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@ARTICLE{Guidoboni:856552,
author = {Guidoboni, G. and Stephenson, E. J. and Wrońska, A. and
Bagdasarian, Z. and Bsaisou, J. and Chekmenev, S. and
Ciullo, G. and Dymov, S. and Eversmann, D. and Gaisser, M.
and Gebel, R. and Hejny, V. and Hempelmann, N. and Hinder,
F. and Kacharava, A. and Keshelashvili, I. and Kulessa, P.
and Lenisa, P. and Lehrach, A. and Lorentz, B. and Maanen,
P. and Maier, R. and Mchedlishvili, D. and Mey, S. and Nass,
A. and Pesce, A. and Orlov, Y. and Pretz, J. and Prasuhn, D.
and Rathmann, F. and Rosenthal, M. and Saleev, A. and
Semertzidis, Y. K. and Senichev, Y. and Shmakova, V. and
Stockhorst, H. and Stroeher, Hans and Talman, R. and
Thörngren Engblom, P. and Trinkel, F. and Valdau, Yu. and
Weidemann, C. and Wüstner, P. and Żurek, M. and Zyuzin,
D.},
title = {{C}onnection between zero chromaticity and long in-plane
polarization lifetime in a magnetic storage ring},
journal = {Physical review accelerators and beams},
volume = {21},
number = {2},
issn = {2469-9888},
address = {College Park, MD},
publisher = {American Physical Society},
reportid = {FZJ-2018-05935},
pages = {024201},
year = {2018},
abstract = {In this paper, we demonstrate the connection between a
magnetic storage ring with additional sextupole fields set
so that the x and y chromaticities vanish and the maximizing
of the lifetime of in-plane polarization (IPP) for a
0.97−GeV/c deuteron beam. The IPP magnitude was measured
by continuously monitoring the down-up scattering asymmetry
(sensitive to sideways polarization) in an in-beam,
carbon-target polarimeter and unfolding the precession of
the IPP due to the magnetic anomaly of the deuteron. The
optimum operating conditions for a long IPP lifetime were
made by scanning the field of the storage ring sextupole
magnet families while observing the rate of IPP loss during
storage of the beam. The beam was bunched and electron
cooled. The IPP losses appear to arise from the change of
the orbit circumference, and consequently the particle speed
and spin tune, due to the transverse betatron oscillations
of individual particles in the beam. The effects of these
changes are canceled by an appropriate sextupole field
setting.},
cin = {IKP-2 / IKP-4 / ZEA-2},
ddc = {530},
cid = {I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)IKP-4-20111104 /
I:(DE-Juel1)ZEA-2-20090406},
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:000424386900001},
doi = {10.1103/PhysRevAccelBeams.21.024201},
url = {https://juser.fz-juelich.de/record/856552},
}