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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. Conference on Cyclotrons, p337, Caen, France 1981. M. Gordon, “The longitudinal space charge effect and energy resolution”, 5th Intl. , pages 305-317, Butterworths, London, 1971. M. Gordon and V. Taivassalo, “The z4 code and the focusing bar fields used in the extraction calculations for superconducting cyclotrons”, Nucl. Inst. , A247, 423 (1986).

2 ISOL Technical Task Force (June 24-25, 1999 at NSCL), C. Leemann, Chairman. 3 E. Baron, M. Bajard and Ch. Ricaud, “Charge exchange of very heavy ions in carbon foils and in the residual gas of GANIL cyclotrons”, NIM, A328 (1993), 177-182. 4 Private communication with Peter Ostroumov. 5 R. 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.

With an rf phase width of ±10o the clear space between turns at extraction is 5 mm. Additional effects caused by longitudinal space charge forces and horizontal-vertical motion coupling were also evaluated and found to be acceptably small effects. 99% is achievable for the Separated Sector Cyclotron design presented. A “bottom up” costing of the Separated Sector Cyclotron system was done and the total estimated cost for this element of the accelerator chain was found to be <100 M$ and the full acceleration chain to be <150 M$.

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Analysis of a Cyclotron-Based 400 MeV Driver System


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