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BiBTeX citation export for MOPOST038: Excitation of the σ_{l}_{l} = 90° Resonance by the Cavity RF Accelerating Fields

@inproceedings{lagniel:ipac2022-mopost038,
  author       = {J.-M. Lagniel},
  title        = {{Excitation of the σ_{l}_{l} = 90° Resonance by the Cavity RF Accelerating Fields}},
  booktitle    = {Proc. IPAC'22},
% booktitle    = {Proc. 13th International Particle Accelerator Conference (IPAC'22)},
  pages        = {152--155},
  eid          = {MOPOST038},
  language     = {english},
  keywords     = {resonance, focusing, space-charge, linac, cavity},
  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-MOPOST038},
  url          = {https://jacow.org/ipac2022/papers/mopost038.pdf},
  abstract     = {{In RF linacs the longitudinal focusing is done by nonlinear forces and at high accelerating fields the zero-current longitudinal phase advance per longitudinal focusing period σ₀l_{l} can be high. The nonlinear components of the RF field (sextupolar, octupolar and higher order components) can then excite parametric resonances, including the 4th-order resonance (σ_{l}_{l} = 90°) when σ₀l_{l} is higher than 90°, inducing strong longitudinal emittance growths and acceptance reductions. The longitudinal beam dynamics is therefore complex, even when the nonlinear space-charge forces are ignored. The parametric resonance excitation by the RF field is analyzed before discussing the additional effect of the nonlinear space-charge forces, in particular to explain why the zero-current longitudinal phase advance per transverse focusing period σ₀l_{t} is not a relevant parameter. Examples are given in the SPIRAL2 linac case.}},
}