Sep 17–22, 2023
Victoria Conference Centre
Canada/Pacific timezone
Fairmont Empress (Conference Hotel): All reservations must be made by phone or email now. https://icis2023.triumf.ca/accommodations.html

Contribution List

176 out of 176 displayed
  1. 2023-09-18, 8:30 a.m.
  2. Mr Olivier Tuske (Université Paris-Saclay, CEA, Département des Accélérateurs, de la Cryogénie et du Magnétisme, 91191, Gif-sur-Yvette, France.)
    2023-09-18, 9:10 a.m.
    Invited Oral

    The production of intense proton beams in CEA Saclay started in the 90’s with the development of the SILHI source to inject the IPHI accelerator. This ECR ion source is still in operation nowadays. ECR plasma is well-known heating process and plasma chamber internal dimensions were investigated in order to reduce size and maintenance time. In 2012 R&D investigations on those simple plasma...

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  3. Kazumasa Takahashi (Nagaoka University of Technology)
    2023-09-18, 9:40 a.m.
    Contribute Oral

    LION is a laser ion source that has been in operation at Brookhaven National Laboratory (BNL). It is the first laser ion source to supply ion beams stably for users at a large accelerator facility in the world. LION is located at the upstream end of the heavy ion accelerator complex at BNL and supplies singly charged ion beams of various ion species. LION has been in operation from 2014 to...

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  4. Mr Sidharth Kumar Dash (1.Institute for Plasma Research, Bhat, Gandhinagar, Gujarat 382428, India 2. Homi Bhabha National Institute, Anushaktinagar, Mumbai, Maharashtra 400094, India.)
    2023-09-18, 10:00 a.m.
    Contribute Oral

    The ion beam divergence & uniformity/homogeneity apart from beam energy are two crucial parameters of a large-size ion source-based NBI (Neutral Beam Injector) for the physical interpretations of beam dynamics & control of its extraction system. Characterization of $H^-$ ion beam in ROBIN (Rf Operated Beam source in India for Negative ion) source using two orthogonally placed cameras installed...

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  5. Huanyu Zhao (Institute of Modern Physics, Chinese Academ of Sciences)
    2023-09-18, 10:50 a.m.
    Invited Oral

    The capability of laser ion sources to produce high intensity short pulse ion beams, especially from solid element, makes them promising pre-injectors for some application facilities, such as cancer therapy facilities and accelerator-based neutron sources. Aiming at these applications, some specific ions, like carbon, lithium ions, have been produced and optimized in terms of the high charge...

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  6. Masahiro Okamura (Brookhaven National Laboratory)
    2023-09-18, 11:20 a.m.
    Invited Oral

    A compact accelerator-driven neutron generator with a lithium beam driver can generate neutrons in a forward direction, even using incident beam energy at a near-threshold energy. Especially for medical and industrial applications, the ability to suppress unwanted radiation to patients is a major advantage. However, it is difficult to supply a high-intensity lithium-ion beam, and its practical...

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  7. Takashi Nagatomo (RIKEN Nishina Center)
    2023-09-18, 11:50 a.m.
    Contribute Oral

    We studied how the transverse phase-space distribution (PSD) of heavy-ion beams extracted from an ECR ion source (ECRIS) changes as a function of the extraction current $I_{\rm ext}$ through the LEBT. Heavy ion beams produced by ECRIS are distributed over a certain range of charge, so that the total current extracted from the ion source $I_{\rm ext}$ is an order of magnitude larger than that...

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  8. Lorenzo Neri (INFN)
    2023-09-18, 1:40 p.m.
    Invited Oral

    The requirements for future accelerator chains need to increase the injected beam brilliance significantly, still keeping high the beam quality in terms of reliability, reproducibility and stability. A roadmap for ion source development may consist of several steps: plasma simulation, multiphysics simulation of each system component, high-level control system, plasma characterisation, beam...

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  9. Dr Dan Faircloth (ISIS-RAL-STFC-UKRI)
    2023-09-18, 2:10 p.m.
    Contribute Oral

    It is a commonly held belief that the beam current extracted from an ion source varies with the applied extraction voltage with a V^(3/2) power law as defined by the space charge limited Child Langmuir equation.
    However, recent experiments and modelling work have shown that the reason for the apparent V^(3/2) relationship is not caused by space charge limited extraction, but instead the...

