Keyword: DTL
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TUPRO061 Benchmarking Beam Envelope Models for the European Spallation Source simulation, dipole, linac, space-charge 1174
 
  • I. List
    Cosylab, Ljubljana, Slovenia
  • E. Laface
    ESS, Lund, Sweden
 
  TraceWin is used at the European Spallation Source (ESS) as the design tool, while fast and accurate on-line models will be needed during the operations. Three models are compared: the ESS Linac Simulator (ELS), TraceWin and the OpenXAL. In all of the benchmarked models, dynamics of each beam-line element is, to the first order, represented by a transfer matrix. Differences in the matrices occur, since different reference frames are used and as well different assumptions about the energy of the particles are made. General transformations of the reference frames will be presented. Using those, the comparison of transfer maps among TraceWin and OpenXAL are given. When the differences between TraceWin and OpenXAL were unclear, the benchmark versus other code, like MAD-X and Dynac was done. The best implementations were combined into a new on-line model implementation Java ELS (or JELS) and at last the comparison of the latter with TraceWin is given.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-TUPRO061  
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WEPRO067 Development of NICA Injection Complex ion, rfq, linac, ion-source 2103
 
  • A.V. Butenko, E.E. Donets, A.D. Kovalenko, K.A. Levterov, A.O. Sidorin, G.V. Trubnikov
    JINR/VBLHEP, Moscow, Russia
  • A. Belov
    RAS/INR, Moscow, Russia
  • E.D. Donets, V.V. Fimushkin, A. Govorov, V. Kobets, V. Monchinsky
    JINR, Dubna, Moscow Region, Russia
  • H. Höltermann, H. Podlech, U. Ratzinger, A. Schempp
    BEVATECH, Frankfurt, Germany
  • T. Kulevoy, D.A. Liakin
    ITEP, Moscow, Russia
  • S.M. Polozov
    MEPhI, Moscow, Russia
 
  The new accelerator complex Nuclotron-based Ion Collider fAcility (NICA) is assumed to operate using two linear accelerators: the Alvarez-type linac LU-20 as injector for light ions, polarized protons and deuterons and a new linac HILac for heavy ions. The new Booster and existing Nuclotron superconducting rings are the main parts of the injection complex of the NICA collider. The status of ion sources, both linacs and rings is presented.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-WEPRO067  
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WEPRO075 The Conceptual Design of the China White Neutron Source linac, neutron, rfq, resonance 2127
 
  • J.H. Li, X.C. Ruan, X. Wang
    CIAE, Beijing, People's Republic of China
  • J.H. Billen, K.R. Crandall
    TechSource, Los Alamos, New Mexico, USA
  • J. Stovall
    ESS, Lund, Sweden
  • J.Y. Tang
    IHEP, Beijing, People's Republic of China
  • L.M. Young
    AES, Medford, New York, USA
 
  Funding: Work supported by NSFC of (91126003)
In order to feed the nuclear data needs for design of the Chinese Accelerator Driven sub-critical System (CADS) and new generation nuclear energy systems, we plan to construct the China White Neutron Source (CWNS). The CWNS will be composed of a Proton Linac, an Accumulator Ring, a Target and Experimental Facilities. The linac is designed to deliver a proton beam having an average current of 1 mA at energy up to 300 MeV. The revolution frequency of the accumulator ring will be ~1.4 MHz. Two spallation targets are planned, with one for short pulsed modes and the other for micro-pulsed mode.
 
