Keyword: injection
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MOBO02 Possible Optimizations of Existing Magnet Structures for the Next Generation of ECRIS ion, ECR, sextupole, ECRIS 5
 
  • D. Xie, G.L. Sabbi, D.S. Todd
    LBNL, Berkeley, California, USA
  • W. Lu
    IMP/CAS, Lanzhou, People's Republic of China
 
  Constructing a minimum-B structure with higher magnetic fields is the prerequisite for the next generation of Electron Cyclotron Resonance Ion Sources (ECRIS): ion sources that will operate at substantially higher heating frequencies than those currently in use. There are three leading candidates of Nb3Sn coil structures for use in future ECRISs: a Mixed Axial and Radial field System (MARS) that merges the sextupole racetrack coils and partial end-solenoids into an exotic closed-loop-coil; a classical Sextupole-In-Solenoids design; and a Solenoids-In-Sextupole configuration. Focusing on efficient magnetic field generation, this article briefly reviews the advantages and disadvantages of each of these magnet structures. Though Sextupole-In-Solenoids and Solenoids-In-Sextupole magnetic structures using NbTi conductor have been validated by current ECRISs, improvements of these magnet structures remain possible. Possible optimizations to the two existing magnet structures, such as using a non-conventional sextupole magnet consisting of either V-bend or skew racetrack coils, are discussed. The development status of a MARS NbTi magnet at LBNL for a new ECRIS will be also presented.  
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DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-MOBO02  
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MOFO01 SPIRAL1 Charge Breeder: Performances and Status ion, experiment, operation, plasma 35
 
  • L. Maunoury, O. Bajeat, C. Barthe-Dejean, P. Delahaye, M. Dubois, R. Frigot, P. Jardin, A. Jeanne, O. Kamalou, P. Lecomte, O. Osmond, G. Peschard, A. Savalle
    GANIL, Caen, France
  • J. Angot, T. Lamy, P. Sole
    LPSC, Grenoble Cedex, France
 
  In the framework of the SPIRAL1 upgrade under progress at the GANIL lab, the charge breeder based on a LPSC Phoenix ECRIS, first tested at ISOLDE* has been modified as to benefit of the last enhancements of this device from the 1+ / n+ community**. Prior to its installation in the middle of the low energy beam line of the SPIRAL1 facility, it has been tested at the 1+/n+ LPSC test bench to validate its operation performances. Charge breeding efficiencies as well as charge breeding times have been measured for noble gases and alkali elements. The experimental results demonstrated that the modifications done were on the right track leading the SPIRAL1 charge breeder to the top worldwide in terms of performances. The experimental outcomes have proved the strong interrelationship between the charge breeding efficiency and the charge breeding times which are still under active discussion.
* P. Delahaye et al, Review of Scientific Instruments. 77, 03B105 (2006)
** R. Vondrasek et al, Review of Scientific Instruments 83 113303 (2012)
 
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DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-MOFO01  
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TUAO01 The Proton Source for the European Spallation Source (PS-ESS): Installation and Commissioning at INFN-LNS ion, plasma, proton, MMI 39
 
  • L. Celona, L. Allegra, A. Amato, G. Calabrese, A.C. Caruso, G. Castro, F. Chines, G. Gallo, S. Gammino, O. Leonardi, A. Longhitano, G. Manno, S. Marletta, D. Mascali, A. Massara, A. Maugeri, M. Mazzaglia, L. Neri, S. Passarello, G. Pastore, A. Seminara, A. Spartà, G. Torrisi, S. Vinciguerra
    INFN/LNS, Catania, Italy
  • S. Di Martino, P. Nicotra
    Si.A.Tel SRL, Catania, Italy
 
  A 2.45 GHz ' 0.1 T microwave discharge Proton Source has been designed and assembled at INFN-LNS for the European Spallation Source (PS-ESS) in order to produce pulsed beams of protons up to 74 mA nominal current, at 75 keV of energy, with a transverse emittance containing 99 % of the nominal proton current below 2.25 π mm mrad and a beam stability of ± 2 %. The challenging performances of the machine have triggered specific studies on the maximization of the proton fraction inside the plasma and of the overall plasma density, including dedicated modelling of the wave-to-plasma interaction and ionization processes. The plasma conditioning phase started in July and excellent RF to plasma coupling, more than 99.5% is evident since the beginning. Reflected power fluctuation less than 0.05 % was measured providing a great starting point to reach the beam stability requested by the ESS accelerator.  
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DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-TUAO01  
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TUAO05 First Plasma of the PHOENIX V3 ECR Ion Source ion, plasma, MMI, ECR 48
 
  • T. Thuillier, J. Angot, L. Bonny, J. Jacob, T. Lamy, P. Sole
    LPSC, Grenoble Cedex, France
  • J.L. Flambard, L. Maunoury
    GANIL, Caen, France
  • T. Kalvas
    JYFL, Jyväskylä, Finland
  • C. Peaucelle
    IN2P3 IPNL, Villeurbanne, France
 
  Funding: This project was partially funded by the EU Grant Agreement 283745.
PHOENIX V3 is an upgrade of the PHOENIX V2 ECR ion source granted by the European CRISP project. This new ECRIS features a larger plasma chamber and a re-duced vacuum pressure under operation. The V3 source will replace the V2 one on the SPIRAL2 accelerator in 2018. The first plasma of PHOENIX V3 was achieved on May 9th 2016. The early commissioning of the V3 source at low 18 GHz power demonstrates as expected an en-hancement of the high charge state production and Ar14+ intensity already exceeds the V2 one. Further enhance-ments are expected the outgassing will be achieved and the full RF power will be injected in the source.
 
