Keyword: sextupole
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MOZMH03 Search for the Charged Particle Electric Dipole Moments in Storage Rings lattice, dipole, polarization, storage-ring 6
 
  • V. Senichev
    FZJ, Jülich, Germany
 
  The idea of searching for the electric dipole moment (EDM) of proton and deuteron using polarized beams in a storage ring was originally proposed at Brookhaven National Laboratory (BNL), USA. Currently, the Jülich Electric Dipole moment Investigations (JEDI) collaboration develops the conceptual design of such a ring specifically for the search of the deuteron electrical dipole moment (dEDM). The idea is that the oscillation of the spin due to a possible finite electric dipole moment is separated from the influence of the magnetic dipole moment (MDM), and the spin behavior indicates the existence of dEDM. In connection with this problem, two questions arise: (i) how to create conditions for maximum growth of the total EDM signal of all particles in the beam bunch, and (ii) how to differentiate the EDM signal from the induced MDM signal. For the design of such a ring, we need to address three major challenges: - the ring lattice should meet the conditions of beam stability, and it has to have incorporated straight sections to accommodate the accelerating station, equipment for injection and extraction of the beam, a polarimeter, and sextupoles; - the polarization lifetime of the beam must be around ~1000 seconds; - systematic errors have to be minimized to eliminate the induced fake EDM signal. In my contribution, I will present the current status of the project.  
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WECBMH02 Collector Ring Project at FAIR: Present Status quadrupole, injection, lattice, operation 86
 
  • P.Yu. Shatunov, V.V. Anashin, E.A. Bekhtenev, D.E. Berkaev, M.I. Bryzgunov, D. Gurov, A.S. Kasaev, V.V. Kolmogorov, I. Koop, A.A. Krasnov, O.I. Meshkov, Yu. A. Rogovsky, T.V. Rybitskaya, A.V. Semenov, Y.M. Shatunov, S.V. Shiyankov, D.B. Shwartz, A.A. Starostenko, A.V. Sukhanov, A.S. Tsyganov, A.V. Utkin
    BINP SB RAS, Novosibirsk, Russia
 
  In November 2013, the FAIR management delegated the responsibility for the technical design, construction, installation, and commissioning of the whole CR and its components from GSI to Budker Institute of Nuclear Physics (BINP). Since that time a lot of modifications of the original design were made aiming to improve the beam parameters and the machine performance. This work shows the present status of the development.  
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THCDMH01 Conceptual Design of Superconducting Combined-Function Magnets for the Next Generation of Beam Cancer Therapy Gantry proton, quadrupole, dipole, superconducting-magnet 138
 
  • S.T. Sanfilippo, A. Anghel, C. Calzolaio, A. Gerbershagen, J.M. Schippers
    PSI, Villigen PSI, Switzerland
 
  An increasing number of proton therapy facilities are being planned and built at hospital based centers. Many facilities use rotatable gantry beamlines to direct the proton or ion-beam at the patient from different angles. A key issue is the need to make future gantries lighter and more compact with the use of cryogen-free superconducting magnets, in particular for the final bending section which can be of large aperture. Benefits of using the superconducting technology are: (1) the possibility to have a large momentum acceptance, hence reducing the need to ramp the magnet and enabling new treatment techniques, (2) the size reduction due to a lower bend radius and (3) the weight reduction up to a factor ten. The latter will also significantly reduce the costs of the supporting structure. We present a conceptual design based on Nb3Sn superconducting combined function magnets (dipole, quadrupole, sextupole). The geometry using racetracks, the superconducting strand and cable parameters and the results of the thermal and the mechanical studies are reported. These magnets will work at a temperature of about 4.2 K cooled with cryocoolers.  
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WEPSB017 Chromatic and Nonlinear Dynamics of Antiprotons Injected to Collector Ring at FAIR antiproton, lattice, target, septum 398
 
  • D.B. Shwartz, I. Koop, P.Yu. Shatunov
    BINP SB RAS, Novosibirsk, Russia
  • D.B. Shwartz
    NSU, Novosibirsk, Russia
 
  Collector Ring (CR) is the storage ring for capturing and stochastic cooling of secondary beams of antiprotons or secondary ions. It is a part of a FAIR project being presently at the early start of a construction phase. Due to the proposed large acceptance in both transverse and longitudinal phase spaces, the chromatic aberrations and their correction with sextupoles are very important for capture efficiency. Calculations results for beam transfer from Pbar target to the ring are presented.  
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WEPSB028 Computer Simulation of the Slow Beam Extraction From Nuclotron extraction, dipole, resonance, lattice 422
 
  • A.D. Kovalenko, I.L. Avvakumova
    JINR/VBLHEP, Moscow, Russia
  • A.D. Kovalenko, V.A. Mikhaylov
    JINR, Dubna, Moscow Region, Russia
 
  The results of modelling of ion's motion during beam slow extraction from Nuclotron at the energy 6 GeV/Amu are shown in this work. Influence of sextupole field component of dipole magnets and fringe fields of Lambertson's magnets on the characteristics of extracted beam was analyzed. The calculations have been done via MadX.
* Issinsky I., Mikhaylov V., Shchepunov V. Nuclotron lattice. Proceedings of EPAC 1990, p.458.
** Kovalenko A. Nuclotron: status and future. Proceedings of EPAC 2000, p.554.
*** Agapov N. et al. Slow beam extraction from Nuclotron. Proceedings of the 2001 Particle Accelerator Conference, p.1646.
 
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WEPSB044 Design and Calculation of Cylindrical Electrostatic Deflector for the Transport Channel of the Heavy Ion Beam ion, cyclotron, quadrupole, heavy-ion 461
 
  • N.Yu. Kazarinov, I.V. Kalagin
    JINR, Dubna, Moscow Region, Russia
  • S.G. Zemlyanoy
    JINR/FLNR, Moscow region, Russia
 
  The cylindrical electrostatic deflector is used in the beam transport channel of GALS spectrometer that is created at U400M cyclotron in Flerov Lab of Nuclear Reaction of Joint Institute for Nuclear research. The design and calculation of the deflector are presented in this report. The angular length of the electrodes and gap between potential electrode and screen are found by using of the minimization procedure.  
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