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000902403 0247_ $$2doi$$a10.18429/JACOW-IPAC2021-MOPAB239
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000902403 037__ $$aFZJ-2021-04235
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000902403 1001_ $$0P:(DE-Juel1)187185$$aVitz, Maximilian$$b0$$eCorresponding author$$ufzj
000902403 1112_ $$aIPAC 2021$$cCampinas$$d2021-05-24 - 2021-05-28$$wBrazil
000902403 245__ $$aSimulation and Optimization of the Spin Coherence Time of Protons in a Prototype EDM Ring
000902403 260__ $$c2021
000902403 29510 $$aProceedings of the 12th International Particle Accelerator Conference, IPAC2021, Campinas, SP, Brazil
000902403 300__ $$a3 pages0.536 MB
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000902403 520__ $$aThe matter-antimatter asymmetry might be understood by investigating the EDM (Electric Dipole Moment) of elementary charged particles. A permanent EDM of a subatomic particle violates time-reversal and parity symmetry at the same time and would be, with the currently achievable experimental accuracy, a strong indication for physics beyond the Standard Model. The JEDI-Collaboration (Jülich Electric Dipole moment Investigations) in Jülich is preparing a direct EDM measurement for protons and deuterons: first at the storage ring COSY (COoler SYnchrotron) and later at a dedicated storage ring. A prototype EDM ring is an intermediate step before building the final storage ring to demonstrate sufficient beam lifetime and SCT (Spin Coherence Time) in a pure electrostatic ring as well as in a storage ring with combined electric and magnetic bending elements. In order to study the effect of E-B-deflectors on the orbit and the spin motion, the software library Bmad is used. The first results of the optics and spin simulations, with a focus on the optimization of the SCT, towards the prototype EDM ring will be discussed.
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000902403 650_7 $$2Other$$aAccelerator Physics
000902403 650_7 $$2Other$$aMC5: Beam Dynamics and EM Fields
000902403 65017 $$0V:(DE-MLZ)GC-2001-2016$$2V:(DE-HGF)$$aNuclei and Particles$$x0
000902403 7001_ $$0P:(DE-Juel1)131234$$aLehrach, Andreas$$b1$$ufzj
000902403 7001_ $$0P:(DE-HGF)0$$aShankar, Rahul$$b2
000902403 773__ $$a10.18429/JACOW-IPAC2021-MOPAB239
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