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@ARTICLE{Hejny:1043475,
author = {Hejny, V. and Andres, A. and Pretz, J. and Abusaif, F. and
Aggarwal, A. and Aksentev, A. and Alberdi, B. and Barion, L.
and Bekman, I. and Beyß, M. and Böhme, C. and Breitkreutz,
B. and Canale, N. and Ciullo, G. and Dymov, S. and
Fröhlich, N.-O. and Gebel, R. and Gaisser, M. and
Grigoryev, K. and Grzonka, D. and Hetzel, J. and
Javakhishvili, O. and Kacharava, A. and Kamerdzhiev, V. and
Karanth, S. and Keshelashvili, I. and Kononov, A. and
Laihem, K. and Lehrach, A. and Lenisa, P. and Lomidze, N.
and Lorentz, B. and Macharashvili, G. and Magiera, A. and
Mchedlishvili, D. and Melnikov, A. and Müller, F. and Nass,
A. and Nikolaev, N. N. and Okropiridze, D. and Pesce, A. and
Piccoli, A. and Poncza, V. and Prasuhn, D. and Rathmann, F.
and Saleev, A. and Shergelashvili, D. and Shmakova, V. and
Shankar, R. and Shurkhno, N. and Siddique, S. and Silenko,
A. and Slim, J. and Soltner, H. and Stassen, R. and
Stephenson, E. J. and Stroeher, Hans and Tabidze, M. and
Tagliente, G. and Valdau, Y. and Vitz, M. and Wagner, T. and
Wirzba, A. and Wrońska, A. and Wüstner, P. and Żurek, M.},
title = {{M}aintaining a resonance condition of an rf spin rotator
through a feedback loop in a storage ring},
journal = {Physical review accelerators and beams},
volume = {28},
number = {6},
issn = {2469-9888},
address = {College Park, MD},
publisher = {American Physical Society},
reportid = {FZJ-2025-02878},
pages = {062801},
year = {2025},
abstract = {This paper presents the successful application of a
phase-lock feedback system to maintain the resonance
condition of a radio frequency (rf) spin rotator
(specifically, an rf Wien filter) with respect to a 120 kHz
spin precession in the Cooler Synchrotron (COSY) storage
ring. Real-time monitoring of the spin precession and the rf
Wien filter signal allows the relative phase between the two
to be stabilized at an arbitrary setpoint. The feedback
system compensates for deviations in the relative phase by
adjusting the frequency and/or phase of the rf device as
needed. With this method, a variation in the phase relative
to the demanded value with a standard deviation of
𝜎Δ𝜑≈0.2 rad could be achieved. The system
was implemented in two runs aiming at a first direct
measurement of the deuteron electric dipole moment in 2018
and 2021. In addition, the difference between a single-bunch
beam affected by the spin rotator and a two-bunch system in
which only one bunch is exposed to the spin rotator fields
is discussed. Both methods have been used during these beam
times. The ability to keep the spin precession and the rf
fields synchronized is crucial for future investigations of
electric dipole moments of charged particles using storage
rings.},
cin = {IKP-2 / IKP-1 / IKP-4 / IKP-TA / IAS-4 / ZEA-2 / ZAT},
ddc = {530},
cid = {I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)IKP-1-20111104 /
I:(DE-Juel1)IKP-4-20111104 / I:(DE-Juel1)IKP-TA-20111104 /
I:(DE-Juel1)IAS-4-20090406 / I:(DE-Juel1)ZEA-2-20090406 /
I:(DE-Juel1)ZAT-20090406},
pnm = {613 - Matter and Radiation from the Universe (POF4-613) /
621 - Accelerator Research and Development (POF4-621) /
srEDM - Search for electric dipole moments using storage
rings (694340)},
pid = {G:(DE-HGF)POF4-613 / G:(DE-HGF)POF4-621 /
G:(EU-Grant)694340},
experiment = {EXP:(DE-Juel1)JEDI-20170712},
typ = {PUB:(DE-HGF)16},
UT = {WOS:001518851400001},
doi = {10.1103/PhysRevAccelBeams.28.062801},
url = {https://juser.fz-juelich.de/record/1043475},
}