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-WEPRO075  
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WEPRO086 Experimental Activity in the ENEA-Frascati Irradiation Facility with 3-7 MeV Protons proton, experiment, detector, linac 2156
 
  • M. Vadrucci, A. Ampollini, F. Bonfigli, M.C. Carpanese, F. Marracino, R.M. Montereali, P. Nenzi, L. Picardi, M. Piccinini, C. Ronsivalle, V. Surrenti, M.A. Vincenti
    ENEA C.R. Frascati, Frascati (Roma), Italy
  • F. Ambrosini
    URLS, Rome, Italy
  • M. Balduzzi, C. Marino, C. Snels
    ENEA Casaccia, Roma, Italy
  • M. Balucani, A. Klyshko
    University of Rome "La Sapienza", Rome, Italy
  • C. De Angelis, G. Esposito, M.A. Tabocchini
    ISS, Rome, Italy
 
  A variable energy (3-7 MeV) and pulsed current (0.1 – 100 μA) proton beam has been made available for different applications (radiobiology experiments, detectors development, material studies) in an irradiation facility at ENEA-Frascati based on the 7 MeV injector of the protontherapy linac under realization in the framework of the TOP-IMPLART Project. It is a 425 MHz linear accelerator consisting in a 3 MeV RFQ followed by a DTL up to 7 MeV (PL-7 ACCSYS-HITACHI model) followed by an horizontal and a vertical beam transport line. The latter one is particularly suitable for radiobiology in vitro studies allowing to irradiate besides cell monolayes also cell growing in suspension culture. The paper describes the facility and the recent results of the experimental activity.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-WEPRO086  
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THPME001 Commissioning and Operation of the MedAustron Injector: Results and Future Outlook ion, rfq, ion-source, emittance 3202
 
  • L.C. Penescu, M. Kronberger, T. Kulenkampff, F. Osmić, P. Urschütz
    EBG MedAustron, Wr. Neustadt, Austria
  • W. Pirkl
    CERN, Geneva, Switzerland
 
  The MedAustron facility is a synchrotron-driven hadron therapy and research center presently under construction in Wiener Neustadt, Austria. In its final outline, the facility will provide H+ beams with kinetic energies ≤250MeV and C6+ beams of ≤400MeV/u for clinical applications, and for non-clinical applications H+ of up to 800MeV. First patient treatment is foreseen for the end of 2015. The (H3)+ and C4+ beams are generated at 8keV/u in continuous mode by three ECR ion sources and transported to the RFQ for acceleration to 400keV/u. An inter-tank section matches the beam to the entrance of an IH-mode DTL that accelerates the particles to 7MeV/u before they are stripped to, respectively, H+ and C6+, debunched and transported to the injection plane of the synchrotron. At a later stage of the project, beams of other species can be generated with similar optics. This contribution presents the results of the injector commissioning and operation. A comparison with the baseline optics and with the design error studies is given. In addition, an overview on the operational experience is given, with emphasis on the system reliability, stability and reproducibility.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME001  
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THPME010 A 325 MHz High Gradient CH – Test Cavity for β=0.16 cavity, linac, operation, focusing 3229
 
  • A. Almomani, U. Ratzinger
    IAP, Frankfurt am Main, Germany
 
  Funding: BMBF, contract no. 05P12RFRB9
This pulsed linac activity aims on compact designs, which means a considerable increase in voltage gain per meter. At IAP – Frankfurt, a CH – cavity was developed for these studies, where mean effective accelerating fields well above 10 MV/m are expected at 325 MHz, β=0.164. This cavity is developed within a funded project. Currently, the cavity is under construction and expected to be ready for copper plating in autumn 2014. The results might influence the rebuilt of the UNILAC – Alvarez section, which aims on achieving the beam intensities specified for the GSI – FAIR project. The new GSI 3 MW Thales klystron test stand will be very important for these investigations. Detailed investigations for two different types of copper plating can be performed on this cavity. In this work, the status of the cavity fabrication will be presented. Moreover, low temperature operation of copper cavities is discussed for the case of very short RF pulses.
 