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  10. Akbar Hossain (University of Jyväskylä)
    2023-09-18, 2:30 p.m.
    Contribute Oral

    The production of negative ions in caesium sputter ion sources occurs on the surface of a cathode, which contains the ionized material and is covered by a thin layer of caesium that enhances the negative ion yield by lowering the work function. We have recently demonstrated that the negative ion beam currents can be enhanced by exposing the ion source cathode to a laser beam [1-3]. In this...

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  11. Bharat Mishra (INFN-LNS and University of Catania)
    2023-09-18, 2:50 p.m.
    Contribute Oral

    Simulations are a powerful method to study the correlation between output beams and internal dynamics of ECR plasmas, which involve a complex interplay between injected power, RF frequency, gas type and pressure. Modelling the microscopic properties of such plasmas is essential not only for fundamental research into the operation of ECR ion sources but also for applications like the PANDORA...

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  12. Dimitar Yordanov (Max Planck Institute for Plasma Physics)
    2023-09-18, 3:10 p.m.
    Contribute Oral

    The ion source for neutral beam injection at ITER has to provide high intensity and low divergence negative hydrogen and deuterium ion beam. Extracting the negative ions from the plasma is inevitably accompanied by co-extraction of electrons, which can limit the source performance, especially in deuterium. Reducing the co-extracted electrons is done by applying a magnetic filter field and a...

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  13. Yoshihide Higurashi (RIKEN)
    2023-09-18, 3:30 p.m.
    Contribute Oral

    Recently, production of highly charged medium mass heavy ion beams, such as Titanium (Ti), Vanadium (V), and Chromium (Cr) ions, are strongly demanded for the synthesis of new elements. At RIKEN, especially, production of intense 51V13+ ion beam for long term was strongly required for synthesis of the new element (Z=119). For this purpose, we constructed new superconducting electron cyclotron...

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  14. 2023-09-19, 8:55 a.m.
  15. Akira Ueno (Japan Atomic Energy Agency (JAEA))
    2023-09-19, 9:00 a.m.
    Invited Oral

    In NIBS2022, the stable 8-hour operation of the J-PARC cesiated RF-driven Hˉ ion source in a test-stand with a 69.9 keV 120 mA beam and a beam duty factor of 4 % (1 ms x 40 Hz) was reported. However, the Cesiation condition was produced after many times and rather large amount of Cesium and H2Os injections. The necessary plasma electrode temperature (TPE) of 254 ${}^\circ$C was also much...

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  16. Jianglong Wei (Institute of Plasma Physics, Chinese Academy of Sciences)
    2023-09-19, 9:30 a.m.
    Contribute Oral

    Burning plasma Experimental Superconducting Tokamak (BEST) will be a new magnetic confinement fusion device (major radius ~3.6 m, minor radius ~1.1 m, plasma current <7 MA, toroidal field <6.1 T) located at Hefei, China. BEST aims to research and develop the physics and technology of the fusion power to generate electricity. Neutral beam injection is one of the auxiliary heating and current...

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  17. Dr Adrian Heiler (Max-Planck-Institut für Plasmaphysik (IPP))
    2023-09-19, 9:50 a.m.
    Contribute Oral

    Negative hydrogen ion sources for neutral beam injection (NBI) systems for nuclear fusion experiments rely on the surface production of negative hydrogen ions on a low work function converter surface. The state-of-the-art technique for the generation of low work function surfaces is steady evaporation of the alkali metal Cs into the ion source. As the Cs layers are affected by residual gases...

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  18. Dr Isabella Mario (Consorzio RFX (CNR, ENEA, INFN, UNIPD, Acciaierie Venete SpA), Corso Stati Uniti 4, 35127 Padova, Italy)
    2023-09-19, 10:10 a.m.
    Contribute Oral

    The experimental fusion reactor ITER will feature two heating neutral beam injectors (NBI) capable of delivering 33(50) MW of power into the plasma. NBI consists of a plasma source for production of negative ions (extracted negative ion current up to $\mathrm{329\,A/m^2}$ in H and $\mathrm{285\,A/m^2}$ in D) then accelerated up to 1 MeV for one hour. The negative ion beam is neutralized, and...

