The SPEAR Injector RF Gun and Linac Performance
Author(s) -
S Park
Publication year - 2000
Publication title -
osti oai (u.s. department of energy office of scientific and technical information)
Language(s) - English
Resource type - Reports
DOI - 10.2172/763858
Subject(s) - linear particle accelerator , klystron , booster (rocketry) , electron gun , beam (structure) , injector , amplifier , physics , chopper , rf power amplifier , electrical engineering , bunches , synchrotron , nuclear engineering , optics , engineering , voltage , nuclear physics , cathode ray , electron , cmos , astronomy , thermodynamics
In light of the SPEAR3 upgrade project where the goal is to store up to 500 mA of beam current at 3.0 GeV beam energy, the injector RF gun and linac performance must be optimized in terms of reliability and injection rate. The basic linac system layout has not been changed for the last ten years of operation. A thermionic 1.5-cell standing wave RF gun is the source of bunched beams at 10 Hz. An alpha magnet then compresses the bunch length to a few picosecond, and a travelling-wave beam chopper then allows only 3 or 4 bunches to reach the linac near the end of the RF pulse. This way the beam loading to the linac is minimized and the linac beam to the Booster synchrotron reaches the maximum energy. Some improvements were made over the past few years to achieve the system reliability and stability. The original three klystrons were replaced by one high-power tube. The modulator is presently charged by a switching power supply. The drive amplifier feeding the klystron was based on thermionic triodes; it is a solid-state amplifier now. The gun cathode assembly underwent several iterations. Some feedback controls stabilize the linac beam energy asmore » needed. In this paper the authors describe the modifications mentioned above, the present status, and the plans for the future.« less
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