10-1140-epjc-s10052-013-2582-8 » errorTable.tex
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\begin{table*}[t]
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\centering
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\caption{Contributions to the errors on the emittance measurements as percentage relative error.\label{tab:errors}} |
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\begin{tabular}{lcccccccccc} |
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\hline
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\multicolumn{2}{c}{Source} & $\delta \epsilon_{x}$ & $\delta \alpha_{x}$ & $\delta \beta_{x}$ & $\delta \eta_{x}$ & $\delta \eta_{x}'$ |
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& $\delta \epsilon_{y}$ & $\delta \alpha_{y}$ & $\delta \beta_{y}$ & $\delta p_{z}$\T\B \\ |
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\hline
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\multirow{2}{*}{TOF1 offsets } & $x$ &0.47 &0.74 & 0.47 &1.39 & 0.69 & 0.014 & 0.05 &$\approx 0$ &$\approx 0$ \T\\ |
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& $y$ & $\approx 0$ &0.01 &$\approx 0$ & 0.29 & 0.17 &0.02 &0.06 & $\approx 0$ &0.71 \\ |
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%\mr
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%\hline
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\multirow{2}{*}{TOF0 offsets} & $x$ & 0.04 & 0.07 & 0.03 & 0.13 & 0.22 & $\approx 0$ & 0.08& 0.01 & $\approx 0$ \\ |
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& $y$& $\approx 0$ & $\approx 0$ & $\approx 0$ & 0.02 & $\approx 0$ &$\approx 0$ & $\approx 0$& $\approx 0$ & $\approx 0$ \\ |
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%\mr
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%\hline
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\multicolumn{2}{c}{$\Delta L$ } & 2.10 & 0.32&2.11 &1.69 &3.30 &2.74 &30.17 & 2.78& 0.71 \\ |
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%\mr
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%\hline
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\multicolumn{2}{c}{Q789 currents } & 0.051 & $\approx 0$& 0.03 & 0.008 & 0.02 & 0.04 & 0.036 &0.035 & 0.002 \\ |
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%\mr
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%\hline
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\multirow{2}{*}{Q789 offsets } & $x$& 0.08 & 0.13& 0.08 & 0.17 &0.99 & $\approx 0$& 0.08 & 0.01 & $\approx 0$ \\ |
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& $y$ & $\approx 0$ &$\approx 0$&$\approx 0$ &0.01 &$\approx 0$ &$\approx 0$ &0.01 &$\approx 0$ & $\approx 0$ \\ |
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%\mr
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%\hline
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\multicolumn{2}{c}{Effective $c$ in scintillator } & 4.87 & 0.05& 5.23&2.22 & 1.59& 4.05 &41.27 & 4.09 & 0.11 \B\\ |
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%\mr
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%\hline
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%\multicolumn{2}{c|}{Resolution subtraction } & (11.80) &(7.71)& (18.35) & $\cdot$&$\cdot$ &(3.65) &(25.34) &(1.41) & $\cdot$ \\
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%\hline
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%\hline
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\hline
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\multicolumn{2}{c}{Total (\%)} & 5.32 & 0.82 & 5.66 & 3.14 & 3.87 &4.89 & 51.12 & 4.94 & 1.02 \T\B\\ |
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\hline
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%\hline
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%\hline
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%\multicolumn{2}{c|}{Total (\%)} & (12.95) & (7.75) & (19.20) & (3.14) & (3.87) &(6.10) & (57.06) &(5.14) & (1.02) \\
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\end{tabular}
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\end{table*}
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