Keyword: rfq
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MOI1B03 Technical Challenges in Multi-MW Proton Linacs linac, cryomodule, proton, acceleration 20
 
  • V.A. Lebedev
    Fermilab, Batavia, USA
 
  The intensity frontier research is an important part of modern elementary particle physics. It uses proton beams to create secondary beams consisting of, but not necessary limited to, neutrinos, muons, kaons and neutrons. Deferent experiments require different time structure of proton beams but all of them require the beam power of about or exceeding 1 MW. In addition, powerful proton linacs can find an application in accelerator driven nuclear reactors and transmutation of radioactive waste. Recent advances in the superconducting RF technology make a multi-MW power level economically acceptable. This paper discusses main physics and technical limitations determining ultimate parameters of such accelerators, their structure and performance.  
slides icon Slides MOI1B03 [2.863 MB]  
 
MOP229 Design of the MEBT1 for C-ADS Injector II quadrupole, emittance, DTL, simulation 115
 
  • H. Jia, Y. He, S.C. Huang, C.L. Luo, M.T. Song, Y.J. Yuan, X. Zhang
    IMP, Lanzhou, People's Republic of China
 
  The MEBT1 of Chinese ADS Injector II is described. It transports a 2.1 MeV, 10 mA CW proton beam through a series of 7 quadruples and two buncher cavities from the RFQ to the superconducting DTL. For emittance preservation, a compact mechanical design is required. Details of the beam dynamics and mechanical design will be given.  
 
MOP235 Medium Energy Beam Transport Design Update for ESS cavity, quadrupole, linac, DTL 128
 
  • I. Bustinduy, F.J. Bermejo, A. Ghiglino, O. González, J.L. Muñoz, I. Rodríguez, A. Zugazaga
    ESS Bilbao, Bilbao, Spain
  • B. Cheymol, M. Eshraqi, R. Miyamoto
    ESS, Lund, Sweden
  • J. Stovall
    CERN, Geneva, Switzerland
 
  The major challenge of this part of the accelerator is to keep a high quality beam, with a pulse well defined in time, a low emittance and a minimized halo, so that the beam losses downstream the linac be limited and the overall ESS reliability be maximized. In order to minimize beam loss at high energy linac, and the consequent activation of components, a fast chopping scheme is presented for the medium energy beam transport section (MEBT). The considered versatile MEBT is being designed to achieve four main goals: First, to contain a fast chopper and its correspondent beam dump, that could serve in the commissioning as well as in the ramp up phases. Second, to serve as a halo scraping section by means of two adjustable blades. Third, to measure the beam phase and profile between the RFQ and the DTL, along with other beam monitors. And finally, to match the RFQ output beam characteristics to the DTL input both transversally and longitudinally. For this purpose a set of ten quadrupoles is used to match the beam characteristics transversally, combined with two 352.2 MHz buncher cavities, which are used to adjust the beam in order to fulfill the required longitudinal parameters.  
 
MOP243 Experimental Results of Beam Halo at IHEP simulation, quadrupole, space-charge, beam-transport 151
 
  • H.F. Ouyang, T. Huang, J. Li, J. Peng, T.G. Xu
    IHEP, Beijing, People's Republic of China
 
  Space-charge forces acting in mismatched beams have been identified as a major cause of beam halo. In this paper, we describe the beam halo experimental results in a FODO beam line at IHEP. With this beam transport line, experiments are firstly carried out to determine the main beam parameters at the exit of a RFQ with intense beams, and then the measured beam profiles at different positions are compared with the multi-particle simulation profiles to study the formation of beam halo. The maximum measured amplitudes of the matched and mismatched beam profiles agreed well with simulations. Details of the experiment will be presented.  
 
TUO1B05 The Design and Commissioning of the Accelerator System of the Rare Isotope Reaccelerator - ReA3 at Michigan State University cryomodule, target, ion, linac 269
 
  • X. Wu, B. Arend, C. Compton, A. Facco, M.J. Johnson, D. Lawton, D. Leitner, F. Montes, S. Nash, J. Ottarson, G. Perdikakis, J. Popielarski, J.A. Rodriguez, M.J. Syphers, W. Wittmer, Q. Zhao
    NSCL, East Lansing, Michigan, USA
 
