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Phase Locking the Spin Precession in a Storage Ring.
Hempelmann, N; Hejny, V; Pretz, J; Stephenson, E; Augustyniak, W; Bagdasarian, Z; Bai, M; Barion, L; Berz, M; Chekmenev, S; Ciullo, G; Dymov, S; Etzkorn, F-J; Eversmann, D; Gaisser, M; Gebel, R; Grigoryev, K; Grzonka, D; Guidoboni, G; Hanraths, T; Heberling, D; Hetzel, J; Hinder, F; Kacharava, A; Kamerdzhiev, V; Keshelashvili, I; Koop, I; Kulikov, A; Lehrach, A; Lenisa, P; Lomidze, N; Lorentz, B; Maanen, P; Macharashvili, G; Magiera, A; Mchedlishvili, D; Mey, S; Müller, F; Nass, A; Nikolaev, N N; Pesce, A; Prasuhn, D; Rathmann, F; Rosenthal, M; Saleev, A; Schmidt, V; Semertzidis, Y; Shmakova, V; Silenko, A; Slim, J.
Afiliação
  • Hempelmann N; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Hejny V; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Pretz J; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Stephenson E; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Augustyniak W; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Bagdasarian Z; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Bai M; Indiana University Center for Spacetime Symmetries, Bloomington, Indiana 47405, USA.
  • Barion L; Department of Nuclear Physics, National Centre for Nuclear Research, 00681 Warsaw, Poland.
  • Berz M; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Chekmenev S; High Energy Physics Institute, Tbilisi State University, 0186 Tbilisi, Georgia.
  • Ciullo G; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Dymov S; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Etzkorn FJ; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Eversmann D; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Gaisser M; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Gebel R; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Grigoryev K; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Grzonka D; Laboratory of Nuclear Problems, Joint Institute for Nuclear Research, 141980 Dubna, Russia.
  • Guidoboni G; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Hanraths T; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Heberling D; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Hetzel J; Center for Axion and Precision Physics Research, Institute for Basic Science (IBS), Daejeon 34141, Republic of Korea.
  • Hinder F; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Kacharava A; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Kamerdzhiev V; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Keshelashvili I; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Koop I; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Kulikov A; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Lehrach A; Institut für Hochfrequenztechnik, RWTH Aachen University, 52056 Aachen, Germany.
  • Lenisa P; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Lomidze N; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Lorentz B; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Maanen P; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Macharashvili G; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Magiera A; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Mchedlishvili D; Budker Institute of Nuclear Physics, 630090 Novosibirsk, Russia.
  • Mey S; Laboratory of Nuclear Problems, Joint Institute for Nuclear Research, 141980 Dubna, Russia.
  • Müller F; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Nass A; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Nikolaev NN; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Pesce A; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Prasuhn D; High Energy Physics Institute, Tbilisi State University, 0186 Tbilisi, Georgia.
  • Rathmann F; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Rosenthal M; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Saleev A; High Energy Physics Institute, Tbilisi State University, 0186 Tbilisi, Georgia.
  • Schmidt V; Laboratory of Nuclear Problems, Joint Institute for Nuclear Research, 141980 Dubna, Russia.
  • Semertzidis Y; Institute of Physics, Jagiellonian University, 30348 Cracow, Poland.
  • Shmakova V; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Silenko A; High Energy Physics Institute, Tbilisi State University, 0186 Tbilisi, Georgia.
  • Slim J; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
Phys Rev Lett ; 119(1): 014801, 2017 Jul 07.
Article em En | MEDLINE | ID: mdl-28731757
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.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2017 Tipo de documento: Article País de afiliação: Alemanha

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2017 Tipo de documento: Article País de afiliação: Alemanha