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BiBTeX citation export for THPOPT043: Injection Design Options for the Low-Emittance PETRA IV Storage Ring

@inproceedings{jebramcik:ipac2022-thpopt043,
  author       = {M.A. Jebramcik and I.V. Agapov and S.A. Antipov and R. Bartolini and R. Brinkmann and D. Einfeld and T. Hellert and J. Keil and G. Loisch and F. Obier},
% author       = {M.A. Jebramcik and I.V. Agapov and S.A. Antipov and R. Bartolini and R. Brinkmann and D. Einfeld and others},
% author       = {M.A. Jebramcik and others},
  title        = {{Injection Design Options for the Low-Emittance PETRA IV Storage Ring}},
  booktitle    = {Proc. IPAC'22},
% booktitle    = {Proc. 13th International Particle Accelerator Conference (IPAC'22)},
  pages        = {2689--2692},
  eid          = {THPOPT043},
  language     = {english},
  keywords     = {septum, injection, kicker, emittance, lattice},
  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-THPOPT043},
  url          = {https://jacow.org/ipac2022/papers/thpopt043.pdf},
  abstract     = {{The proposed PETRA IV electron storage ring that will replace DESY’s flagship synchrotron light source PETRA III will feature a horizontal emittance as low as 20 pm based on a hybrid six-bend achromat lattice. Such a lattice design leads to the difficulty of injecting the incoming beam into an acceptance that is as small as 2.6 um. In contrast to earlier lattice iterations based on a seven-bend achromat lattice, the latest version allows accumulation, i.e., the off-axis injection of the incoming beam. In this contribution, the effects of deploying different septum types, namely a pulsed or a Lambertson septum, on the injection process as well as the injection efficiency are presented. This analysis includes the effects of common manipulations to the injected beam, e.g., beam rotation and aperture sharing, on the injection efficiency. Furthermore, the option of a nonlinear kicker and its optimization (wire positions, wire current, optics functions) are presented since a nonlinear kicker could provide an alternative to the rather large number of strip-line kickers that are necessary to generate the orbit bump at the septum.}},
}