A study of Polarized Proton Acceleration in j-parc a. U. Luccio, M. Bai, T. Roser



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A Study of Polarized Proton Acceleration in J-PARC

  • A.U.Luccio, M.Bai, T.Roser

  • Brookhaven National Laboratory, Upton, NY 11973, USA

  • A.Molodojentsev, C.Ohmori, H.Sato

  • High Energy Accelerator Research Organization, Tsukuba, Ibaraki, Japan

  • H.Hatanaka

  • Research Center for Nuclear Physics, Osaka University, Japan


Layout of J-PARC for polarized proton acceleration



Setup for accelerating polarized protons at J-PARC

    • Optically Pumped Polarized Ion Source: 1012 H- per 0.5 ms pulse and > 5 Hz rep. rate, 85% polarization (similar to KEK-TRIUMF-BNL OPPIS)
    • Bunch emittance: ~ 5  rad and 0.3 eVs for 2  1011 protons (required for polarized beam acceleration)
    • Linac: No depolarization
    • RCS (25 Hz, y = 6.35, P = 3, Ekin = .18 … 3 GeV, G = 2.2 … 7.5)
      • 5 imperfection resonances; harmonic correction needed for G = 7
      • Intrinsic resonances:
        • G = 2.65 (9- y), 3.35 (-3+ y), 5.65 (12- y), 6.35 (0+ y)
        • Full spin flip with rf dipole: 20 Gm gives > .99 spin-flip (seems feasible)
        • Avoid depolarization with tune jump: y = 0.2 in 6 turns  large aperture ferrite quadrupoles with fast pulsing power supplies (difficult)


Intrinsic Spin Resonance at RCS – Rapid Cyclic Synchrotron



Issues of accelerating polarized protons in Main Ring

    • Beam energy: 3  50 GeV (G = 7.5  97.5)
    • Design working point: x = 22.34; y = 20.27
    • Many imperfection resonances
    • Strong intrinsic resonances
    • No space for full snake installation




Solution of accelerating polarized protons in Main Ring



12 particles at 4  rad (1.5 beam sigma)

    • 12 particles at 4  rad (1.5 beam sigma)
    • Two 30% synthetic snakes
    • Working point:
      • x = 22.128
      • y = 20.960




Main Ring Partial Snake

  • AGS type of cold snake

  • magnetic field strength: 3.4 Tesla

    • snake strength 30% (540 spin rotation angle) at injection and gets weaker at higher energy according to:




Matching of the INSA with snake at the energy =11



Matching snakes to the lattice



Solution of Correcting Quadrupoles





Conclusion

  • Possible to accelerate polarized protons of 10 mm-mrad in the J-PARC Main Ring using two 30% partial snakes of AGS type.

  • The perturbation on the MR optics from snakes is significant at low energy. This can be minimized by using a correcting quadrupole doublet each at the entrance and exit of each snake.

  • Tracking with the code Spink using synthetic snakes with variable strength and a static lattice shows good polarization survival.



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