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DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-TUAO05  
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WEPP15 Design, Construction and Commissioning of the New Superconducting Ion Source AISHa ion, plasma, ECR, MMI 109
 
  • L. Celona, G. Castro, F. Chines, G. Ciavola, G. Costa, S. Gammino, O. Leonardi, S. Marletta, D. Mascali, F. Noto, G. Pastore, G. Torrisi, S. Vinciguerra
    INFN/LNS, Catania, Italy
 
  At INFN-LNS a new superconducting ECRIS named AISHa has been designed with the aim to provide highly charged ion beams with low ripple, high stability and high reproducibility, also fulfilling the needs of hospital installations (e.g. L-He free, easy to use, etc.). It is a hybrid ion source based on a permanent magnet hexapole providing 1.3 T on plasma chamber walls, and four superconducting coils for the axial trapping. The axial magnetic system is very flexible in order to minimize the hot electron component and to optimize the ECR heating by controlling the field gradients and the resonance length. The design of the hexapole aimed to minimize the demagnetization due to SC coils. The magnetic system measurement confirmed the effectiveness of the adopted solutions. Innovative solutions have been also implemented as it concerns the RF system design. It will permit to operate in single/double frequency mode, supported by variable frequency high power klystron generators, thus exploiting at the same time the FTE Frequency Tuning Effect and the Two Frequency Heating. The source has been assembled at the INFN-LNS site and the commissioning phase already started.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-WEPP15  
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WEPP35 Four-Dimension Transverse Phase-Space Distribution Measured by a Pepper-Pot Emittance Meter ion, emittance, ECR, plasma 125
 
  • T. Nagatomo, O. Kamigaito, M. Kase, T. Nakagawa
    RIKEN Nishina Center, Wako, Japan
  • J.W. Stetson
    NSCL, East Lansing, Michigan, USA
  • V. Tzoganis
    Cockcroft Institute, Warrington, Cheshire, United Kingdom
 
  Four-dimensional (4-D) transverse emittance of the highly charged heavy ion beam extracted from ECR ion source is invariant under linear 4-D symplectic operation. Thus, it is essential quantity to improve the beam quality. Measurement of the 4-D phase-space distribution provides quantitative and essential information to improve the efficiency of beam transport. We have developed an on-line pepper-pot-type emittance meter, which is a suitable device to obtain the 4-D phase-space distribution from an image of beamlets passing through the well-aligned pinholes. The emittance meter consists of a thin metal plate with a pinhole array, which is translated along the beam axis, and an imaging screen (P46) with a MCP. We optimized the analysis procedure to obtain the distribution so that the elapsed time of the process was shortened as less than 1 second, and which was enough short for on-line measurements. We will discuss the quality of the obtained 4-D distribution by comparing it with the one obtained from a simulation. Further, we will also discuss how the gas pressure of LEBT affects the 4-D distribution to establish to improve the beam brightness.  
poster icon Poster WEPP35 [2.753 MB]  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-WEPP35  
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WEPP40 Fast Sputtering Measurement Studies using Uranium with the NSCL ECR Ion Sources ion, plasma, ECR, high-voltage 129
 
  • D.E. Neben, J. Fogleman, A.N. Pham, S. Renteria, L. Tobos
    NSCL, East Lansing, Michigan, USA
  • D. Leitner
    LBNL, Berkeley, California, USA
  • G. Machicoane
    FRIB, East Lansing, Michigan, USA
  • G. Parsey
    MSU, East Lansing, Michigan, USA
  • J.P. Verboncoeur
    Michigan State University, East Lansing, Michigan, USA
 
  Funding: Michigan State University and the National Science Foundation: NSF Award Number PHY-1415462
Existing heavy ion facilities such as the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University rely on Electron Cyclotron Resonance (ECR) ion sources as injectors of highly charged ion beams. Long ion confinement times are necessary to produce dense populations of highly charged ions because of steadily decreasing ionization cross sections with increasing charge state. To further understand ion extraction and confinement we are using a fast sputtering technique first developed at Argonne National Laboratory [1] to introduce a small amount of uranium metal into the plasma at a well-defined time. In addition we utilize an axial x-ray apparatus [2] to characterize the hot electron plasma population via its bremsstrahlung emission.
*R. Vondrasek, et. Al., Rev. Sci. Instrum. 73, 548 (2002)
**T. Ropponen, et. Al., Proceedings of ECRIS2010, Grenoble France (2010)
 
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-ECRIS2016-WEPP40  
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