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BiBTeX citation export for TUPAB015: Beam Loading Compensation of APS Cavity with Off-Crest Acceleration in ILC e-Driven Positron Source

@inproceedings{kuriki:ipac2021-tupab015,
  author       = {M. Kuriki and S. Konno and H. Nagoshi and T. Omori and T. Takahashi and J. Urakawa and K. Yokoya},
% author       = {M. Kuriki and S. Konno and H. Nagoshi and T. Omori and T. Takahashi and J. Urakawa and others},
% author       = {M. Kuriki and others},
  title        = {{Beam Loading Compensation of APS Cavity with Off-Crest Acceleration in ILC e-Driven Positron Source}},
  booktitle    = {Proc. IPAC'21},
  pages        = {1368--1371},
  eid          = {TUPAB015},
  language     = {english},
  keywords     = {positron, beam-loading, linac, electron, target},
  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-TUPAB015},
  url          = {https://jacow.org/ipac2021/papers/tupab015.pdf},
  note         = {https://doi.org/10.18429/JACoW-IPAC2021-TUPAB015},
  abstract     = {{In E-Driven positron source of ILC, the generated positron is captured by RF accelerator by APS cavity. The positron is initially placed at the deceleration phase and gradually slipped down to acceleration phase. Because the beam-loading is expected to be more than 1A with a multi-bunch format, the compensation is essential to obtain uniform intensity over the pulse. A conventional method for the compensation is controlling the timing, but it doesn’t work in off-crest case. In this manuscript, we discuss the compensation with the phase and amplitude modulation on the input RF.}},
}