# | Wien angle | beam | runs | target | Ptarget% | Pbeam% |
---|---|---|---|---|---|---|
1 | 30° | 0.58 µA | 13055-13058 | 5 | 7.97 | -81.7±0.3±2.0 |
2 | 30° | 0.80 µA | 13059-13060 | 5 | 7.97 | -81.1±0.3±2.0 |
3 | 50° | 0.80 µA | 13061-13064 | 5 | 7.97 | -90.8±0.3±2.0 |
4 | 70° | 0.80 µA | 13065-13068 | 5 | 7.97 | -88.4±0.3±2.0 |
5 | -30° | 0.80 µA | 13070-13073 | 5 | 7.97 | -9.4±0.3±2.0 |
6 | 54° | 0.80 µA | 13074-13077 | 5 | 7.97 | -91.0±0.3±2.0 |
7 | 54° | 0.80 µA | 13079-13082 | 4 | 7.44 | -90.5±0.2±2.0 |
8 | 54° | 0.55 µA | 13083-13086 | 3 | 7.62 | -88.0±0.2±2.0 |
9 | 54° | 0.55 µA | 13087-13090 | 2 | 8.21 | -90.8±0.2±2.0 |
10 | 30° | 0.80 µA | 13091-13094 | 5 | 7.97 | -82.3±0.2±2.0 |
average 6,7,9 | 54° | average the targets | -90.8±0.1±2.0 | |||
2,3,4,5 | dance | 0.80 µA | maximum at 54±1.° | 5 | 7.97 | -91.0±0.2±2.0 |
best | 30° | scaled to all targets | -82.1±0.3±2.0 |
A large chi2 of the spin dance fit (20/NDF) is likely caused by an energy instability,
which affects the measurements at large spin angles (far from 54°).
Figure 1
Figure 2