  Funding: This material is based upon work supported by the U.S. Department of Energy Office of Sciences under Cooperative Agreement DE-SC0000661
The National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University (MSU) is currently constructing its new rare isotope reaccelerator facility: ReA3, which will provide unique low-energy rare isotope beams by stopping fast rare isotopes in gas stopping systems, boosting the charge state in an Electron Beam Ion Trap (EBIT) and reaccelerating them in a superconducting linac. The rare isotope beams will be producted intially by Coupled Cyclotron Facility (CCF) at NSCL and later by Facility for Rare Isotope Beams (FRIB), currently being designed and constructed at MSU. The accelerator system consists of a Low Energy Beam Transport (LEBT), a room temperature RFQ and a linac utilizing superconducting QWRs. An achromatic High Energy Beam Transport (HEBT) will deliver the reaccelerated beams to the mutiple target stations. Beams from ReA3 will range from 3 MeV/u for heavy nuclei such as uranium to about 6 MeV/u for ions with A<50. The commissioning of the EBIT, RFQ and two cryomodules of the linac is currently underway. The ReA3 accelerator system design and status of commissioning will be presented.
 
slides icon Slides TUO1B05 [6.046 MB]  
 
TUO3B01 Beam Dynamics Design of ESS Warm Linac linac, DTL, emittance, proton 274
 
  • M. Comunian, F. Grespan, A. Pisent
    INFN/LNL, Legnaro (PD), Italy
  • I. Bustinduy
    ESS Bilbao, Bilbao, Spain
  • L. Celona, S. Gammino, L. Neri
    INFN/LNS, Catania, Italy
  • R. De Prisco
    Lund University, Lund, Sweden
  • M. Eshraqi, R. Miyamoto, A. Ponton
    ESS, Lund, Sweden
 
  In the present design of the European Spallation Source (ESS) accelerator, the Warm Linac will accelerate a pulsed proton beam of 50 mA peak current from source at 0.075 MeV up to 80 MeV. Such Linac is designed to operate at 352.2 MHz, with a duty cycle of 4% (3 ms pulse length, 14 Hz repetition period).In this paper the main design choices and the beam dynamics studies for the source up to the end of DTL are shown.  
slides icon Slides TUO3B01 [17.664 MB]  
 
TUO3B04 End to End Beam Dynamics and Design Optimization for CSNS Linac DTL, lattice, linac, quadrupole 286
 
  • J. Peng, S. Fu, H.C. Liu, H.F. Ouyang, X. Yin
    IHEP, Beijing, People's Republic of China
 
  The China Spallation Neutron Source (CSNS) will use a linear accelerator delivering a 15mA beam up to 80MeV for injection into a rapid cycling synchrotron (RCS). Since each section of the linac was determined individually, a global optimization based on end-to-end simulation results has refined some design choices, including the drift-tube linac (DTL) and the medium energy beam transport (MEBT). The simulation results and reasons for adjustments are presented in this paper.  
slides icon Slides TUO3B04 [1.131 MB]  
 
TUO3B05 Beam Dynamics of the 13 MeV/50 mA Proton Linac for the Compact Pulsed Hadron Source at Tsinghua University proton, DTL, simulation, target 289
 
  • Q.Z. Xing, X. Guan, C. Jiang, C.-X. Tang, X.W. Wang, H.Y. Zhang, S.X. Zheng
    TUB, Beijing, People's Republic of China
  • J.H. Billen, J. Stovall, L.M. Young
    TechSource, Santa Fe, New Mexico, USA
  • G.H. Li
    NUCTECH, Beijing, People's Republic of China
 
  Funding: Work supported by the Major Research plan of the National Natural Science Foundation of China (Grant No. 91126003)
We present the start-to-end simulation result on the high-current proton linac for the Compact Pulsed Hadron Source (CPHS) at Tsinghua University. The CPHS project is a university-based proton accelerator platform (13 MeV, 16 kW, peak current 50 mA, 0.5 ms pulse width at 50 Hz) for multidisciplinary neutron and proton applications. The 13 MeV proton linac contains the ECR ion source, LEBT, RFQ, DTL and HEBT. The function of the whole accelerator system is to produce the proton beam, accelerate it to 13 MeV, and deliver it to the target where one uniform round beam spot is obtained with the diameter of 5 cm.
 
slides icon Slides TUO3B05 [7.715 MB]  
 
TUO1C06 Instrumentation Developments and Beam Studies for the Fermilab Proton Improvement Plan Linac Upgrade and New RFQ Front-End linac, proton, ion-source, instrumentation 315
 
  • V.E. Scarpine, D.S. Bollinger, K.L. Duel, N. Eddy, P.R. Karns, N. Liu, W. Pellico, A. Semenov, C.-Y. Tan, R.E. Tomlin
    Fermilab, Batavia, USA
 
