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Formation of a single-bunch beam in the booster synchrotron at SPring-8
In order to fill an radio frequency (rf) bucket with an electron beam in the storage ring at SPring-8, an rf knockout system was installed in the booster synchrotron. With this system, the energy of the electron beam injected from the linac was increased from 1 to 8 GeV. The time width of multi-bunc...
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Published in: | Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Accelerators, spectrometers, detectors and associated equipment, 2000-04, Vol.444 (3), p.515-533 |
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Main Authors: | , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In order to fill an radio frequency (rf) bucket with an electron beam in the storage ring at SPring-8, an rf knockout system was installed in the booster synchrotron. With this system, the energy of the electron beam injected from the linac was increased from 1 to 8
GeV. The time width of multi-bunch beams from the linac operated at 2856
MHz rf can be selected as 1 or 40
ns. The beam injected from the linac is distributed in rf buckets of the booster synchrotron operated at 508.58
MHz rf. To fill a single rf bucket with a beam, the rf knockout system is operated at a minimum beam energy of 1
GeV. By using the rf knockout system, the electron beam is effectively kept in a single rf bucket. Then the beam is injected into a targeted rf bucket in the storage ring with a precise timing system. The beam intensity of satellite rf buckets in the storage ring was measured with a photon counting method and determined to be 10
−6 less than that of the main rf bucket. In this paper, we describe the rf knockout system installed in the booster synchrotron. |
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ISSN: | 0168-9002 1872-9576 |
DOI: | 10.1016/S0168-9002(99)01183-3 |