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BiBTeX citation export for THPOST021: Beam Dynamics Simulations of Linear Accelerator for Natural Rubber Vulcanization at Chiang Mai University

@inproceedings{saisut:ipac2022-thpost021,
  author       = {J. Saisut and M. Jitvisate and S. Rimjaem and C. Thongbai},
  title        = {{Beam Dynamics Simulations of Linear Accelerator for Natural Rubber Vulcanization at Chiang Mai University}},
  booktitle    = {Proc. IPAC'22},
% booktitle    = {Proc. 13th International Particle Accelerator Conference (IPAC'22)},
  pages        = {2491--2493},
  eid          = {THPOST021},
  language     = {english},
  keywords     = {electron, simulation, linac, gun, cathode},
  venue        = {Bangkok, Thailand},
  series       = {International Particle Accelerator Conference},
  number       = {13},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {07},
  year         = {2022},
  issn         = {2673-5490},
  isbn         = {978-3-95450-227-1},
  doi          = {10.18429/JACoW-IPAC2022-THPOST021},
  url          = {https://jacow.org/ipac2022/papers/thpost021.pdf},
  abstract     = {{The Linear accelerator system for natural rubber vulcanization has been developed at the Plasma and Beam Physics Research Facility, Chiang Mai University, Thailand. The main components of the accelerator system consist of a DC electron gun with a thermionic cathode, an RF linear accelerator, an RF system, a control system, and an irradiation system. The electron beam properties for natural rubber vulcanization are predicted from the beam dynamics simulation starting from a cathode to the titanium exit window. The electron beam generation and the particle in cell simulation inside the DC electron gun are performed using CST Studio Suit software. The electron distribution at the gun exit from the CST output is covered to be an input distribution of the ASTRA beam dynamics simulation program. The electron beam enters linac and is accelerated by RF filed inside the linac. The ASTRA simulation code is used to track electron trajectories including the space-charge interaction and the simulation starts from linac entrance to the exit windows. The electron beam properties for various conditions are evaluated and will be used for further simulations.}},
}