  Funding: This work was supported by the U.S. Department of Energy under contract No. DE-AC02-07CH11359.
Fermilab is developing a Proton Improvement Plan (PIP) to increase throughput of it's the proton source. The plan addresses hardware modifications to increase repetition rate and improve beam loss while ensuring viable operation of the proton source through 2025. The first phase of the PIP will enable the Fermilab proton source to deliver 1.8·1017 protons per hour by mid-2013. As part of this initial upgrade, Fermilab plans to install a new front-end consisting of dual H ion sources and a 201 MHz pulsed RFQ. This talk will present beam studies measurements of this new front-end as well as present new beam instrumentation upgrades for the Fermilab linac.
 
slides icon Slides TUO1C06 [2.546 MB]  
 
WEO3B01 FRIB Accelerator Beam Dynamics Design and Challenges ion, linac, target, solenoid 404
 
  • Q. Zhao, A. Facco, F. Marti, E. Pozdeyev, M.J. Syphers, J. Wei, X. Wu, Y. Yamazaki, Y. Zhang
    FRIB, East Lansing, Michigan, USA
 
  Funding: This material is based upon work supported by the U.S. Department of Energy Office of Science under Cooperative Agreement DE-SC0000661.
The Facility for Rare Isotope Beams (FRIB) will be a new national user facility for nuclear science. This cw, high power, superconducting (SC), heavy ion driver linac consists of a frontend to provide various highly charged ions at 0.5 MeV/u, three SC acceleration segments connected by two 180° bending systems to achieve an output beam energy of ≥200 MeV/u for all varieties of stable ions, and a beam delivery system to transport multi-charge-state beams to a fragmentation target at beam power of up to 400 kW. The linac utilizes four types of low-beta resonators with one frequency transition from 80.5 to 322 MHz after Segment 1, where ion charge state(s) is boosted through a stripper at ≤20 MeV/u. The beam dynamics design challenges include simultaneous acceleration of multi-charge-state beams to meet beam-on-target requirements, efficient acceleration of high intensity, low energy heavy ion beams, limitation of uncontrolled beam loss to <1 W/m, accommodation of multiple charge stripping scenarios, etc. We present the recent optimizations on linac lattice, the results of end-to-end beam simulations with machine errors, and the simulation of beam tuning and fault conditions.
 
slides icon Slides WEO3B01 [7.899 MB]  
 
WEO3B02 Acceleration and Transportation of Multiple Ion Species at Ebis-based Preinjector ion, linac, booster, emittance 409
 
  • D. Raparia
    BNL, Upton, Long Island, New York, USA
 
  A new heavy ion pre-injector at Brookhaven National Laboratory consist of an electron Beam Ion Source (EBIS), RFQ and IH Linac and a short transport line. This pre-injector provide any ion Helium to Uranium at energy of 2 MeV/u for Relativistic Heavy Ion Collider (RHIC) and the NASA Space Radiation Laboratory (NSRL). EBIS produces multiple charge states of an ion of interested. These charge states are accelerated through RFQ (300 keV/u) and IH Linac (2 MeV/u) and transported to booster. Charge desecration occurs just before the injection into the booster. This paper discusses implication of acceleration and transports of multiple charge state ions.  
slides icon Slides WEO3B02 [5.825 MB]  
 
WEO3B03 PXIE at FNAL cavity, kicker, diagnostics, ion 414
 
  • N. Solyak, C.M. Baffes, A.Z. Chen, Y.I. Eidelman, B.M. Hanna, S.D. Holmes, V.A. Lebedev, S. Nagaitsev, J.-F. Ostiguy, R.J. Pasquinelli, D.W. Peterson, L.R. Prost, G.W. Saewert, A. Saini, V.E. Scarpine, A.V. Shemyakin, D. Sun, V.P. Yakovlev
    Fermilab, Batavia, USA
 
  PXIE is the integrated systems test for the Project X frontend. It is expected to accelerate 1-2 mA CW beam up to 30 MeV. The major goal of the project is a validation of the Project X concept and elimination of technical risks. It is expected to be constructed in the period of 2012-2016. In presentation the conceptual design of the experimental test facility, lattice and beam dynamics studies will be discussed in details.  
slides icon Slides WEO3B03 [4.561 MB]  
 
WEO3B04 RFQ Beam Dynamics Design for Large Science Facilities and Accelerator-Driven Systems proton, bunching, linac, ion 419
 
  • C. Zhang
    IAP, Frankfurt am Main, Germany
 
  Serving as the front-end of large science facilities and Accelerator-Driven Systems (ADS), the Radio-Frequency Quadrupole (RFQ) accelerator usually needs to reach low beam losses, good beam quality, high reliability, and cost savings such design goals at high beam intensities. To address the challenges for modern RFQs, a special beam dynamics design technique characterized by a reasonable and efficient bunching process with balanced space-charge forces has been developed as an alternative to the classic Four-Section Procedure proposed by Los Alamos National Laboratory (LANL). In this paper, the design studies of some recent RFQ projects will be presented as examples.  
slides icon Slides WEO3B04 [3.698 MB]  
 
