000188209 001__ 188209
000188209 005__ 20210129215144.0
000188209 037__ $$aFZJ-2015-01651
000188209 041__ $$aEnglish
000188209 1001_ $$0P:(DE-Juel1)156478$$aMey, Sebastian$$b0$$eCorresponding Author$$ufzj
000188209 1112_ $$aDPG-Frühjahrstagung der Sektion Kondensierte Materie$$cDresden$$d2014-03-30 - 2014-04-04$$gDPG Dresden 2014$$wGermany
000188209 245__ $$aAn RF E×B Dipole for Spin Manipulation at COSY - Prototype Commissioning and First Measurements
000188209 260__ $$c2014
000188209 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1425394118_24708$$xOther
000188209 3367_ $$033$$2EndNote$$aConference Paper
000188209 3367_ $$2DataCite$$aOther
000188209 3367_ $$2ORCID$$aLECTURE_SPEECH
000188209 3367_ $$2DRIVER$$aconferenceObject
000188209 3367_ $$2BibTeX$$aINPROCEEDINGS
000188209 520__ $$aPermanent EDMs (Electric Dipole Moments) of fundamental particles violate both time invariance and parity and thus, according to the CPT theorem, imply CP violation. The standard model prediction for the EDM gives unobservably small magnitudes, therefore any measurement of non-vanishing EDMs would be a signature of “new physics”.The JEDI Collaboration investigates the feasibility of EDM experiments with charged hadrons in dedicated storage rings. They incorporate measurements with horizontally polarized particles. To maximize the lifetime of the horizontal polarization, systematic studies of unwanted spin rotations utilizing for instance a vertical RF-B field are required. To avoid kicking the beam in the horizontal plane, the resulting Lorentz force needs to be compensated by the force of an orthogonal electric field, leading to a Wien-Filter configuration. For preliminary studies, the Cooler Synchrotron COSY is currently being supplemented with a new RF-E-B-Dipole.The talk will incorporate the setup of the new system from the RF-Supply to the electrode and coil configuration providing the electromagnetic fields, as well as the commissioning and first measurements taken at COSY.
000188209 536__ $$0G:(DE-HGF)POF2-53G32$$a53G - COSY (POF2-53G32)$$cPOF2-53G32$$fPOF II$$x0
000188209 65027 $$0V:(DE-MLZ)SciArea-230$$2V:(DE-HGF)$$aParticle Physics$$x0
000188209 65027 $$0V:(DE-MLZ)SciArea-220$$2V:(DE-HGF)$$aInstrument and Method Development$$x1
000188209 65027 $$0V:(DE-MLZ)SciArea-200$$2V:(DE-HGF)$$aNuclear Physics$$x2
000188209 65017 $$0V:(DE-MLZ)GC-160$$2V:(DE-HGF)$$aFundamental Science $$x0
000188209 693__ $$0EXP:(DE-Juel1)JEDI-20170712$$5EXP:(DE-Juel1)JEDI-20170712$$eJülich Electric Dipole moment Investigations$$x0
000188209 773__ $$y2014
000188209 8564_ $$uhttp://collaborations.fz-juelich.de/ikp/jedi/public_files/usual_event/2014-03-31.pdf
000188209 8564_ $$uhttps://juser.fz-juelich.de/record/188209/files/FZJ-2015-01651.pdf$$yRestricted
000188209 909CO $$ooai:juser.fz-juelich.de:188209$$pVDB
000188209 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)156478$$aForschungszentrum Jülich GmbH$$b0$$kFZJ
000188209 9132_ $$0G:(DE-HGF)POF3-631$$1G:(DE-HGF)POF3-630$$2G:(DE-HGF)POF3-600$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vAccelerator R & D$$x0
000188209 9131_ $$0G:(DE-HGF)POF2-53G32$$1G:(DE-HGF)POF2-530$$2G:(DE-HGF)POF2-500$$3G:(DE-HGF)POF2$$4G:(DE-HGF)POF$$aDE-HGF$$bStruktur der Materie$$lPhysik der Hadronen und Kerne$$vCOSY$$x0
000188209 9141_ $$y2014
000188209 920__ $$lyes
000188209 9201_ $$0I:(DE-Juel1)IKP-4-20111104$$kIKP-4$$lKernphysikalische Großgeräte$$x0
000188209 980__ $$aconf
000188209 980__ $$aVDB
000188209 980__ $$aI:(DE-Juel1)IKP-4-20111104
000188209 980__ $$aUNRESTRICTED