-\large \centering{\textcolor{cyan}{\LARGE\sf Mass correlators}}
+\large \centering{\textcolor{cyan}{\LARGE\sf Mass correlators in the confined phase}}
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+ 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.