We use Gaussian process regression to determine the shape of a component which can compensate for the model inadequacy seen in the intermediate TOF area (30-60 ns).
Parameter limits ---------------- Fuel ratio: [0.01, 0.06] T fraction: [-inf, inf] D fraction: [-inf, inf] H fraction: [-inf, inf] NBI power: [1e-09, inf] RF power: [0, 0] Neutron yield: [1e+15, inf] Resonance pos: [-inf, inf] RF particle: tritons
| JPN | t0 | t1 |
|---|---|---|
| 100503 | 40 | 80 |
| 100505 | 40 | 80 |
| 100515 | 40 | 80 |
| 100516 | 40 | 80 |
| 100535 | 40 | 80 |
| 100536 | 40 | 80 |
| 100539 | 40 | 80 |
| 100540 | 40 | 80 |
| 100541 | 40 | 80 |
| 100542 | 40 | 80 |
| 100557 | 40 | 80 |
| 100569 | 40 | 80 |
| 100570 | 40 | 80 |
| 100572 | 40 | 80 |
| 100573 | 40 | 80 |
| 100580 | 40 | 80 |
| 100585 | 40 | 80 |
| 100602 | 40 | 80 |
| 100603 | 40 | 80 |
| 100718 | 40 | 80 |
| 100720 | 40 | 80 |
| 100721 | 40 | 80 |
| 100722 | 40 | 80 |
| 100723 | 40 | 80 |
| 100724 | 40 | 80 |
| 100725 | 40 | 80 |
| 100728 | 40 | 80 |
| 100737 | 40 | 80 |
| 100746 | 40 | 80 |
| 100747 | 40 | 80 |
| 100748 | 40 | 80 |
| 100760 | 40 | 80 |
| 100761 | 40 | 80 |
| 100763 | 40 | 80 |
| 100789 | 40 | 80 |
| 100790 | 40 | 80 |
| 100791 | 40 | 80 |
| 100792 | 40 | 80 |
| 100796 | 40 | 80 |
| 100797 | 40 | 80 |
| 100800 | 40 | 80 |
| 100803 | 40 | 80 |
| 100806 | 40 | 80 |
| 100828 | 40 | 80 |
| 100831 | 40 | 80 |
| 100841 | 40 | 80 |
| 100842 | 40 | 80 |
| 100844 | 40 | 80 |
| 100845 | 40 | 80 |
| 100846 | 40 | 80 |
| 100860 | 40 | 80 |
| 100863 | 40 | 80 |
| 100882 | 40 | 80 |
| 100896 | 40 | 80 |