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BiBTeX citation export for TUPB014: Design of a Large Momentum Acceptance Gantry Based on AG-CCT for Lightweight Proton Therapy Facility

@inproceedings{liao:sap2023-tupb014,
% --- JACoW template Dec 2024 ---
  author       = {Y.C. Liao and X. Liu and R.Y. Luo and B. Qin and W. Wang},
  title        = {{Design of a Large Momentum Acceptance Gantry Based on AG-CCT for Lightweight Proton Therapy Facility}},
  booktitle    = {Proc. 14th Symp. Accel. Phys. (SAP'23)},
  eventdate    = {2023-07-10/2023-07-12},
  pages        = {111--113},
  eid          = {TUPB014},
  language     = {english},
  keywords     = {toolkit, lattice, simulation, proton, optics},
  venue        = {Xichang, China},
  series       = {Symposium on Accelerator Physics},
  number       = {14},
  publisher    = {JACoW Publishing},
  location     = {Geneva, Switzerland},
  date         = {2024-11},
  month        = {11},
  year         = {2024},
  isbn         = {978-3-95450-265-3},
  doi          = {10.18429/JACoW-SAP2023-TUPB014},
  url          = {https://jacow.org/sap2023/papers/tupb014.pdf},
  abstract     = {{Superconducting (SC) gantry can be applied to proton therapy with significantly reduced footprint and weight. However, the relatively lower ramping limit of the SC magnetic field becomes a bottle-neck for fast energy change and beam delivery. The issue can be mitigated by designing a large momentum acceptance (LMA) beam optics. We present the design of an LMA gantry using AG-CCT SC magnets and symmetrical achromatic lattice. A fast degrader is combined in the design so that the gantry can rapidly switch energy during the treatment. The AG-CCT design process and beam transport simulation are all performed with our homemade integrated code CSPT, which has interfaces to Geant-4 and Opera, and can reach a maximum speed-up ratio of ~450 by applying parallel computation technique. The multi-particle simulation based on realistic field distribution proves that the gantry has a large momentum acceptance of ~20\%. Due to its large momentum acceptance, the dispersion effect caused by the scanning magnet is not neglectable. A dispersion compensation method, accompanied by a compact nozzle layout, is proposed to achieve a scanning field of 25×25 cm² with a maximum beam energy spread of 5.2\%.}},
}