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NuFact'11 XIIIth Workshop on Neutrino Factories, Superbeams and Beta-beams

1โ€“6 Aug 2011
Europe/Zurich timezone

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Session

WG3 Accelerator Physics

1 Aug 2011, 14:00

Conveners

WG3 Accelerator Physics

  • Alex Bogacz (Jefferson Lab)
  • Makoto YOSHIDA (Osaka University)
  • Elena Wildner (CERN)

WG3 Accelerator Physics

  • Makoto YOSHIDA (Osaka University)
  • Alex Bogacz (Jefferson Lab)
  • elena wildner (CERN)

WG3 Accelerator Physics

  • Makoto YOSHIDA (Osaka University)
  • Alex Bogacz (Jefferson Lab)
  • elena wildner (CERN)

WG3 Accelerator Physics

  • Alex Bogacz (Jefferson Lab)
  • elena wildner (CERN)
  • Makoto YOSHIDA (Osaka University)

WG3 Accelerator Physics

  • Alex Bogacz (Jefferson Lab)
  • Makoto YOSHIDA (Osaka University)
  • elena wildner (CERN)

WG3 Accelerator Physics

  • elena wildner (CERN)
  • Makoto YOSHIDA (Osaka University)
  • Alex Bogacz (Jefferson Lab)

WG3 Accelerator Physics

  • Makoto YOSHIDA (Osaka University)
  • Alex Bogacz (Jefferson Lab)
  • elena wildner (CERN)

Presentation materials

There are no materials yet.

  1. 161. Accelerators for the PS neutrino beam
    Rende Steerenberg (CERN)
    01/08/2011, 14:00
  2. 162. Beta Beams in the CERN complex: PS studies
    Elena Benedetto (CERN)
    01/08/2011, 14:15
  3. 163. 60 GHz ECR source status
    Thierry Lamy (LPSC CNRS)
    01/08/2011, 14:30
  4. 164. Collection of 8B and 8Li
    Semen Mitrofanov (UCL)
    01/08/2011, 14:45
  5. 205. Placeholder
    01/08/2011, 15:00
  6. 166. Beamline status and plans of NOvA
    Philip Adamson (Fermilab)
    02/08/2011, 13:30
  7. 167. Status of the LBNE Neutrino Beamline
    Vaia Papadimitriou
    02/08/2011, 13:50
  8. 168. The CNGS Operation and perspectives
    Edda Gschwendtner (CERN)
    02/08/2011, 14:10
  9. 169. A new design for the CERN to Frรฉjus neutrino beam
    Marco Zito
    02/08/2011, 14:30
  10. 9. WG3 neutrino flux monitoring in the neutrino factory
    Alain Blondel (DPNC)
    02/08/2011, 14:55
    The presentation will summarize the beam controls necessary to efine the flux in the neturino factory with a precision of 10-3. A polarimeter, a beam divergence measurement and a beam current measurement will do the job
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  11. 206. Placeholder
    02/08/2011, 15:10
  12. 172. Target and magnetic horn for CERN -Frรฉjus superbeam
    Nikolaos Vassilopoulos (IPHC/CNRS)
    03/08/2011, 11:00
  13. 173. Liquid targets for isotope production
    Jerry Nolen
    03/08/2011, 11:24
  14. 174. Target options for NF
    Chris Densham (Particle Physics-Rutherford Appleton Laboratory-STFC - Science)
    03/08/2011, 11:48
  15. 199. Simulation of Dynamic Interaction of the Neutrino Factory Mercury Jet with the Mercury Collection Pool/Beam Dump
    Kirk McDonald (Princeton University)
    03/08/2011, 12:12
  16. 175. Commissioning and status of the muon test area at FNL
    Katsuya Yonehara
    03/08/2011, 14:00
  17. 176. MICE step I: first meas. of emittance with part. Phys. det
    David Adey
    03/08/2011, 14:20
  18. 177. Progress in the construction of the MICE cooling channel
    Gail Hanson
    03/08/2011, 14:35
  19. 178. RF Cavity processing and testing plan
    Michael Zisman (Lawrence Berkeley National Laboratory)
    03/08/2011, 14:50
  20. 84. WG3 Performance Comparison Between FSIIA and Bucked Coils for the Neutrino Factory Cooling Lattice
    Ms Androula Alekou (Imperial College London)
    03/08/2011, 15:05
    The transverse emittance of the muon beam produced at the Neutrino Factory front-end needs to be decreased using ionisation cooling. The current baseline cooling lattice for the Neutrino Factory, FSIIA, achieves acceptable muon transmission and transverse emittance reduction. However, recent studies indicate that high magnetic field at the position of the RF cavities may limit their maximum...
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  21. 198. Opportunities for neutrino experiments at ISOLDE
    Tania Manuela De Melo Mendonca (FCUP Faculdade de Ciencias (FCUP)-Universidade do Porto)
    03/08/2011, 15:20
  22. 207. Placeholder
    03/08/2011, 15:35
  23. 59. Neutrino Factory Front End and Extensions
    David Neuffer (Fermilab)
    04/08/2011, 14:00
    The (International Design Report) IDR neutrino factory scenario for capture, bunching, phase-energy rotation and initial cooling of muโ€™s produced from a proton source target is presented. It requires a drift section from the target, a bunching section and a phase-energy rotation section leading into the cooling channel. The rf frequency changes along the bunching and rotation transport in...
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  24. 180. Linac & RLA design status and simulations
    Kevin Beard (Muons,Inc.)
    04/08/2011, 14:15
  25. 73. A new lattice for the beta-beam decay ring to enlarge the stability limit
    Dr Jacques Payet (CEA, IRFU, SACM)
    04/08/2011, 14:30
    The beta-beam concept relies on the production, by beta decay of radioactive ions of a very high flux, of an electron neutrino and anti-neutrino beam towards a distant detector. After production and acceleration in an accelerator complex consisting of a rapid cycling synchrotron, the CERN PS and the CERN SPS, the radioactive isotopes are injected into a long racetrack-shaped ring, called the...
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  26. 87. Recent developments on the muon Non-Scaling FFAG for the Neutrino Factory and its subsystems
    Dr Jaroslaw Pasternak (Imperial College, London)
    04/08/2011, 14:45
    The current status and new developments on the muon Non Scaling FFAG for the Neutrino Factory studied in the framework of the EUROnu/IDS-NF projects are presented. The beam dynamics in the presence of magnet errors, misalignments including the process of acceleration is discussed. The conclusions on the magnet and alignment tolerances are drawn. The progress on the machine subsystems like main...
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  27. 181. Scaling FFAG straight line
    JB Lagrange
    04/08/2011, 15:00
  28. 182. High Tc superconductor magnet technology for FFAG accelerators
    Naoyuki Amemiya (Kyoto Univ.)
    04/08/2011, 15:15
    Recent developments of high Tc coated superconductor ((RE)BCO coated conductor) lead to the possibilities of very high field magnets operated at low temperature (~4.2 K) and efficient magnets operated at high temperature (several tens of Kelvin). For accelerator applications, however, the use coated conductors has been considered difficult due to their tape shape. A project funded by Japan...
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  29. 209. Placeholder
    04/08/2011, 15:35
  30. 200. Preparation for WG summary (I)
    05/08/2011, 13:40
  31. 201. Preparation for WG summary (II)
    05/08/2011, 16:00
  32. 214. Placeholder
    06/08/2011, 09:00
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