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@ARTICLE{Hempelmann:834558,
author = {Hempelmann, N. and Hejny, V. and Pretz, J. and Stephenson,
E. and Augustyniak, W. and Bagdasarian, Z. and Bai, M. and
Barion, L. and Berz, M. and Chekmenev, S. and Ciullo, G. and
Dymov, S. and Etzkorn, F.-J. and Eversmann, D. and Gaisser,
M. and Gebel, R. and Grigoryev, K. and Grzonka, D. and
Guidoboni, G. and Hahnraths - von der Gracht, Tanja and
Heberling, D. and Hetzel, J. and Hinder, F. and Kacharava,
A. and Kamerdzhiev, V. and Keshelashvili, I. and Koop, I.
and Kulikov, A. and Lehrach, A. and Lenisa, P. and Lomidze,
N. and Lorentz, B. and Maanen, P. and Macharashvili, G. and
Magiera, A. and Mchedlishvili, D. and Mey, S. and Müller,
F. and Nass, A. and Nikolaev, N. N. and Pesce, A. and
Prasuhn, D. and Rathmann, F. and Rosenthal, M. and Saleev,
A. and Schmidt, V. and Semertzidis, Y. and Shmakova, V. and
Silenko, A. and Slim, J. and Soltner, H. and Stahl, A. and
Stassen, R. and Stockhorst, H. and Stroeher, Hans and
Tabidze, M. and Tagliente, G. and Talman, R. and Thörngren
Engblom, P. and Trinkel, F. and Uzikov, Yu. and Valdau, Yu.
and Valetov, E. and Vassiliev, A. and Weidemann, C. and
Wrońska, A. and Wüstner, P. and Zuprański, P. and Żurek,
M.},
title = {{P}hase {L}ocking the {S}pin {P}recession in a {S}torage
{R}ing},
journal = {Physical review letters},
volume = {119},
number = {1},
issn = {1079-7114},
address = {College Park, Md.},
publisher = {APS},
reportid = {FZJ-2017-04486},
pages = {014801},
year = {2017},
abstract = {This Letter reports the successful use of feedback from a
spin polarization measurement to the revolution frequency of
a 0.97 GeV/c bunched and polarized deuteron beam in the
Cooler Synchrotron (COSY) storage ring in order to control
both the precession rate (≈121 kHz) and the phase of
the horizontal polarization component. Real time
synchronization with a radio frequency (rf) solenoid made
possible the rotation of the polarization out of the
horizontal plane, yielding a demonstration of the feedback
method to manipulate the polarization. In particular, the
rotation rate shows a sinusoidal function of the horizontal
polarization phase (relative to the rf solenoid), which was
controlled to within a 1 standard deviation range of
σ=0.21 rad. The minimum possible adjustment was 3.7
mHz out of a revolution frequency of 753 kHz, which changes
the precession rate by 26 mrad/s. Such a capability
meets a requirement for the use of storage rings to look for
an intrinsic electric dipole moment of charged particles.},
cin = {IKP-2 / IKP-4 / IKP-1 / IKP-TA / ZEA-2 / ZEA-1},
ddc = {550},
cid = {I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)IKP-4-20111104 /
I:(DE-Juel1)IKP-1-20111104 / I:(DE-Juel1)IKP-TA-20111104 /
I:(DE-Juel1)ZEA-2-20090406 / I:(DE-Juel1)ZEA-1-20090406},
pnm = {612 - Cosmic Matter in the Laboratory (POF3-612) / 631 -
Accelerator R $\&$ D (POF3-631) / srEDM - Search for
electric dipole moments using storage rings (694340)},
pid = {G:(DE-HGF)POF3-612 / G:(DE-HGF)POF3-631 /
G:(EU-Grant)694340},
experiment = {EXP:(DE-Juel1)JEDI-20170712},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000418530600001},
pubmed = {pmid:28731757},
doi = {10.1103/PhysRevLett.119.014801},
url = {https://juser.fz-juelich.de/record/834558},
}