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  19. Emanuele Sartori (Consorzio RFX - Università degli Studi di Padova)
    2023-09-19, 11:00 a.m.
    Invited Oral

    Giant negative ion sources are used for neutral beam injectors in fusion devices. A high density of cold negative hydrogen ions is required over the large extraction area of the caesium-seeded plasma source, to provide the required negative ion current, distributed uniformly over thousands of extraction apertures. In this regard, it is expected that the expansion of plasma and neutrals from...

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  20. Prof. Katsuyoshi Tsumori (National Institute for Fusion Science)
    2023-09-19, 11:30 a.m.
    Invited Oral

    Reduction of beamlet divergence angle is one of the most challenging issues in negative ion sources driven with Radio-Frequency (RF). Minimum divergence of the beamlet accelerated from Filament-Arc (FA) driven source is ~5 mrad, while that from RF driven source is ~12 mrad, which is larger than the beamlet divergences of 7 mrad required for ITER HNB and DNB. The reason why the beamlet...

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  21. Dirk Wünderlich (Max-Planck-Institut für Plasmaphysik)
    2023-09-19, 12:00 p.m.
    Contribute Oral

    Negative hydrogen or deuterium ion sources for neutral beam injection (NBI) systems used at fusion devices are based on the surface production process at a caesiated low work function converter surface. The ITER NBI system will deliver a large beam (≈2 m × 1 m, extraction area ≈0.2 m$^2$) with an accelerated current of 40 A negative deuterium ions (46 A in hydrogen) with a high homogeneity,...

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  22. Christian Wimmer (Max-Planck-Institut f. Plasmaphysik)
    2023-09-19, 1:50 p.m.
    Invited Oral

    Neutral beam injectors (NBI) for fusion facilities have strict requirements on the beam divergence (7 mrad for the ITER NBI at 1 MeV). Measurements of the single beamlet divergence of RF negative ion sources (at lower beam energy < 100 keV) show significantly higher values (12-15 mrad), also larger than filament arc sources at similar beam energies. This opened up questions whether the higher...

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  23. Weidong Chen (Institute of high energy physics, Chinese academy of sciences (CAS))
    2023-09-19, 2:20 p.m.
    Negative Ion Sources and Sources for Fusion Facilities
    Contribute Oral

    The RF-driven ion source has been put into commissioning on China spallation neutron source (CSNS) accelerator since September of 2021. It has a service life time of more than 310 days and availability of almost 100%. To fully meet the requirements of CSNS project phase-II (CSNS-II), the beam intensity should be enhanced and the transverse emittance should be minimized. This report covers...

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  24. Baoxi Han (Oak Ridge National Laboratory)
    2023-09-19, 2:40 p.m.
    Contribute Oral

    The Spallation Neutron Source (SNS) located at the Oak Ridge National Laboratory is an accelerator-based, pulsed neutron scattering facility utilized for a broad range of scientific research applications. For the past decade, the facility has operated at its original design beam power of 1.4 MW, and it is currently undergoing an upgrade to double its power to 2.8 MW within the next several...

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  25. Dr Taneli Kalvas (University of Jyvaskyla, Department of Physics)
    2023-09-20, 9:00 a.m.
    Invited Oral

    The vast majority of the ECRIS are based on magnetic confinement with solenoid and sextupole field components. The development of such structure using present superconducting wire technology is limited to 56 GHz, whereas the minimum-B quadrupole ARC-ECRIS topology has been theoretically shown to enable up to 100 GHz operation. The CUBE-ECRIS is a recently commissioned permanent magnet...

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  26. Laurent Maunoury (Normandy Hadrontherapy)
    2023-09-20, 9:30 a.m.
    Applications of Ion Sources
    Contribute Oral

    Normandy Hadrontherapy (NHa) and Ion Beam Application (IBA) are collaborating to develop a full hadrontherapy treatment solution based on a new multiparticle cyclotron. C6+ and He2+ ions will be accelerated up to 400 MeV/u and (H2)+ up to 260 MeV/u. Three different ion sources will be carried out for each accelerated particle: the mono-charged ion sources (H2)+ and low charged ion source He2+...