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME010  
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THPME016 Experimental Results on SCDTL Structures for Protons proton, beam-transport, coupling, rfq 3247
 
  • L. Picardi, A. Ampollini, G. Bazzano, P. Nenzi, C. Ronsivalle, V. Surrenti, M. Vadrucci
    ENEA C.R. Frascati, Frascati (Roma), Italy
  • F. Ambrosini
    URLS, Rome, Italy
 
  The medium-energy section of the proton linear accelerator for radiotherapy under realization in the framework of the TOP-IMPLART Project consists in a high frequency 7-35 MeV SCDTL (Side Coupled Drift Tube Linac) structure. The structure, made of 4 modules supplied by one klystron, has been completely designed. The first module up to 11.6 MeV has been built and is under commissioning at ENEA-Frascati and the second and third modules are under realization. The paper describes the system and presents the main results of the experimental activity on this part of the accelerator.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME016  
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THPME041 ESS DTL Status: Redesign and Optimizations emittance, linac, quadrupole, focusing 3314
 
  • R. De Prisco, M. Eshraqi
    ESS, Lund, Sweden
  • M. Comunian, F. Grespan, A. Pisent
    INFN/LNL, Legnaro (PD), Italy
  • A.R. Karlsson
    Lund University, Lund, Sweden
 
  The European Spallation Source (ESS) uses a linear accelerator to deliver the high intensity proton beam to the target station. The average beam power is 5 MW with a peak beam power at target of 125 MW. In 2013 the ESS linac was costed and to meet the budget some modifications were introduced: the final energy was decreased from 2.5 GeV to 2.0 GeV and the beam current was increased from 50 mA to 62.5 mA to keep the same beam power. As a consequence the ESS Drift Tube Linac, DTL, has been re-designed to match the new requirements. This paper presents the main Radio Frequency (RF) and beam dynamics choices for the ESS DTL.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME041  
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THPME044 Statistical Error Studies in the ESS Linac rfq, linac, emittance, alignment 3323
 
  • M. Eshraqi, R. De Prisco, R. Miyamoto, E. Sargsyan
    ESS, Lund, Sweden
  • H.D. Thomsen
    ISA, Aarhus, Denmark
 
  Following the completion of the latest layout of the ESS linac statistical error studies have been performed to define the field vector quality and alignment tolerances. Based on these tolerances and error study results a scheme for the correction system is proposed that assures low losses and permits hands-on maintenance. This paper reports on the strategy of simulating and performing the error studies as well as setting the tolerances.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME044  
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THPME045 Beam Physics Design of the ESS Medium Energy Beam Transport linac, rfq, lattice, emittance 3326
 
  • R. Miyamoto, B. Cheymol, M. Eshraqi
    ESS, Lund, Sweden
  • I. Bustinduy
    ESS Bilbao, Bilbao, Spain
 
  A radio frequency quadrupole (RFQ) and drift tube linac (DTL) in the ESS proton linac are connected with a medium energy beam transport (MEBT) to remove low intensity bunches on the head and tail of a macro-pulse with a chopper and house diagnostic devices to characterize and adjust the beam out of the RFQ for the DTL. These must be achieved within a relatively short space and without large degradation of beam quality due to space charge force, imposing a challenge on the lattice design. This paper presents a beam physics design of the MEBT in the ESS proton linac, which satisfies its requirement while preserving a decent beam quality.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME045  
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THPME049 TAC Proton Accelerator Facility: Normal Conducting Part proton, ion-source, ion, linac 3335
 
  • E. Algin
    Eskisehir Osmangazi University, Eskisehir, Turkey
  • B. Akkus, L. Sahin
    Istanbul University, Istanbul, Turkey
  • H. Cetinkaya
    Dumlupinar University, Faculty of Science and Arts, Kutahya, Turkey
 
  The Turkish Accelerator Center Proton Accelerator Facility (TAC PAF) based on a 1 MW, 2 GeV proton linac will include both normal conducting and superconducting accelerator structures. The project is currently in the technical design phase. The normal conducting part of the TAC PAF will consist of an ion source, a low energy beam transport line, a radio frequency quadrupole, a medium energy beam transport line, and two drift tube linac structures in order to accelerate the beam up to 65 MeV. Acceleration from 65 MeV up to 150 MeV and then 2 GeV energy will be provided by a SC-spoke cavity and two SC-elliptical cavities, respectively. In the long term, TAC PAF will be used as a neutron source. The accelerator structures, their design, and possible experimental stations of TAC PAF project will be presented.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME049  
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THPME059 Preparation of the Coupled RFQ-IH-cavity for FRANZ rfq, coupling, cavity, operation 3367
 
