In principle both accelerator types can deliver the required proton beam for ADS applications. However, the nature of each — one compact unit for an isochronous cyclotron, a sequential modular structure for the linac — brings both advantages and disadvantages.
Due to its recirculation nature, a cyclotron is compact and cost effective. However, it lacks every form of redundancy which is crucial for fault tolerance. Hence, a cyclotron will not reach the wanted level of availability, and furthermore an upgrade of its beam energy is not a realistic option.
Linacs on the other hand, can be built as a sequence of many independent accelerating structures (RF cavities), which is a highly modular situation. It is this modularity that makes such a linac particularly well suited to tackle the availability issue. In case of failure of a single accelerating module, independently controlling the RF amplitude and phase of the adjacent modules creates the conceptual possibility of recovering the beam within a short time. Furthermore, increasing the final beam energy is obtained by merely adding accelerating modules.
For these reasons MYRRHA favours the linac option.
Linac versus cyclotron
| LINAC |
CYCLOTRON |
| Large space requirement (few hundred m long) but light |
Compact but heavy |
| Expensive |
Cheaper in construction |
| Less efficient power conversion |
More efficient power conversion |
| Modularity provides redundancy |
No intrinsic redundancy |
| Upgradable in energy |
Difficult to upgrade in energy |
| Straightforward beam extraction |
Difficult extraction and related beam losses |
| Capable of high beam current (100 mA) |
Modest beam current capability (5 mA) |