A   B   C   D   E   F   G   H   I   J   K   L   M   N   O   P   Q   R   S   T   U   V   W   X   Y   Z  

Perry, A.

Paper Title Page
TUP091 Energy and Energy Spread Measurements Using the Rutherford Scattering Technique for Tuning the SARAF Superconducting Linac 620
 
  • J. Rodnizki, A. Perry, L. Weissman
    Soreq NRC, Yavne
 
 

The SARAF accelerator is designed to accelerate both deuteron and proton beams up to 40 MeV. Phase I of SARAF consists of a a 4-rod RFQ (1.5 MeV/u) and a superconducting module housing 6 half-wave resonators and 3 superconducting solenoids (4-5 MeV). The ions energy and energy spread were measured using the Rutherford scattering technique . This technique is used to tune the cavities to the desired amplitude and phase. The downstream HWR is used as a buncher and the beam energy spread as function of the bunching RF voltage is applied to estimate the longitudinal emittance. In this work, we present a longitudinal emittance measurement algorithm, which is based on the bunch energy spread as a function of the buncher's amplitude, similar to the standard algorithm that uses the bunches' temporal spread. The tuning and measured longitudinal parameters are in qualitative agreement with the predicted beam dynamics simulation.

 
WE102 The Status of the SARAF Linac Project 679
 
  • L. Weissman, D. Berkovits, I. Eliyahu, I. Gertz, A. Grin, S. Halfon, G. Lempert, I. Mardor, A. Nagler, A. Perry, J. Rodnizki
    Soreq NRC, Yavne
  • A. Bechtold
    NTG Neue Technologien GmbH & Co KG, Gelnhausen
  • K. Dunkel, M. Pekeler, C. Piel
    RI Research Instruments GmbH, Bergisch Gladbach
 
 

Phase I of the Soreq Applied Research Accelerator Facility, SARAF, has been installed and is currently being commissioned at Soreq NRC [1]. According to the Phase I design, SARAF should yield 2 mA proton and deuteron beams at energies up to 4 and 5 MeV, respectively. The status of the main Phase I components is reported. We further present beam commissioning results, which include acceleration of a 1 mA CW proton beam up to 3 MeV. Further improvements in the facility in order to achieve the desired performance are discussed.

 

slides icon

Slides