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  27. Thomas Thuillier (LPSC)
    2023-09-20, 9:50 a.m.
    Contribute Oral

    A new A/Q=7 injector is under development for the SPIRAL2 accelerator at Caen, France (NEWGAIN project). A new 28 GHz superconducting electron cyclotron resonance ion source (ECRIS) named ASTERICS*, located on a high voltage platform, is under design for this project. The source features a modern cryostat allowing for the saving of helium during a quench and a large plasma chamber (90 mm...

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  28. Yushi Kato (Osaka Univ.)
    2023-09-20, 10:10 a.m.
    Contribute Oral

    For many years, we have been promoting basic and applied research on multiply-charged ion generation in an electron cyclotron resonance (ECR) ion source (ECRIS). Based on these experimental results, we considered the accessibility conditions for wave propagation in the magnetized plasma in ECRIS, and proposed various microwave feeding methods to improve the efficiency of multiply-charged ion...

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  29. Hannu Koivisto (Accelerator Laboratory, Department of Physics, University of Jyväskylä)
    2023-09-20, 11:00 a.m.
    Invited Oral

    The European Electron Cyclotron Resonance (ECR) ion source community has more than 20 years of experience working together in various EU-funded projects. In the recent project, called ERIBS (European Research Infrastructure – Beam Services), we will focus on improving ion beam services for the EURO-LABS (European-Laboratories for Accelerator Based Sciences) research infrastructures. The...

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  30. Liangting Sun (Institute of Modern Physics, CAS)
    2023-09-20, 11:30 a.m.
    Invited Oral

    Aiming to the production of 1 emA U3x+ intense highly charged ion beam, the 4th generation ECR ion source 45 GHz FECR (First 4th generation ECR ion source) is under development at IMP. Fundamental progresses have been made towards this challenging machine. The first superconducting ECR ion source magnet based on Nb3Sn technology is going to be in place to provide sufficient magnetic...

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  31. Oskari Timonen (Accelerator Laboratory, Department of Physics, University of Jyväskylä)
    2023-09-20, 12:00 p.m.
    Contribute Oral

    Optical emission spectroscopy provides a noninvasive method to probe the properties of hot and highly charged magnetically confined plasmas. The optical emission line profiles enable, for example, identifying the different species and characterizing the relative population densities and temperatures of the ions and neutrals forming the plasma. The feasibility of this approach has been...

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  32. 2023-09-20, 12:45 p.m.
  33. Joseph Adegun (TRIUMF)
    2023-09-21, 9:00 a.m.
    Invited Oral

    The RF system of the TRIUMF electron cyclotron resonance ion source charge state booster (CSB) was recently upgraded for the implementation of two-frequency heating using a single waveguide. The injection and extraction optics as well as the injection and extraction systems of the CSB were systematically modelled and optimized. The quadrupole scan technique was developed for beam emittance...

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  34. Eugenia Naselli (Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud (INFN, LNS))
    2023-09-21, 9:30 a.m.
    Contribute Oral

    An innovative ECR ion trap facility, called PANDORA (Plasma for Astrophysics, Nuclear Decay Observation and Radiation for Archaeometry), was designed for fundamental plasma processes and nuclear physics investigations. The overall structure consists of three main pillars: a) a large (70 cm in length, 30 cm in diameter) ECR plasma trap with a fully superconducting B-minimum magnetic system...

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  35. Dr Junwei Guo (Facility for Rare Isotope Beams)
    2023-09-21, 9:50 a.m.
    Contribute Oral

    The Facility for Rare Isotope Beams (FRIB) has become operational as a user facility in April 2022. The primary beam power available on target routinely now reaches 5 kW and preparations for operation at 10 kW are underway with an ultimate design goal to deliver 400 kW within the next 6 years. FRIB front end currently operates two ECR ion sources: a room temperature ECR ion source operating at...

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  36. Sophie Hurier (SCK CEN & KULeuven)
    2023-09-21, 10:10 a.m.
    Contribute Oral

    MYRRHA will be the world’s first large-scale Accelerator Driven System at power levels scalable to industry. In ISOL@MYRRHA, Radioactive Ion Beams (RIBs) will be produced using the Isotope Separation On-Line (ISOL) technique, with increased isotope production through high-intensity primary beam and long irradiation times. High-quality RIBs are to be maintained over that period, up to 4 weeks....

