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BiBTeX citation export for TUPOPA24: Design of an X-Band Bunching and Accelerating System for AWAKE Run 2

@inproceedings{arnesano:linac2022-tupopa24,
  author       = {J.M. Arnesano and S. Döbert},
  title        = {{Design of an X-Band Bunching and Accelerating System for AWAKE Run 2}},
  booktitle    = {Proc. LINAC'22},
% booktitle    = {Proc. 31st International Linear Accelerator Conference (LINAC'22)},
  pages        = {458--461},
  eid          = {TUPOPA24},
  language     = {english},
  keywords     = {cavity, acceleration, electron, bunching, gun},
  venue        = {Liverpool, UK},
  series       = {International Linear Accelerator Conference},
  number       = {31},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {09},
  year         = {2022},
  issn         = {2226-0366},
  isbn         = {978-3-95450-215-8},
  doi          = {10.18429/JACoW-LINAC2022-TUPOPA24},
  url          = {https://jacow.org/linac2022/papers/tupopa24.pdf},
  abstract     = {{The AWAKE experiment at CERN demonstrated in its Run 1 that it is possible to accelerate electrons in plasma wakefields driven by a self-modulated proton bunch. In Run2, AWAKE aims to increase the accelerating gradient in the plasma even further and demonstrate beam quality in order to be ready for high-energy physics experiments. In this framework, a new electron injector, consisting of an S-band RF-gun and a subsequent X-band bunching and accelerating section, capable of producing very short bunches with a small emittance, has been designed. In this paper, two different configurations of the X-band section and their corresponding high-power distribution systems are presented. The first one consists of three identical cavities to bunch and accelerate the beam while the second one uses a separate short structure for velocity bunching followed by three long, pure accelerating structures. A discussion of the strengths and weaknesses of each configuration is carried out and beam dynamics aspects are analyzed. Finally the X-Band power distribution systems are described with particular attention to the choice of the klystron, the pulse compression system and the waveguide distribution.}},
}