Keyword: solenoid
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WECO03 Transverse Coupling of Ion Beams From an RCR Ion Source ion, emittance, extraction, coupling 76
 
  • Y. Yang, Y. Liu, L.T. Sun, Y.J. Yuan, H.W. Zhao
    IMP/CAS, Lanzhou, People's Republic of China
 
  ECR ion source beam quality will deteriorate under the influence of beam transverse coupling and high-order magnetic field aberration. Ion beams from an ECR ion source will experience a descending axial magnetic field at the extraction region, leading to a strong transverse coupling to the extracted beam, with projection emittance growth both in horizontal and vertical and two eigen emittances separation. On the other hand, sextupole field in the ECR and the sextupole component in the analyzing dipole can also degrade the beam quality by resulting in beam distortion. Proper adjusting of the extraction field strength of the ion source and the pre-focusing solenoid field can help to weaken the correlation in the inter-plane phase spaces and reduce the projection emittances. Another approach to improve the beam quality is to compensate for the high-order magnetic fields. This paper presents the property of beam coupling in the transverse phase space by analytical theory and simulations. Some experimental results are also presented and discussed. In addition, a high-order compensation scheme is displayed, whose feasibility has been verified by preliminary tests with SECRAL at IMP.  
slides icon Slides WECO03 [5.500 MB]  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-WECO03  
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WEPP01 High Intensity Beam Production at CEA/Saclay For The IPHI Project ion, rfq, proton, diagnostics 83
 
  • R. Gobin, D. Bogard, O. Delferrière, M. Desmons, Y. Gauthier, F. Harrault, F. Peauger, G. Perreu, B. Pottin, Y. Sauce, J. Schwindling, F. Senée, O. Tuske, D. Uriot, T.V. Vacher
    CEA/DRF/IRFU, Gif-sur-Yvette, France
 
  CEA/Saclay is involved in high power proton accelerators for long years. This activity started in the 90's, with the development of the SILHI source which routinely produces tens mA of proton beam. Several industrial difficulties led to a very long IPHI RFQ construction process. The 352 MHz RFQ conditioning is presently in progress. Before the completion of the conditioning in CW mode, tests with pulsed proton beam have been decided. As a consequence, the SILHI source recently produced very short H+ beam pulses in order to allow the first IPHI beam acceleration. Such very short pulses, in the range of few hundred microseconds, allowed analyzing the beam loading of the RFQ cavity as well as conditioning the middle energy diagnostic. This article will focus on the source parameters and beam characteristics in the low energy beam line leading to the best RFQ transmission.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-WEPP01  
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WEPP02 Commissioning of the High Intensity Proton Injector of the Facility for Anti Proton and Ion Research at CEA-Saclay ion, proton, plasma, diagnostics 86
 
  • O. Tuske, N. Chauvin, O. Delferrière, Y. Gauthier, P. Girardot, N. Misiara, Y. Sauce, F. Senée, C. Simon
    CEA/IRFU, Gif-sur-Yvette, France
  • F. Ameil, R. Berezov, J. Fils, R. Hollinger
    GSI, Darmstadt, Germany
  • T.V. Vacher
    CEA/DSM/IRFU, France
 
  The Facility for Antiproton and Ion Research (FAIR) located at GSI (Darmstadt) in Germany addresses several fields of physics research within a single installation. One of the contribution of Irfu/SACM at CEA-Saclay to the FAIR linear proton accelerator concerns the development and construction of the ion source and the low energy line. The 2.45 GHz microwave ion source will deliver a 100 mA H+ beam pulsed at 4 Hz with an energy of 95 keV. A low energy beam transport (LEBT) line based on a dual solenoids focusing scheme allows the injection of the proton beam into the radio frequency quadrupole (RFQ) within an acceptance of 0.3π mm.mrad (norm., rms). An electrostatic chopper system located between the second solenoid and the RFQ is used to cut the beam macro pulse from the source to inject 36 μs long beam pulses into the RFQ. This article reports the finalization of the installation of the injector with the detail of dedicated diagnostics, the first beam measurements and gives a planning of the different commissioning phases  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-WEPP02  
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