AVF Cyclotron |
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cyclotron must be designed that the average magnetic field can match the mass increase of the accelerated particle. Increasing radially magnetic field causes the axial defocusing. It is solved by provided magnetic field Azimuthally Varing Field.
CHARACTERISTISCS OF THE AVF CYCLOTRON |
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| Model | 370V | 480 | 560 | 750 | 930 |
| acceleration energy | |||||
| proton (MeV) | 18 | 4-30 | 5-42 | 25-70 | 6-90 |
| duteron (MeV) | 9.5 | 7-15 | 10-21 | 12.5-35 | 10-50 |
| 3He | 24 | 11-40 | 15-52 | 20-90 | 16-130 |
| 4He (α) | 14 | 14-30 | 20-42 | 25-70 | 20-100 |
| beam current | |||||
| proton | 50µA | 100µA | 100µA | 100µA | 40µA |
| deuteron | 50µA | 100µA | 100µA | 100µA | 40µA |
| 3He | 10µA | 30µA | 50µA | 30µA | 30µA |
| 4He (α) | 5µA | 50µA | 50µA | 50µA | 50µA |