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Extra resources for Analysis of a Cyclotron-Based 400 MeV Driver System
1 Pre-Accelerator (PA) Cost (M$) 1 1 43 45 Item RFQ RT Linac ≈250MV SC Linac SUBTOTAL Table 9. Summary costs for the 30 MeV/u pre-accelerator system. 4 Table 10. Summary costs for a 400 MeV/u Separated Sector Cyclotron system. 33 As a cross check on the Separated Sector Cyclotron, the relative fractional costs of the main elements of the cyclotron system are compared in Table 11 to that realized for the PSI Ring and TRIUMF cyclotrons. This comparison shows that the cost distribution in the SSC is essentially the same as those of other extant large cyclotrons.
To address this issue, calculations were performed using the Z 4 code13 that utilizes higher-order derivatives of the 30 magnetic field. The simulation accelerates four particles on the periphery of a half ellipse (the motion is symmetric for the other half) in the z-pz plane and the maximum beam height as a function of energy is obtained. 0 cm respectively. From Figure 29, the maximum vertical beam size for each of the four particles is less than 2 cm near extraction. The increase in size is due to the decreasing vertical focusing frequency with increasing energy.
Summary costs for a 400 MeV/u Separated Sector Cyclotron system. 33 As a cross check on the Separated Sector Cyclotron, the relative fractional costs of the main elements of the cyclotron system are compared in Table 11 to that realized for the PSI Ring and TRIUMF cyclotrons. This comparison shows that the cost distribution in the SSC is essentially the same as those of other extant large cyclotrons. Element Magnet System RF System Other PSI (%) 56 17 27 TRIUMF (%) 49 17 34 MSU Separated Sector Cyclotron (%) 59 22 19 Table 11.
Analysis of a Cyclotron-Based 400 MeV Driver System
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