THO3A01 High Intensity Aspects of J-PARC Linac Including Re-commissioning after Earthquake linac, simulation, multipactoring, DTL 497
 
  • M. Ikegami, K. Futatsukawa, T. Miyao
    KEK, Ibaraki, Japan
  • Y. Liu
    KEK/JAEA, Ibaraki-Ken, Japan
  • T. Maruta, A. Miura, J. Tamura
    JAEA/J-PARC, Tokai-mura, Japan
 
  We had a massive earthquake in March 2011, which forced us to shutdown J-PARC accelerators for nearly nine months due to its resultant damages. After significant restoration effort, we resumed the beam operation of J-PARC linac in December 2011 and user operation in January 2012. Subsequently, we restored the same beam power as just before the earthquake in March 2012. In the course of the beam commissioning after the earthquake, we have experienced beam losses which were not observed before the earthquake. We discuss the experimentally observed beam losses and its comparison with particle simulations.  
slides icon Slides THO3A01 [5.249 MB]  
 
THO3A02 Beam Dynamics of China ADS Linac linac, cavity, lattice, emittance 502
 
  • Z. Li
    Private Address, Beijing, People's Republic of China
  • P. Cheng, H. Geng, Z. Guo, C. Meng, B. Sun, J.Y. Tang, F. Yan
    IHEP, Beijing, People's Republic of China
 
  Funding: Supported by China ADS Program(XDA03020000), National Natural Science Fundation of China (10875099) and IHEP Special Fundings(Y0515550U1)
An ADS study program is approved by Chinese Academy of Sciences at 2011, which aims to design and built an ADS demonstration facility with the capability of more than 1000 MW thermal power within the following 25 years. The 15 MW driver accelerator will be designed and constructed by the Institute of High Energy Physics (IHEP) and Institute of Modern Physics (IMP) of China Academy of Sciences. This linac is characterized by the 1.5 GeV energy, 10 mA current and CW operation. It is composed by two parallel 10 MeV injectors and a main linac integrated with fault tolerance design. The superconducting acceleration structures are employed except the RFQ. The general considerations and the beam dynamics design of the driver accelerator will be presented.
 
slides icon Slides THO3A02 [5.822 MB]  
 
THO3A03 Simulations and Measurements in High Intensity LEBT with Space Charge Compensation emittance, simulation, injection, space-charge 507
 
  • N. Chauvin
    CEA/IRFU, Gif-sur-Yvette, France
  • O. Delferrière, R. Gobin, P.A.P. Nghiem, D. Uriot
    CEA/DSM/IRFU, France
  • R.D. Duperrier
    ESS, Lund, Sweden
 
  Over the last years, the interest of the international scientific community for high power accelerators in the megawatt range has been increasing. One of the major challenges is to extract and transport the beam while minimizing the emittance growth in the Low Energy Beam Transport line (LEBT). Consequently, it is crucial to perform precise simulations and cautious design of LEBT. In particular, the beam dynamics calculations have to take into account not only the space charge effects but also the space charge compensation of the beam induced by ionization of the residual gas. The code SOLMAXP has been developed in CEA-Saclay to perform self-consistent calculations taking into account space charge compensation. Extensive beam dynamics simulations have been done with this code to design the IFMIF LEBT (Deuteron beam of 125 mA at 100 keV, cw). The commissioning of the IFMIF injector started a few months ago and emmittance measurements of H+ and D+ beams have been done. The first experimental results will be presented and compared to simulation.  
slides icon Slides THO3A03 [3.165 MB]  
 
FRO1A02 WG-B: Beam Dynamics In High Intensity Linacs linac, emittance, DTL, resonance 612
 
  • D. Raparia
    BNL, Upton, Long Island, New York, USA
  • Z. Li
    IHEP, Beijing, People's Republic of China
  • P.A.P. Nghiem
    CEA/DSM/IRFU, France
 
  Emittance coupling, equipartioning and losses were a few topics, which were discussed thoroughly during parallel session for beam dynamics in high intensity linacs (Group B). Linac designs for the future, under construction, upgrade and the existing linacs from around the world were presented in three working sessions. A total of 18 talks were presented. Five presentations are general beam dynamics in nature and twelve talks were project specific. The detail of each contribution can be found in these proceedings. Here we report the summary of the discussions and some concluding remarks of the general interest to all the projects presented in the working group.  
slides icon Slides FRO1A02 [14.464 MB]