000858237 001__ 858237
000858237 005__ 20210129235905.0
000858237 037__ $$aFZJ-2018-07137
000858237 041__ $$aEnglish
000858237 1001_ $$0P:(DE-Juel1)131267$$aNass, Alexander$$b0$$eCorresponding author$$ufzj
000858237 1112_ $$a23rd International Spin Symposium$$cFerrara$$d2018-09-10 - 2018-09-14$$gSPIN 2018$$wItaly
000858237 245__ $$aCommissioning of the RF Wien filter for a first deuteron EDM measurement at COSY / Jülich
000858237 260__ $$c2018
000858237 3367_ $$033$$2EndNote$$aConference Paper
000858237 3367_ $$2DataCite$$aOther
000858237 3367_ $$2BibTeX$$aINPROCEEDINGS
000858237 3367_ $$2DRIVER$$aconferenceObject
000858237 3367_ $$2ORCID$$aLECTURE_SPEECH
000858237 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1547469481_18910$$xPlenary/Keynote
000858237 520__ $$aThe JEDI Collaboration (Jülich Electric Dipole Investigations) aims for a measurement of the electric dipole moments (EDMs) of Deuterons and Protons at the COoler SYnchrotron (COSY). To make this possible, a novel high precision waveguide RF Wien filter was installed in COSY inside a so-called low-beta section, to modulate the spin of deuterons and protons. With this device the force of the radial electric field iscanceled by the corresponding vertical magnetic force. So it is possible to directly manipulate the polarization vector of the particles without introducing any beam oscillations. The RF Wien filter has been designed tooperate at harmonics of the spin precession frequency ranging from 0.6 to 1.7 MHz. For systematic investigations of sources of false EDM signals, the waveguide RF Wien filter can be rotated by 90 degrees around the beamaxis. The results of several weeks of commissioning experiments at COSY with the RF Wien filter, including Lorentz force measurements, driven oscillations and the resonant build-up of vertical polarization will be presented. A series of test measurements similar to the the upcoming first Deuteron EDM measurement were performed as well.
000858237 536__ $$0G:(DE-HGF)POF3-612$$a612 - Cosmic Matter in the Laboratory (POF3-612)$$cPOF3-612$$fPOF III$$x0
000858237 536__ $$0G:(DE-HGF)POF3-631$$a631 - Accelerator R & D (POF3-631)$$cPOF3-631$$fPOF III$$x1
000858237 536__ $$0G:(EU-Grant)694340$$asrEDM - Search for electric dipole moments using storage rings (694340)$$c694340$$fERC-2015-AdG$$x2
000858237 65027 $$0V:(DE-MLZ)SciArea-230$$2V:(DE-HGF)$$aParticle Physics$$x0
000858237 65017 $$0V:(DE-MLZ)GC-2001-2016$$2V:(DE-HGF)$$aNuclei and Particles$$x0
000858237 693__ $$0EXP:(DE-Juel1)JEDI-20170712$$5EXP:(DE-Juel1)JEDI-20170712$$eJülich Electric Dipole moment Investigations$$x0
000858237 8564_ $$uhttp://spin2018.unife.it/
000858237 909CO $$ooai:juser.fz-juelich.de:858237$$pec_fundedresources$$pVDB$$popenaire
000858237 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131267$$aForschungszentrum Jülich$$b0$$kFZJ
000858237 9131_ $$0G:(DE-HGF)POF3-612$$1G:(DE-HGF)POF3-610$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Universum$$vCosmic Matter in the Laboratory$$x0
000858237 9131_ $$0G:(DE-HGF)POF3-631$$1G:(DE-HGF)POF3-630$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vAccelerator R & D$$x1
000858237 9141_ $$y2018
000858237 920__ $$lyes
000858237 9201_ $$0I:(DE-Juel1)IKP-2-20111104$$kIKP-2$$lExperimentelle Hadrondynamik$$x0
000858237 980__ $$aconf
000858237 980__ $$aVDB
000858237 980__ $$aI:(DE-Juel1)IKP-2-20111104
000858237 980__ $$aUNRESTRICTED