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  37. Mia Au (CERN)
    2023-09-21, 11:00 a.m.
    Invited Oral

    The ISOLDE facility at CERN provides ion beams of nuclides produced in reactions between 1.4-GeV protons and thick targets. Molecules have been studied as a method to deliver beams of release-limited refractory elements by forming volatile molecules [1-5]. Molecular sideband extraction is also used as a technique to improve beam purity. Molecular beams additionally provide opportunities for...

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  38. Sebastian Rothe (CERN)
    2023-09-21, 11:30 a.m.
    Invited Oral

    The ISOLDE radioactive ion beam facility is located at CERN’s Proton Synchrotron Booster, where thick targets are irradiated with 1.4-GeV protons. Over 1000 different radioisotopes with half-lives down to milliseconds can be delivered to low-energy experimental setups at up to 60 keV, or post accelerated using the REX and HIE ISOLDE linear accelerators.
    One important factor for planning...

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  39. Dr Alain Lapierre (FRIB/MSU)
    2023-09-21, 12:00 p.m.
    Contribute Oral

    The Reaccelerator (ReA) of the Facility for Rare-Isotope Beams (FRIB) at Michigan State University (MSU) uses a helium gas-filled Radio-Frequency Quadrupole (RFQ) ion trap and an Electron-Beam Ion Trap (EBIT) as a charge-breeding system. Rare isotopes produced via projectile fragmentation or in-flight fission are selected by the Advanced Rare Isotope Separator of FRIB and stopped in a helium...

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  40. Valentin Fedosseev (CERN)
    2023-09-21, 2:20 p.m.
    Invited Oral
  41. Mariusz Juchno (Lawrence Berkeley National Laboratory)
    2023-09-21, 2:50 p.m.
    Invited Oral

    Future heavy-ion driver accelerators will require high charge state ECR sources operating beyond the currently achievable heating radio frequency of 28 GHz. Lawrence Berkeley National Laboratory is exploring two technological paths that can enable reaching this goal. The first approach is by using Mixed Axial and Radial field System (MARS). This novel coil system allows the use of the Nb-Ti...

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  42. Asar AH Jaradat (CERN)
    2023-09-21, 3:20 p.m.
    Contribute Oral

    Laser resonance ionization spectroscopy is a sensitive tool for investigating nuclear structures [1], but its spectral resolution is limited by Doppler broadening, which becomes significant at ion source temperatures of approximately 2000°C. This can limit resolution to 1-10 GHz, making it difficult to measure nuclear magnetic and quadrupole moments.
    A new laser ion source design has been...

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  43. Hikaru Souda (Yamagata University)
    2023-09-21, 4:10 p.m.
    Invited Oral

    A world smallest carbon ion radiotherapy facility, East Japan Heavy Ion Center, Faculty of Medicine, Yamagata University, started treatment operations in February 2021. The treatment system consists of an ECR ion source, an RFQ and IH-type drift tube linac, a 430 MeV/u synchrotron and a spot-scanning irradiation system. It has two treatment rooms, one is a fixed horizontal beam port and the...

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  44. Mr Arun Tejaswee Annaluru (High Voltage Engineering Europa B.V.)
    2023-09-21, 4:40 p.m.
    Contribute Oral

    Since decades, High Voltage Engineering (HVE) manufactures particle accelerator systems for research and industry. HVE’s product line includes Singletron and Tandetron accelerator systems with terminal voltages of up to 6 MV. They are dedicated to a wide range of applications, including ion implantation and irradiation, Ion Beam Analysis (IBA), Accelerator Mass Spectrometry (AMS), and neutron...

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  45. Tetsuhiko Yorita (RCNP, Osaka Univ.)
    2023-09-21, 5:00 p.m.
    Contribute Oral

    For simple applications, such as the calibration of a charged particle detector, a multi-MeV proton generator may be preferable to cyclotrons or electrostatic accelerators such as Van de Graaff generator. Thus, a compact proton generating system, consisting of 10Ghz ECR ion source NANOGAN and a deuteron target, was developed at the Research Center for Nuclear Physics at Osaka University. A...

