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Servranckx, "Users Guide to the Program DIMAD", SLAC REPORT 285, UC-28(A), May 1985. 6 B. F. 3", TRI-DN-99-4,January 28, 1999. 7 B. Franzke, Vacuum Requirements for Heavy Ion Synchrotrons, IEEE Trans. on Nuc. Sci. 3, (1981) 2116. 8 N. Bohr and J. Lindhard, Dan. Mat. Fys. Medd. 28, no. 7 (1954). D. Betz and Ch. Schmelzer, UNILAC 1-67 (1967). D. Betz, G. Hortig, E. Leischner, Ch. Schmelzer, B. Stadler, and J. Weihrauch, Phys. Lett. 22 No. 5 (1966)643 11 W. Joho, “High Intensity Problems in Cyclotrons”, 9th Int.

Figure 27. 03%) . The particles are tracked from the injection energy to the entrance of the deflector where their position is plotted. 5 Transverse Emittance From Figure 27, a turn separation of approximately 6 mm is achieved with most of the reduction in turn separation attributable to the extreme (± 15o) phase bunches. 8 π mm mrad normalized); this result is given in Figure 28. 28 Figure 28. 8 π mm mrad). From Figure 28, it was determined that after the inclusion of twice the transverse phase space, an rf voltage ripple, and an injection energy spread, there would be 5 mm separation between turns if the beam phase width is limited to ±10o in lieu of ±15 o.

2. 3. 4. g. ) Number Units Required Price per Unit Number of FTE-Years to Complete Task The FTE costs were converted to dollars by assuming a rate of 150 K$ per FTE-Year. 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.

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