001041519 001__ 1041519
001041519 005__ 20250424202216.0
001041519 0247_ $$2datacite_doi$$a10.34734/FZJ-2025-02293
001041519 037__ $$aFZJ-2025-02293
001041519 1001_ $$0P:(DE-Juel1)131187$$aHejny, Volker$$b0$$eCorresponding author$$ufzj
001041519 1112_ $$aPolarized Ion Sources and Beams at EIC$$cStony Brook$$d2025-03-10 - 2025-03-12$$wUSA
001041519 245__ $$aSpin tune determination and feedback
001041519 260__ $$c2025
001041519 3367_ $$033$$2EndNote$$aConference Paper
001041519 3367_ $$2DataCite$$aOther
001041519 3367_ $$2BibTeX$$aINPROCEEDINGS
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001041519 3367_ $$2ORCID$$aLECTURE_SPEECH
001041519 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1745478203_10185$$xInvited
001041519 520__ $$aThe talk covers over 10 years of R&D by the JEDI collaboration at COSY, Jülich. Main topics discussed are: online determination of spin tune and in-plane polarization, how to achieve large spin coherence times, and phase-lock feedback for synchronizing spin precession and RF devices. The R&D is primarily motivated by precision experiments on Electric Dipole Moments (EDMs) of charged particles in storage rings, including feasibility studies and a first deuteron EDM measurement at COSY.
001041519 536__ $$0G:(DE-HGF)POF4-612$$a612 - Cosmic Matter in the Laboratory (POF4-612)$$cPOF4-612$$fPOF IV$$x0
001041519 536__ $$0G:(EU-Grant)694340$$asrEDM - Search for electric dipole moments using storage rings (694340)$$c694340$$fERC-2015-AdG$$x1
001041519 693__ $$0EXP:(DE-Juel1)JEDI-20170712$$5EXP:(DE-Juel1)JEDI-20170712$$eJülich Electric Dipole moment Investigations$$x0
001041519 8564_ $$uhttps://juser.fz-juelich.de/record/1041519/files/Presentation.pdf$$yOpenAccess
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001041519 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131187$$aForschungszentrum Jülich$$b0$$kFZJ
001041519 9131_ $$0G:(DE-HGF)POF4-612$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vCosmic Matter in the Laboratory$$x0
001041519 9141_ $$y2025
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001041519 9201_ $$0I:(DE-Juel1)IKP-2-20111104$$kIKP-2$$lExperimentelle Hadrondynamik$$x0
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