/doc/alice-int-2012-040.tex
index 0e3c91b18da4444905db962bc3b205ad0c0b20e8..1ba94f8bb87f4e2bd1d4c53356851eb51e1e59e9 100644 (file)
@@ -187,7 +187,7 @@ signals to properly reconstruct the energy loss of a single particle.
 
 \begin{figure}[htbp]
   \centering
-  \includegraphics[keepaspectratio,height=3cm]{share_fraction}
+  \figinput[3cm]{share_fraction}
   \caption{A particle traversing 2 strips and depositing energy in
     each strip. }
   \label{fig:share_fraction}
@@ -542,8 +542,7 @@ simulations to give an idea of the magnitude of the effects of
 secondaries.
 \begin{figure}[]
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{%
-    secondary_origin}
+  \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}
@@ -819,7 +818,7 @@ Figures below show some examples \cite{hhd:2009}.  Note these are not
 finalised plots.
 \begin{figure}[]
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{results_ppdndeta}
+  \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}. 
@@ -832,7 +831,7 @@ finalised plots.
 \end{figure} 
 \begin{figure}[]
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{results_PbPbdndeta}
+  \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}. 
@@ -894,7 +893,7 @@ when using FMD1 and FMD2I as a function of vertex with displaced
 vertices.
 \begin{figure}[hbp]
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{performance_coverage}
+  \figinput[\textwidth]{performance_coverage}
   \caption{Pseudorapidity coverage of the FMD as a function of vertex
     with displaced vertices.}
   \label{coverage}
@@ -906,7 +905,7 @@ the three different measurements albeit residual differences of up to
 $6 \%$ remain.
 \begin{figure}[hbp]
    \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{performance_spdfmdvzero}
+  \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.}
@@ -921,11 +920,11 @@ agreement between the three different measurements.
   \centering
   \begin{minipage}{0.5\linewidth}
     \centering
-    \includegraphics[keepaspectratio,width=\textwidth]{performance_ratio_tocombined}
+    \figinput[\textwidth]{performance_ratio_tocombined}
   \end{minipage}%
   \begin{minipage}{0.5\linewidth}
     \centering
-    \includegraphics[keepaspectratio,width=\textwidth]{performance_ratio_tospd}
+    \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
@@ -954,7 +953,7 @@ distributions.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{performance_dndphi_fmd1}
+  \figinput[\textwidth]{performance_dndphi_fmd1}
   \caption{Examples of $\dndphi$ from FMD1 (positive
     pseudorapidities). The distributions are essentially flat.}
   \label{dndphi_pos}
@@ -962,7 +961,7 @@ distributions.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{performance_dndphi_fmd2}
+  \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
@@ -978,8 +977,8 @@ clearly seen.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=0.8\textwidth]{performance_pervertex_negfield}
-  \includegraphics[keepaspectratio,width=0.8\textwidth]{performance_pervertex_posfield}
+  \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
@@ -995,7 +994,7 @@ pseudorapidities for the FMD. It is seen that there are discrepancies
 of up to $\sim 5 \%$.
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=0.7\textwidth]{performance_ratio_leftright}
+  \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
@@ -1014,7 +1013,7 @@ VZERO, and FMD in the full pseudorapidity range of $-5<\eta<5.5$.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{results_PbPbdndeta_sat}
+  \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
@@ -1029,7 +1028,7 @@ 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
-  \includegraphics[keepaspectratio,width=\textwidth]{results_PbPbnpart_sat}
+  \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
@@ -1047,7 +1046,7 @@ be flat for all pseudorapidity intervals.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{results_PbPbnpart_ratio}
+  \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
@@ -1067,7 +1066,7 @@ that longitudinal scaling exist from RHIC to LHC energies.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{results_PbPblongscaling_sat}
+  \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
@@ -1087,7 +1086,7 @@ by the procedure of varying fit functions discussed in \cite{maxime}.
 
 \begin{figure}
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{results_PbPbtotalnch_sat}
+  \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
@@ -1114,11 +1113,11 @@ hold with the FMD analysis run properly for nominal vertices.
   \centering
   \begin{minipage}{0.5\linewidth}
     \centering
-    \includegraphics[keepaspectratio,width=\textwidth]{oldprelim_wrong}
+    \figinput[\textwidth]{oldprelim_wrong}
   \end{minipage}%
   \begin{minipage}{0.5\linewidth}
     \centering
-    \includegraphics[keepaspectratio,width=\textwidth]{oldprelim_right}
+    \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
@@ -1374,7 +1373,7 @@ void Analyse(int mask=AliAODForwardMult::kInel,
 
 \begin{figure}[htbp]
   \centering
-  \includegraphics[keepaspectratio,width=\textwidth]{eloss_fits}
+  \figinput[\textwidth]{eloss_fits}
   \caption{Summary of energy loss fits in each $\eta$ bin (see also
     \secref{sec:sub:sub:eloss_fits}).
     \newline
index c141c6b7e6f8cdedb47c22db4bb7569a7eaaa4b1..317a0b6448ec7f696a52bfb169cd1e7646f8ab33 100644 (file)
@@ -67,4 +67,7 @@
 \setlength{\parskip}{1ex}
 \setlength{\parindent}{0em}
 
+\newcommand\figinput[2][\textwidth]{% 
+  \includegraphics[keepaspectratio,width=#1]{\jobname-#2}}
+
 \endinput