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ECR

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MOP039 First Beams Produced by the Spiral-2 Injectors ion, emittance, heavy-ion, proton 139
 
  • J.-L. Biarrotte
    IPN, Orsay
  • P. Bertrand
    GANIL, Caen
  • C. Peaucelle
    IN2P3 IPNL, Villeurbanne
  • T. Thuillier
    LPSC, Grenoble
  • O. Tuske, D. Uriot
    CEA, Gif-sur-Yvette
 
 

The SPIRAL-2 superconducting linac driver, which aims at delivering 5 mA, 40 MeV deuterons and up to 1 mA, 14.5 A.MeV q/A=1/3 heavy ions, has now entered its construction phase in GANIL (Caen, France). The linac is composed of two injectors feeding one single RFQ, followed by a superconducting section based on 88 MHz independently-phased quarter-wave cavities with room-temperature focusing elements. The first stages of the injectors have been fully built and are now operational. They have been partly commissioned with beam in Grenoble and Saclay in 2010. This paper describes the results obtained so far in this context.

 
MOP042 UNILAC Upgrades for Coulomb Barrier Energy Experiments ion, ECRIS, rfq, ion-source 148
 
  • L.A. Dahl, W.A. Barth, P. Gerhard, S. Mickat, W. Vinzenz, H. Vormann
    GSI, Darmstadt
  • A. Schempp, M. Vossberg
    IAP, Frankfurt am Main
 
 

The GSI linear accelerator UNILAC provides heavy ion beams at Coulomb barrier energies for search and study of super heavy elements. Typical cross-sections of 55 fb require beam doses of 1.4·1019 according to a beam time of 117 days. Several upgrades will reduce the beam time to only 16 days. A second injection branch with a 28GHz-MS-ECRIS anticipates a factor of 10 in particle intensity. By a new cw rfq-structure all accelerator tanks are suitable for a duty cycle of at least 50% instead of 25% presently. Due to this, thermal power increase of 19 rf-amplifiers eased by higher ion charge states of the ECRIS is necessary. Finally the UNILAC timing system controlling 50Hz pulse-to-pulse operation of up to six beams differing in ion species and energy has to be modified considering beam diagnostics electronics and pulsable magnets. The front end comprising ECRIS, rfq- and IH-structure is cw suitable and will serve as injector for a new future sc-cw-linac.

 
TUP019 Proton Linac for ADS Application in China linac, cavity, rfq, proton 437
 
  • S. Fu, S.X. Fang, J.Q. Wang
    IHEP Beijing, Beijing
  • X. Guan
    CIAE, Beijing
 
 

In the next two decades, China will be in period of fast development of nuclear power to meet the energy demands of the rapid economy growth and to cut down the CO2 release. Accelerator Driven System is recognized as the best option for nuclear radioactive waste transmutation. ADS long-term development roadmap has been proposed. Based on the ADS basic study in the last decade, a samll-scale ADS facility is going to be built to do experimental research on ADS system. In this paper, we will first review the previous R&D activity on ADS linac research in China, and then introduce the design of the linac in the small-scale ADS facility.

 
TUP041 The New GSI HLI-RFQ for CW-Operation rfq, ion, emittance, alignment 494
 
  • M. Vossberg, A. Schempp, C. Zhang
    IAP, Frankfurt am Main
  • W.A. Barth, L.A. Dahl
    GSI, Darmstadt
 
 

A new CW-RFQ has been built for the upgrade of the HLI (High Charge State Injector) of GSI for operating with a 28GHz-ECR-Ion source and simultaneous increase of the beam duty cycle from 25 % now to 100 %. The new HLI 4-rod RFQ will accelerate charged ions from 4 keV/u to 300 keV/u for the injection into the IH-structure. High beam transmission, a small energy spread and small transverse emittance growth and good input matching are design goals. Properties of this CW-RFQ, status of project and first measurements will be presented.

 
TUP086 Emittance Measurements for Stable and Radioactive Ion Beams emittance, ion, ion-source, insertion 608
 
  • S.A. Kondrashev, A. Barcikowski, A. Levand, P.N. Ostroumov, R.C. Pardo, G. Savard, R.H. Scott, T. Sun, R.C. Vondrasek, G.P. Zinkann
    ANL, Argonne
 
 

An emittance meter based on a pepper-pot coupled to a CsI (Tl) scintillator has been developed over the last several years [1] at Argonne National Laboratory. A compact version of such a probe for on-line emittance measurements has been designed, built and installed into the low energy beam transport (LEBT) line of the Argonne Tandem Linac Accelerator System (ATLAS) and also downstream of the gas catcher of the recently commissioned Californium Rare Isotope Breeder Upgrade (CARIBU). The probe has demonstrated the capability to measure emittance of ion beams with a current density as low as 10 nA/cm2. Systematic emittance measurements in the ATLAS LEBT for different ion species have been done and results will be presented. The probe, based on a pepper-pot coupled to an MCP viewing system, has been designed and built to measure the emittance of low intensity (102-106 ions/s) radioactive CARIBU ion beams.


[1] S. Kondrashev et al. Development of a pepper-pot emittance probe and its application for ECR ion beam studies. Nuclear Instruments and Methods in Physics Research A 606, 2009, pp. 296-304.

 
THP117 Study of the Frequency Tuning Effect for the Improvement of Beam Brightness in ECR Ion Sources plasma, electron, ion, resonance 1013
 
  • S. Gammino, L. Celona, G. Ciavola, D. Mascali, R. Miracoli
    INFN/LNS, Catania
  • F. Maimone
    GSI, Darmstadt
 
 

According to the model that has driven the development of ECRIS in the last years, a large variation of the pumping microwave frequency (order of GHz) boosts the extracted current for each charge state because of a larger plasma density. Recent experiments have demonstrated that even slight frequency's changes (of the order of MHz) considerably influence the output current, and also the beam properties after the extraction (beam shape, brightness and emittance). In order to investigate how this fine tuning affects the plasma heating, a set-up for the injection of different microwave frequencies into the ECRIS cavity has been prepared. The microwave power is fed by means of a Travelling Wave Tube amplifier with a broad operating frequency range. The frequency can be systematically changed and the beam output is recorded either in terms of charge state distributions and beam emittance. The detected brehmsstralung X-rays are additionally analysed: they give insights about the electron energy distribution function (EEDF). The results are compared with simulations and data coming from previous preliminary experiments.