  • M. Heilmann, C. Claessens, O. Meusel, D. Mäder, U. Ratzinger, A. Schempp, M. Schwarz
    IAP, Frankfurt am Main, Germany
 
  The Frankfurt neutron source at the Stern-Gerlach-Zentrum (FRANZ) will provide ultra-short neutron pulses at high intensities and repetition rates. The neutrons will be produced using the 7Li(p, n)7Be reaction induced by a proton beam. The 175 MHz IH-type drift tube linac with 8 gaps succeeds a 4-rod-RFQ. Together they form a coupled linac combination with a length of 2.3 m and accelerate the protons from 120 keV to 2.03 MeV. As the RF losses add up to 200 kW, the cooling of both accelerators is a central challenge. The RFQ-IH combination is powered by a radio frequency amplifier, which couples the RF power into the RFQ. The two structures are connected via inductive coupling. The initial beam operation of the accelerators is configured for 50 mA in cw mode. The IH-components were fabricated, RF tuning measurements are underway. The RFQ and the IH-DTL will be conditioned separately and then be connected, aiming for a beam operation at the end of 2014. A main challenge in fabrication was the precise welding required for the water cooled drift tubes and stems.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME059  
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THPME179 Beam Diagnostics Measurements at 3MeV of the LINAC4 H Beam at CERN linac, emittance, electron, quadrupole 3694
 
  • F. Zocca, J.C. Allica Santamaria, M. Duraffourg, G.J. Focker, D. Gerard, B. Kolad, L. Lenardon, M. Ludwig, U. Raich, F. Roncarolo, M. Sordet, J. Tan, J. Tassan-Viol, C. Vuitton
    CERN, Geneva, Switzerland
  • A. Feschenko
    MIPT, Dolgoprudniy, Moscow Region, Russia
  • A. Feschenko
    RAS/INR, Moscow, Russia
 
  As part of the CERN LHC injector chain upgrade, LINAC4 will accelerate H ions to 160 MeV, replacing the old 50 MeV proton linac. The ion source, the Low Energy Beam Transfer (LEBT) line, the 3 MeV Radio Frequency Quadrupole and the Medium Energy Beam Transfer (MEBT) line hosting a chopper, have been first commissioned in a dedicated test stand and are now tested in the LINAC4 tunnel. Diagnostics devices are installed in the LEBT and MEBT line and in a movable diagnostics test bench which is temporarily added to the MEBT exit. The paper gives an overview of all the instruments used, including beam current transformers, beam position monitors, wire scanners and wire grids for transverse profile measurements, a longitudinal bunch shape monitor and a slit-and-grid emittance meter. The movable test bench also includes a spectrometer that allows measuring the beam energy spread in conjunction with a wire grid. The present understanding of the instrumentation performance is discussed and the measurement results that allowed characterizing the 3 MeV beam in the LINAC4 tunnel are summarized.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPME179  
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THPRI056 A New Debunching Cavity for the ISIS H Injector cavity, vacuum, simulation, radio-frequency 3899
 
  • B.S. Drumm, A.P. Letchford, R.E. Williamson
    STFC/RAL/ISIS, Chilton, Didcot, Oxon, United Kingdom
  • M. Keelan
    STFC/RAL, Chilton, Didcot, Oxon, United Kingdom
 
  The energy range of the ISIS 70MeV H injected beam is reduced using an RF debunching cavity. The existing cavity consists of a mild steel vacuum vessel containing a water-cooled copper shell into which RF power is fed. The unit is made up of components designed for the 50 MeV Proton Linear Accelerator (PLA) which used to occupy the Rutherford Appleton Laboratory (RAL) site between 1957 and 1969. The component drawings date back to the late 1960s. Due to its age, complexity and a lack of spares, there is a need for a modern solution. This paper documents the development of a new debunching cavity for the ISIS neutron source.  
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-THPRI056  
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