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1% would provide no limitations on the fragment intensities and that this range was achievable for the Separated Sector Cyclotron. A vacuum of ≈10-7 torr was found to provide adequate transmission with the power loss estimated to be only ≈170 W under this condition. An rf system largely based on the PSI design was determined to meet design requirements. The extraction system efficiency was simulated including the effects of larger than nominal transverse emittance, rf voltage ripple, and injected beam energy spread.

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).

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.

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Analysis of a Cyclotron-Based 400 MeV Driver System

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