deletions | additions       diff --git a/appendix_reconstructed_wedges1.tex b/appendix_reconstructed_wedges1.tex  index 28ed936..f3d1d02 100644  --- a/appendix_reconstructed_wedges1.tex  +++ b/appendix_reconstructed_wedges1.tex 
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\section{Model-independent $H$, $D_{\rm A}$ without priors}  %============================================================  \begin{table}  \label{tab:hda_wigglez_reconstructed}  \caption{Caption for table!}  \begin{tabular}{ $cz/H/r_{\rm s}$ | c | r }  \hline  first & second & third \\  \hline  1 & 2 & 3 \\  4 & 5 & 6 \\  7 & 8 & 9 \\  \end{tabular}  \medskip  comments for table  \end{table}  %============================================================  In Figures \ref{fig:HDA_z60_noprior}-\ref{fig:HDA_z26_noprior} we present similar results to those shown in Figures \ref{fig:HDA_z60_epsilon0.15}-\ref{fig:HDA_z26_epsilon0.15} but without priors on $\epsilon$. We can see that in all three redshift bins that the BAO-only fit algorithm appears to yields a secondary psueo-mode at very high values of $cz/H/r_{\rm s}$. This