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  46. Shixiang Peng (Peking University)
    2023-09-21, 5:20 p.m.
    Contribute Oral

    The first fully domestically boron neutron capture therapy demonstration device located in Yangtze River Delta region based on an accelerator neutron source will be build recently. It is held by "Xi'an Jiaotong University-Huzhou Neutron Science Laboratory" joint lab established by Xi'an Jiaotong University and Huzhou Industrial Group. The BNCT facility requires a proton beam of 30 mA@40 keV at...

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  47. Olli Tarvainen (UK Science and Technology Facilities Council)
    2023-09-22, 9:00 a.m.
    Invited Oral

    There are a huge variety of ion source types employed to produce charged particle beams for discovery physics and accelerator applications such as neutral beam heating of thermonuclear fusion plasmas and spallation neutron sources. In most ion sources the ion beams are extracted directly from a plasma sustained by a DC or RF energy source. What is common to all ion sources is the need for...

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  48. Nicolas Savard (TRIUMF, D-Pace)
    2023-09-22, 9:30 a.m.
    Contribute Oral

    Particle-in-Cell (PIC) codes used to study plasma dynamics within ion sources typically use an explicit scheme. These methods can be slow when simulating regions of high electron density in ion sources, which require resolving the Debye length in space and the plasma frequency in time. Recent developments on fully-implicit PIC models in curvilinear geometries have shown that these spatial/time...

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  49. Anand Mathai George (TRIUMF/D-Pace)
    2023-09-22, 9:50 a.m.
    Contribute Oral

    D-Pace is developing a 13.56 MHz RF ion source capable of producing negative ions (H$^-$, D$^-$). The ion source is a hybrid design between the TRIUMF-licensed filament ion source and the RADIS ion source licensed from the University of Jyväskylä. An Inductively Coupled Plasma (ICP) is generated inside the plasma chamber using a planar spiral external antenna, powered by an RF power supply....

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  50. Roland Friedl (AG Experimentelle Plasmaphysik (EPP), University of Augsburg)
    2023-09-22, 10:10 a.m.
    Contribute Oral

    The ion source discharge influences the plasma-facing surfaces by impinging fluxes of ions, radicals and photons. This plasma surface interaction is particularly important for, but not limited to, caesiated ion sources for negative hydrogen ions due to its influence on the surface work function and possible photo-emission of electrons into the plasma sheath. While the role of ions and radicals...

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  51. Damon Todd (Lawrence Berkeley National Laboratory)
    2023-09-22, 11:00 a.m.
    Invited Oral

    The superconducting ECR ion source VENUS remains one of the world’s highest-performing ECRs for producing high-current, highly-charged ion beams. However, VENUS has up-to-twenty control parameters defining an operation space that is largely unexplored and inside which record beams are still produced via dedicated tuning time. This size of operation space has proven manageable for computer...

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  52. Richard Racz (Institute for Nuclear Research (Atomki))
    2023-09-22, 11:30 a.m.
    Invited Oral

    ECR (Electron Cyclotron Resonance) Ion Sources (ECRIS) are widely used to provide highly charged heavy ions for high energy accelerators. In their plasmas, ECRISs are able to generate electron population having enough high energy to effectively ionize the atoms up to their inner shells. The quality (intensity, emittance, stability) of the ion beam used by the end-stations of the accelerators...

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  53. Benoît Gall (IPHC / Université de Strasbourg)
    2023-09-22, 12:00 p.m.
    Contribute Oral

    Some metallic ion beams such as titanium are quite difficult to produce at the intensity level required in order to deliver several particle micro-amperes on target for nuclear physics experiments. At the University of Jyväskylä (JYFL), Matti Nurmia proposed to use organometallic compounds giving birth to the so-called MIVOC method [1]. Ferrocene is the archetype of metallic beams procced via...

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  54. Shixiang Peng (Peking University)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    In a modern ion implanter, plasma flood gun (PFG) is used to neutralize wafer charge during doping process, preventing the breakdown of floating wafers caused by the space charge accumulation. Surface wave plasma (SWP) source that has a simple structure and no hot filament requirement, which can avoid metal pollution, is a potential competitive prospect as a PFG for ion implanter. At Peking...

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  55. Lihua Chen (中国原子能科学研究院)
    Applications of Ion Sources
    Poster (by default)

    Neutron generator has the characteristics of high neutron energy generation, high inherent safety and flexible use scenarios, and is widely used in many fields, such as scientific research, activation analysis and contraband monitoring. This paper introduces the development of a small Neutron generator based on ECR source, which is being developed by China Institute of Atomic Energy. The...

