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Author: K. Seiya


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Reference
A. Narayanan et al., “Machine Learning for Slow Spill Regulation in the Fermilab Delivery Ring for Mu2e”, in Proc. North American Particle Accelerator Conf. (NAPAC'22), Albuquerque, NM, USA, Aug. 2022, pp. 214-217.
A. Narayanan et al., “Optimizing Mu2e Spill Regulation System Algorithms”, in Proc. 12th Int. Particle Accelerator Conf. (IPAC'21), Campinas, Brazil, May 2021, pp. 4281-4284.
A. V. Shemyakin, R. Prakash, and K. Seiya, “Finding Beam Loss Locations in a Linac with Oscillating Dipole Correctors”, in Proc. North American Particle Accelerator Conf. (NAPAC'19), Lansing, MI, USA, Sep. 2019, pp. 663-666.
B. C. Brown et al., “Fermilab Main Injector Collimation Systems: Design, Commissioning and Operation”, in Proc. 23rd Particle Accelerator Conf. (PAC'09), Vancouver, Canada, May 2009, paper WE6RFP025, pp. 2841-2843.
C. M. Bhat et al., “Energy Spread of the Proton Beam in the Fermilab Booster at Its Injection Energy”, in Proc. 6th Int. Particle Accelerator Conf. (IPAC'15), Richmond, VA, USA, May 2015, pp. 3979-3981.
C. M. Bhat et al., “Foil Scattering Model for Fermilab Booster”, in Proc. North American Particle Accelerator Conf. (NAPAC'19), Lansing, MI, USA, Sep. 2019, pp. 632-635.
C. M. Bhat et al., “Mixed pbar Source Operation at the Fermilab Tevatron”, in Proc. 21st Particle Accelerator Conf. (PAC'05), Knoxville, TN, USA, May 2005, paper TPAP022, pp. 1763-1765.
C.-Y. Tan, D. S. Bollinger, B. A. Schupbach, and K. Seiya, “Hydrogen and Cesium Monitor for H- Magnetron Sources”, in Proc. 5th Int. Particle Accelerator Conf. (IPAC'14), Dresden, Germany, Jun. 2014, pp. 617-619.
C.-Y. Tan, L. R. Prost, K. Seiya, and A. K. Triplett, “Optics Corrections with LOCO in the Fermilab Booster”, in Proc. 7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 2016, pp. 3385-3387.
D. C. Jones, D. S. Bollinger, V. V. Kapin, and K. Seiya, “Investigation of the Beam Propagation Through the FNAL LEBT”, in Proc. 31st Linear Accelerator Conf. (LINAC'22), Liverpool, UK, Aug.-Sep. 2022, pp. 597-600.


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