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New Method for a Continuous Determination of the Spin Tune in Storage Rings and Implications for Precision Experiments.
Eversmann, D; Hejny, V; Hinder, F; Kacharava, A; Pretz, J; Rathmann, F; Rosenthal, M; Trinkel, F; Andrianov, S; Augustyniak, W; Bagdasarian, Z; Bai, M; Bernreuther, W; Bertelli, S; Berz, M; Bsaisou, J; Chekmenev, S; Chiladze, D; Ciullo, G; Contalbrigo, M; de Vries, J; Dymov, S; Engels, R; Esser, F M; Felden, O; Gaisser, M; Gebel, R; Glückler, H; Goldenbaum, F; Grigoryev, K; Grzonka, D; Guidoboni, G; Hanhart, C; Heberling, D; Hempelmann, N; Hetzel, J; Hipple, R; Hölscher, D; Ivanov, A; Kamerdzhiev, V; Kamys, B; Keshelashvili, I; Khoukaz, A; Koop, I; Krause, H-J; Krewald, S; Kulikov, A; Lehrach, A; Lenisa, P; Lomidze, N.
Afiliação
  • Eversmann D; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Hejny V; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Hinder F; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Kacharava A; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Pretz J; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Rathmann F; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Rosenthal M; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Trinkel F; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Andrianov S; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Augustyniak W; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Bagdasarian Z; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Bai M; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Bernreuther W; Faculty of Applied Mathematics and Control Processes, Saint Petersburg State University, 198504 Saint Petersburg, Russia.
  • Bertelli S; Department of Nuclear Physics, National Centre for Nuclear Research, 00681 Warsaw, Poland.
  • Berz M; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Bsaisou J; High Energy Physics Institute, Tbilisi State University, 0186 Tbilisi, Georgia.
  • Chekmenev S; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Chiladze D; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Ciullo G; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Contalbrigo M; Institut für Theoretische Teilchenphysik und Kosmologie, RWTH Aachen University, 52056 Aachen, Germany.
  • de Vries J; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Dymov S; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Engels R; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Esser FM; Institute for Advanced Simulation, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Felden O; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Gaisser M; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Gebel R; High Energy Physics Institute, Tbilisi State University, 0186 Tbilisi, Georgia.
  • Glückler H; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Goldenbaum F; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Grigoryev K; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Grzonka D; Institute for Advanced Simulation, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Guidoboni G; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Hanhart C; Laboratory of Nuclear Problems, Joint Institute for Nuclear Research, 141980 Dubna, Russia.
  • Heberling D; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Hempelmann N; Zentralinstitut für Engineering, Elektronik und Analytik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Hetzel J; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Hipple R; Center for Axion and Precision Physics Research, Institute for Basic Science, 291 Daehak-ro, Yuseong-gu, Daejeon 305-701, Republic of Korea.
  • Hölscher D; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Ivanov A; Zentralinstitut für Engineering, Elektronik und Analytik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Kamerdzhiev V; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Kamys B; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Keshelashvili I; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Khoukaz A; University of Ferrara and INFN, 44100 Ferrara, Italy.
  • Koop I; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Krause HJ; Institute for Advanced Simulation, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Krewald S; JARA-FAME (Forces and Matter Experiments), Forschungszentrum Jülich and RWTH Aachen University, 52056 Aachen, Germany.
  • Kulikov A; Institut für Hochfrequenztechnik, RWTH Aachen University, 52056 Aachen, Germany.
  • Lehrach A; III. Physikalisches Institut B, RWTH Aachen University, 52056 Aachen, Germany.
  • Lenisa P; Institut für Kernphysik, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Lomidze N; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
Phys Rev Lett ; 115(9): 094801, 2015 Aug 28.
Article em En | MEDLINE | ID: mdl-26371657
A new method to determine the spin tune is described and tested. In an ideal planar magnetic ring, the spin tune-defined as the number of spin precessions per turn-is given by ν(s)=γG (γ is the Lorentz factor, G the gyromagnetic anomaly). At 970 MeV/c, the deuteron spins coherently precess at a frequency of ≈120 kHz in the Cooler Synchrotron COSY. The spin tune is deduced from the up-down asymmetry of deuteron-carbon scattering. In a time interval of 2.6 s, the spin tune was determined with a precision of the order 10^{-8}, and to 1×10^{-10} for a continuous 100 s accelerator cycle. This renders the presented method a new precision tool for accelerator physics; controlling the spin motion of particles to high precision is mandatory, in particular, for the measurement of electric dipole moments of charged particles in a storage ring.
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Base de dados: MEDLINE Idioma: En Ano de publicação: 2015 Tipo de documento: Article
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Base de dados: MEDLINE Idioma: En Ano de publicação: 2015 Tipo de documento: Article