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BiBTeX citation export for TUPAB356: Electron Beam Driven Cavities

@inproceedings{schuett:ipac2021-tupab356,
  author       = {M. Schuett and U. Ratzinger},
  title        = {{Electron Beam Driven Cavities}},
  booktitle    = {Proc. IPAC'21},
  pages        = {2342--2345},
  eid          = {TUPAB356},
  language     = {english},
  keywords     = {electron, cavity, simulation, linac, klystron},
  venue        = {Campinas, SP, Brazil},
  series       = {International Particle Accelerator Conference},
  number       = {12},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {08},
  year         = {2021},
  issn         = {2673-5490},
  isbn         = {978-3-95450-214-1},
  doi          = {10.18429/JACoW-IPAC2021-TUPAB356},
  url          = {https://jacow.org/ipac2021/papers/tupab356.pdf},
  note         = {https://doi.org/10.18429/JACoW-IPAC2021-TUPAB356},
  abstract     = {{State of the art high power feeder for RF cavities used as accelerators generally require RF amplifiers consisting of a vacuum tube, such as a klystron or Grid Tubes. In addition, a number of cost intensive RF auxiliary devices are needed: Modulator, waveguides, circulator, power dump and couplers. The equipment requires significant floor space within the linac building. Alternatively, we propose a direct driven system. Aμbunched electron beam is injected directly into the cavity. A high perveance bunched electron beam can be generated by a standard electron gun combined with a deflecting beam chopper*, an off-the-shelf IOT or klystron, respectively. The pulse rate is determined by the resonance frequency of the cavity. The resonator hereby acts like the output cavity of a klystron: Within its propagation through the cavity the beam is decelerated increasing the stored energy of the accelerator. We present 3D particle PIC simulations evaluating the geometry and beam properties in order to optimize the coupling efficiency and cavity excitation of state-of-art CH particle accelerator structures.}},
}