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Positron background for test run




$\displaystyle \sigma$ $\textstyle \propto$ $\displaystyle \frac{(\char93  \mathrm{of}~\mathrm{events})\times
(\mathrm{scale...
...rm{accepted}~\mathrm{triggers}}
\times\frac{1}{\mathrm{target}~\mathrm{length}}$ (1)
$\displaystyle \frac{\sigma_{e^+}}{\sigma_{e^-}}$ $\textstyle =$ $\displaystyle \frac{N_{e^+}}{N_{e^-}}\times
\frac{[\mathrm{accepted}~\mathrm{tr...
...~\mathrm{charge}]_{e^+}}
{[\mathrm{scaler}~\mathrm{per}~\mathrm{charge}]_{e^+}}$  


$\displaystyle \mathrm{for }~~ p_e = 1.5 \mathrm{GeV/c}~~~~~
\frac{\char93 2786}{\char93 2773}$ $\textstyle =$ $\displaystyle \frac{70}{29185}
\times\frac{393070\times 4}{1803176\times 15}
\times\frac{62367.3}{3121.6}$ (2)
  $\textstyle =$ $\displaystyle 0.28\% \nonumber$  


$\displaystyle \mathrm{for }~~ p_e = 0.9 \mathrm{GeV/c}~~~~~
\frac{\char93 2791}{\char93 2776}$ $\textstyle =$ $\displaystyle \frac{611}{3980}
\times\frac{303126\times 4}{1805844\times 15}
\times\frac{1171888.0}{71144.2}$ (3)
  $\textstyle =$ $\displaystyle 11.32\% \nonumber$  


$\displaystyle \mathrm{for }~~ p_e = 0.55 \mathrm{GeV/c}~~~~~
\frac{\char93 2778}{\char93 2815}$ $\textstyle =$ $\displaystyle \frac{1679}{10372}
\times\frac{926232\times 4}{1809950\times 15}
\times\frac{3394497.9}{198813.6}$ (4)
  $\textstyle =$ $\displaystyle 37.72\%$  
       



next up previous contents
Next: Comparison between code and Up: Data analysis for pion Previous: Electron(positron) pion separation for   Contents
Xiaochao Zheng 2001-05-01