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001     188209
005     20210129215144.0
037 _ _ |a FZJ-2015-01651
041 _ _ |a English
100 1 _ |a Mey, Sebastian
|0 P:(DE-Juel1)156478
|b 0
|e Corresponding Author
|u fzj
111 2 _ |a DPG-Frühjahrstagung der Sektion Kondensierte Materie
|g DPG Dresden 2014
|c Dresden
|d 2014-03-30 - 2014-04-04
|w Germany
245 _ _ |a An RF E×B Dipole for Spin Manipulation at COSY - Prototype Commissioning and First Measurements
260 _ _ |c 2014
336 7 _ |a Conference Presentation
|b conf
|m conf
|0 PUB:(DE-HGF)6
|s 1425394118_24708
|2 PUB:(DE-HGF)
|x Other
336 7 _ |a Conference Paper
|0 33
|2 EndNote
336 7 _ |a Other
|2 DataCite
336 7 _ |a LECTURE_SPEECH
|2 ORCID
336 7 _ |a conferenceObject
|2 DRIVER
336 7 _ |a INPROCEEDINGS
|2 BibTeX
520 _ _ |a Permanent 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.
536 _ _ |a 53G - COSY (POF2-53G32)
|0 G:(DE-HGF)POF2-53G32
|c POF2-53G32
|f POF II
|x 0
650 2 7 |a Particle Physics
|0 V:(DE-MLZ)SciArea-230
|2 V:(DE-HGF)
|x 0
650 2 7 |a Instrument and Method Development
|0 V:(DE-MLZ)SciArea-220
|2 V:(DE-HGF)
|x 1
650 2 7 |a Nuclear Physics
|0 V:(DE-MLZ)SciArea-200
|2 V:(DE-HGF)
|x 2
650 1 7 |a Fundamental Science
|0 V:(DE-MLZ)GC-160
|2 V:(DE-HGF)
|x 0
693 _ _ |5 EXP:(DE-Juel1)JEDI-20170712
|e Jülich Electric Dipole moment Investigations
|x 0
|0 EXP:(DE-Juel1)JEDI-20170712
773 _ _ |y 2014
856 4 _ |u http://collaborations.fz-juelich.de/ikp/jedi/public_files/usual_event/2014-03-31.pdf
856 4 _ |u https://juser.fz-juelich.de/record/188209/files/FZJ-2015-01651.pdf
|y Restricted
909 C O |o oai:juser.fz-juelich.de:188209
|p VDB
910 1 _ |a Forschungszentrum Jülich GmbH
|0 I:(DE-588b)5008462-8
|k FZJ
|b 0
|6 P:(DE-Juel1)156478
913 2 _ |a DE-HGF
|b Forschungsbereich Materie
|l Materie und Technologie
|1 G:(DE-HGF)POF3-630
|0 G:(DE-HGF)POF3-631
|2 G:(DE-HGF)POF3-600
|v Accelerator R & D
|x 0
913 1 _ |a DE-HGF
|b Struktur der Materie
|l Physik der Hadronen und Kerne
|1 G:(DE-HGF)POF2-530
|0 G:(DE-HGF)POF2-53G32
|2 G:(DE-HGF)POF2-500
|v COSY
|x 0
|4 G:(DE-HGF)POF
|3 G:(DE-HGF)POF2
914 1 _ |y 2014
920 _ _ |l yes
920 1 _ |0 I:(DE-Juel1)IKP-4-20111104
|k IKP-4
|l Kernphysikalische Großgeräte
|x 0
980 _ _ |a conf
980 _ _ |a VDB
980 _ _ |a I:(DE-Juel1)IKP-4-20111104
980 _ _ |a UNRESTRICTED

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