almost done.

[phys/poster_lattice14.git] / poster_lattice14.tex

diff --git a/poster_lattice14.tex b/poster_lattice14.tex
index 3cb71271e02c1ba26639e88e070aa40a635f6072..43405bc8f85375b864261579f7ea36ccd65db6ec 100644 (file)
--- a/poster_lattice14.tex
+++ b/poster_lattice14.tex
@@ -235,9 +235,9 @@
 
   \vspace{0.2cm}
 
-  \begin{center}
-    \includegraphics[height=13cm]{dofs.pdf}
-  \end{center}
+  %\begin{center}
+    %\includegraphics[height=13cm]{dofs.pdf}
+  %\end{center}
 
   \vspace{-24pt}
 \end{minipage}
@@ -254,7 +254,7 @@
 \begin{minipage}[b]{350mm}
 
   \begin{center}
-    \includegraphics[height=20cm]{phasediagram.pdf}
+    \includegraphics[height=25cm]{phasediagram.pdf}
     \cite{PhysRevLett.111.141601}
   \end{center}
 
@@ -265,12 +265,14 @@
 %%%%%%%%%%%%%%%%%%%%%%% MASS CORRELATORS %%%%%%%%%%%%%%%%%%%%%%%%%%%
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
-\large \centering{\textcolor{cyan}{\LARGE\sf Mass correlators}}
+\large \centering{\textcolor{cyan}{\LARGE\sf Mass correlators in the confined phase}}
 
 \vspace{1.0cm}
 
 \begin{minipage}[b]{350mm}
 
+  For the fundamental correlators $F_1$ and $F_2$, as expected, we see no plateaus. The masses of the bound states $U_1$ and $U_2$ are split because we set the effective masses of the two flavours to different values.
+
   \begin{center}
     \includegraphics[height=28cm]{mass.pdf}
   \end{center}
@@ -288,8 +290,10 @@
 
 \begin{minipage}[b]{350mm}
 
+  We here show different observables as function of $\mu$. The dotted lines show the masses $U_1$ and $U_1$ determined from the plots above.
+
   \begin{center}
-    %\includegraphics[height=28cm]{mass.pdf}
+    \includegraphics[height=35cm]{finmu_840.pdf}
   \end{center}
 
   \vspace{-24pt}