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BiBTeX citation export for MOP26: Bunch Length Measurement Systems at S-DALINAC*

@inproceedings{brauch:ibic2022-mop26,
  author       = {A. Brauch and M. Arnold and J. Enders and L.E. Jürgensen and N. Pietralla and S. Weih},
  title        = {{Bunch Length Measurement Systems at S-DALINAC*}},
& booktitle    = {Proc. IBIC'22},
  booktitle    = {Proc. 11th Int. Beam Instrum. Conf. (IBIC'22)},
  pages        = {96--99},
  eid          = {MOP26},
  language     = {english},
  keywords     = {cavity, target, electron, linac, diagnostics},
  venue        = {Kraków, Poland},
  series       = {International Beam Instrumentation Conference},
  number       = {11},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {12},
  year         = {2022},
  issn         = {2673-5350},
  isbn         = {978-3-95450-241-7},
  doi          = {10.18429/JACoW-IBIC2022-MOP26},
  url          = {https://jacow.org/ibic2022/papers/mop26.pdf},
  abstract     = {{A high-quality beam is necessary for electron scattering experiments at the superconducting Darmstadt electron linear accelerator S-DALINAC. An optimization of the bunch length to typical values of < 2 ps is performed to reach a high energy resolution of 1e-4. Currently, this is accomplished by inducing a linear momentum spread on the bunch in one of the accelerating cavities. The bunch length can then be measured with a target downstream. This method is time consuming and provides only an upper limit of the bunch length. Two new setups for bunch length measurements will improve the optimization process significantly. On the one hand, a new diagnostic beam line is set up in the low energy beam area. It includes a deflecting copper cavity used for measuring the bunch length by shearing the bunch and projecting its length on a target. On the other hand, a streak camera placed at different positions downstream the injector and the main linac will be used to measure the bunch length. Optical transition radiation from an aluminium coated kapton target is used to perform this measurement. The present layout of both systems and their current status will be presented in this contribution.}},
}