We recently studied the spin flipping of a 202.7 MeV vertically polarized proton beam stored in the Indiana University Cyclotron Facility cooler ring during the first polarized run with its new cooler injector synchrotron and its new cooler injector polarized ion source. We first set the vertical betatron tune to avoid the measured ny value of the Gg 7 2n y intrinsic depolarizing resonance in the cooler ring. We then flipped the spin by ramping the frequency of an rf dipole through an rf-induced depolarizing resonance. After optimizing the rf dipole’s frequency ramp parameters, we used multiple spin flips to measure a maximum spin-flip efficiency of 97.5 6 1%. PACS numbers: 29.27.Bd, 29.27.Hj, 41.75.Ak There is a growing interest in polarized beam experiments in storage rings such as the Indiana University Cyclotron Facility (IUCF) cooler ring [1], the MIT-Bates storage ring [2], the Brookhaven relativistic heavy ion collider (RHIC) [3], and HERA at DESY [4]. Frequent reversals of the beam polarization direction can significantly reduce the systematic errors in an experiment’s spin asymmetry measurements. An rf solenoid was used earlier [5] to spin flip a vertically polarized proton beam stored in the cooler ring with no Siberian snake [6]. Since a solenoid’s spin rotation decreases linearly with energy, a solenoid is impractical for spin flipping in high energy rings. However, a dipole’s spin rotation is energy independent. Therefore, we recently used an rf dipole to spin flip a 202.7 MeV vertically polarized proton beam stored in the IUCF cooler ring with no Siberian snake. In any flat circular accelerator or storage ring with no horizontal magnetic fields, each proton’s spin precesses around the vertical fields of the ring’s dipole magnets. The spin tune ns, which is the number of spin precessions during one turn around the ring, is proportional to the proton’s energy
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