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A report on the International Conference on Sector‐Focused Cyclotrons

AUG 01, 1962
David J. Clark

The conventional cyclotron, pioneered by Lawrence in the 1930’s, is limited in energy by contradictory requirements for the magnetic field. To provide beam stability in the direction of the magnetic field, the field must decrease with radius. But to keep the beam in phase with a constant‐frequency dee voltage, the field must increase with radius as the particle mass increases. In a conventional machine, the first requirement is satisfied and phase loss of the beam has limited the energy of protons from this first‐generation cyclotron to about 15 MeV, but it has been pushed as high as 22 MeV by the Oak Ridge group.

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References

  1. 1. L. H. Thomas, Phys. Rev. 54, 580 (1938).https://doi.org/PHRVAO

  2. 2. E. L. Kelley, et al., Rev. Sci. Instr. 27, 493 (1956).https://doi.org/RSINAK

  3. 3. K. R. Symon, et al., Phys. Rev. 103, 1837 (1956).https://doi.org/PHRVAO

  4. 4. H. G. Blosser, et al., Rev. Sci. Instr. 29, 819 (1958).https://doi.org/RSINAK

  5. 5. F. A. Heyn and K. K. Tat, Rev. Sci. Instr. 29, 662 (1958).https://doi.org/RSINAK

  6. 6. V. I. Danilov et al., Proc. Int’l Conf. on High‐Energy Accelerators, p. 221, CERN, Geneva (1959).

  7. 7. D. L. Judd (private communication).

  8. 8. A. I. Yavin, Physics Today, May 1962, p. 19.

More about the Authors

David J. Clark. Rutherford High Energy Laboratory, Harwell.

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This Content Appeared In
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Volume 15, Number 8

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