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000132053 0247_ $$2doi$$a10.1103/PhysRevSTAB.15.124202
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000132053 041__ $$aEnglish
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000132053 1001_ $$0P:(DE-Juel1)VDB89344$$aBenati, P.$$b0$$eCorresponding author
000132053 245__ $$aSynchrotron oscillation effects on an rf-solenoid spin resonance
000132053 260__ $$a[S.l.] @$$bSoc.$$c2012
000132053 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2012-12-19
000132053 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2012-12-01
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000132053 520__ $$aNew measurements are reported for the time dependence of the vertical polarization of a 0.97 GeV/c deuteron beam circulating in a storage ring and perturbed by an rf solenoid. The storage ring is the cooler synchrotron (COSY) located at the Forschungszentrum Juelich. The beam polarization was measured continuously using a 1.5 cm thick carbon target located at the edge of the circulating deuteron beam and the scintillators of the EDDA detector. An rf solenoid mounted on the ring was used to generate fields at and near the frequency of the 1 - G spin resonance. Measurements were made of the vertical beam polarization as a function of time with the operation of the rf solenoid in either fixed or continuously variable frequency mode. Using rf-solenoid strengths as large as 2.66*10^5 revolutions/turn, slow oscillations ( 1 Hz) were observed in the vertical beam polarization. When the circulating beam was continuously electron cooled, these oscillations completely reversed the polarization and showed no sign of diminishing in amplitude. But for the uncooled beam, the oscillation amplitude was damped to nearly zero within a few seconds. A simple spin-tracking model without the details of the COSY ring lattice was successful in reproducing these oscillations and demonstrating the sensitivity of the damping to the magnitude of the synchrotron motion of the beam particles. The model demonstrates that the characteristic features of measurements made in the presence of large synchrotron oscillations are distinct from the features of such measurements when made off resonance. These data were collected in preparation for a study of the spin coherence time, a beam property that needs to become long to enable a search for an electric dipole moment using a storage ring.
000132053 536__ $$0G:(DE-HGF)POF2-53G32$$a53G - COSY (POF2-53G32)$$cPOF2-53G32$$fPOF II$$x0
000132053 542__ $$2Crossref$$i2012-12-19$$uhttp://creativecommons.org/licenses/by/3.0/
000132053 588__ $$aDataset connected to CrossRef, juser.fz-juelich.de
000132053 650_7 $$2INSPIRE$$adeuteron: beam
000132053 650_7 $$2INSPIRE$$abeam: polarization
000132053 650_7 $$2INSPIRE$$aspin: resonance
000132053 650_7 $$2INSPIRE$$acarbon: target
000132053 650_7 $$2INSPIRE$$asolenoid
000132053 650_7 $$2INSPIRE$$asynchrotron oscillation: effect
000132053 650_7 $$2INSPIRE$$ascintillation counter
000132053 650_7 $$2INSPIRE$$aJuelich COSY PS
000132053 650_7 $$2INSPIRE$$abeam dynamics
000132053 650_7 $$2INSPIRE$$aEDDA
000132053 650_7 $$2INSPIRE$$aelectric moment: measurement methods
000132053 650_7 $$2INSPIRE$$abeam profile
000132053 650_7 $$2INSPIRE$$apolarization: time dependence
000132053 693__ $$0EXP:(DE-Juel1)JEDI-20170712$$5EXP:(DE-Juel1)JEDI-20170712$$eJülich Electric Dipole moment Investigations$$x0
000132053 7001_ $$0P:(DE-Juel1)VDB69734$$aChiladze, D.$$b1
000132053 7001_ $$0P:(DE-Juel1)VDB284$$aDietrich, J.$$b2
000132053 7001_ $$0P:(DE-HGF)0$$aGaisser, M.$$b3
000132053 7001_ $$0P:(DE-Juel1)VDB5067$$aGebel, R.$$b4
000132053 7001_ $$0P:(DE-HGF)0$$aGuidoboni, G.$$b5
000132053 7001_ $$0P:(DE-Juel1)131187$$aHejny, V.$$b6
000132053 7001_ $$0P:(DE-Juel1)VDB713$$aKacharava, A.$$b7
000132053 7001_ $$0P:(DE-Juel1)131203$$aKamerdzhiev, Vsevolod$$b8$$ufzj
000132053 7001_ $$0P:(DE-Juel1)VDB4141$$aKulessa, P.$$b9
000132053 7001_ $$0P:(DE-Juel1)131234$$aLehrach, A.$$b10
000132053 7001_ $$0P:(DE-Juel1)VDB53860$$aLenisa, P.$$b11
000132053 7001_ $$0P:(DE-Juel1)VDB964$$aLorentz, B.$$b12
000132053 7001_ $$0P:(DE-Juel1)131248$$aMaier, R.$$b13
000132053 7001_ $$0P:(DE-Juel1)131251$$aMchedlishvili, D.$$b14
000132053 7001_ $$0P:(DE-HGF)0$$aMorse, W. M.$$b15
000132053 7001_ $$0P:(DE-HGF)0$$aÖllers, D.$$b16
000132053 7001_ $$0P:(DE-HGF)0$$aPesce, A.$$b17
000132053 7001_ $$0P:(DE-Juel1)VDB97444$$aPolyanskiy, A.$$b18
000132053 7001_ $$0P:(DE-Juel1)VDB61138$$aPrasuhn, D.$$b19
000132053 7001_ $$0P:(DE-Juel1)VDB71539$$aRathmann, F.$$b20
000132053 7001_ $$0P:(DE-HGF)0$$aSemertzidis, Y. K.$$b21
000132053 7001_ $$0P:(DE-HGF)0$$aStephenson, E. J.$$b22
000132053 7001_ $$0P:(DE-Juel1)VDB5270$$aStockhorst, H.$$b23
000132053 7001_ $$0P:(DE-HGF)0$$aStröher, H.$$b24
000132053 7001_ $$0P:(DE-HGF)0$$aTalman, R.$$b25
000132053 7001_ $$0P:(DE-Juel1)VDB43806$$aValdau, Yu.$$b26
000132053 7001_ $$0P:(DE-Juel1)131371$$aWeidemann, Ch.$$b27
000132053 7001_ $$0P:(DE-Juel1)133959$$aWüstner, P.$$b28
000132053 77318 $$2Crossref$$3journal-article$$a10.1103/physrevstab.15.124202$$bAmerican Physical Society (APS)$$d2012-12-19$$n12$$p124202$$tPhysical Review Special Topics - Accelerators and Beams$$v15$$x1098-4402$$y2012
000132053 773__ $$0PERI:(DE-600)2844143-6$$a10.1103/PhysRevSTAB.15.124202$$gVol. 15, no. 12, p. 124202$$n12$$p124202$$tPhysical review accelerators and beams$$v15$$x1098-4402$$y2012
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000132053 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/0168-9002(90)90128-S
000132053 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/0168-9002(90)90129-T
000132053 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/S0168-9002(97)01135-2
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