Christopher Berry Non-spinning  almost 9 years ago

Commit id: aebd0fc2972b38da939d1fcceabbd18d46d2e3f4

deletions | additions      

       

\begin{table}  \begin{tabular}{ccccccc} \begin{tabular}{ccccc}  \textbf{Log ratio} & & \textbf{Mean} & & & \textbf{Standard deviation} & \\   & \textsc{bayestar} & non-spinning & spinning Spinning  & \textsc{bayestar} & non-spinning & spinning Spinning  \\ $\displaystyle \vphantom{\frac{0}{0}} \mathcal{R}^\mathrm{B}_{\mathrm{CR}_{0.5}}$ \mathcal{R}^X_{\mathrm{CR}_{0.5}}$  & $0.095$ & $0.008$ & ? $0.018$  & $0.117$ & $0.041$ & ? $0.064$  \\ $\displaystyle \vphantom{\frac{0}{0}} \mathcal{R}^\mathrm{B}_{\mathrm{CR}_{0.9}}$ \mathcal{R}^X_{\mathrm{CR}_{0.9}}$  & $0.075$ & $0.005$ & ? $0.018$  & $0.094$ & $0.048$ & ? $0.065$  \\ $\displaystyle \vphantom{\frac{0}{0}} \mathcal{R}^\mathrm{B}_{A_\ast}$ \mathcal{R}^X_{A_\ast}$  & $0.106$ & $0.018$ & ? $0.002$  & $0.447$ & $0.313$ & ? $0.340$  \end{tabular}  \caption{\label{tab:sky-ratio} Comparison of sky localization areas produced by the low-latency \textsc{bayestar}(B) analysis, the nonspinning SpinTaylorT4 (ns)  analysis and the high-latency fully spinning SpinTaylorT4(s)  analysis to the medium-latency non-spinning  TaylorF2 analysis. The mean and standard deviation of the log ratio for the $50\%$ credible region $\mathrm{CR}_{0.5}$, the $90\%$ credible region $\mathrm{CR}_{0.9}$ and the searched area $A_\ast$ are listed for each analysis.} \end{table}