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  56. Bo Liu (University of Science and Technology of China)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    The negative ion based neutral beam injector (NNBI) of 400 keV beam energy is a subproject of Comprehensive Research Facility for Fusion Technology (CRAFT) in China. A core snubber will be used to absorb the energy released by the stray capacitance during the occurrence of accelerator ignition faults, avoiding greater losses. The equivalent model of the CRAFT NNBI high potential circuit was...

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  57. Andrew Cooper (Los Alamos National Laboratory)
    Production of High Intensity Ion Beams
    Poster (by default)

    The capability to directly study neutron capture reactions on radionuclides with half-lives on the order of minutes would allow key cross section measurements in nuclear astrophysics and energy applications. However, such experiments with stationary targets are currently impossible because of signal detection and target sample fielding issues. To overcome these challenges, a neutron target...

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  58. Prof. Jun Hasegawa (Laboratory for Zero Carbon Energy, Institute of Innovative Research, Tokyo Institute of Technology)
    Key Technologies for Ion Sources
    Poster (by default)

    A laser ion source employing a cryogenically solidified gas target has been developed and demonstrated to supply highly charged carbon ions for a long period of time without being limited by the lifetime of the laser target. This new laser ion source is expected to be applied to the next-generation heavy ion cancer treatment accelerator based on inductive synchrotron technology. A solid carbon...

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  59. Giuseppe Chitarin (Univ. of Padova and Consorzio RFX)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    The negative ion sources currently used for Fusion applications produce tens of Amperes of Hydrogen or Deuterium ion current from a low-temperature (few eV) plasma. Being the negative ion current typically limited below 200 - 300 A/m2 at the extraction apertures, these sources can be quite large and their input power ranges from some tens to hundreds of kW. Two source types are currently used:...

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  60. Scott Schipmann (Avalanche Energy)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Avalanche Energy is developing deuterium ion beams for the Orbitron fusion concept. To successfully deliver high currents to the reactor, both focusing and steering are necessary. Many concepts proposed to solve this problem rely on separated focusing and steering sections. However, doing so inherently extends the beamline and may enhance beam losses. Combining the two into a single piece,...

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  61. Mr Xiang CAO (Sun Yat-sen University)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Pyroelectric neutron generator is an ideal neutron calibration source for free of radioactive contamination and high-frequency noise interference. The basic principle involves using pyroelectric crystals to generate high-voltage electric fields, which in turn accelerate deuterons produced by ionization to bombard deuterium-rich targets, initiating deuterium-deuterium (D-D)...

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  62. Michele Ballan (INFN-LNL)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    In the facilities for the production of Radioactive Ion Beams (RIBs) according to the Isotope Separation On Line (ISOL) technique, a production target is typically impinged by a high energy and high intensity primary beam, generating radioactive isotopes. The target is coupled to an ion source, where the produced species are ionized, allowing their electrostatic extraction and acceleration as...

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  63. Seth Veitzer (TECH-X CORPORATION)
    Applications of Ion Sources
    Poster (by default)

    Ion sources that use low-temperature plasma (LTP) discharges are used in a variety of applications, including ion implantation, mass spectrometry, and plasma processing. In recent years, there has been a growing interest in using particle-in-cell (PIC) modeling to improve the performance and optimization of LTP-based ion sources. PIC modeling is a powerful tool for simulating the dynamics of...

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  64. Giuseppe Castro (INFN-LNS)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Electron Cyclotron Resonance Ion Sources (ECRIS) are widely used to produce highly charged high intensity ion beams for research, medical and industrial applications.
    ECRIS performances, namely the charge state distribution and beam intensity, depend critically on the electron energy distribution function. Further improvements of ECRIS performances require a deeper and deeper understanding...

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  65. Glynnis Mae Saquilayan (RIKEN)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The beam emittance of extracted ions from ion sources is an important parameter relating to the beam quality of high energy accelerators such as the Radioactive Isotope beam Factory (RIBF) in RIKEN. In order to improve the output beam intensity and transmission efficiency to be well within the acceptance range of low-energy beam transport systems, it is important to maintain a low beam...

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  66. Yasuyuki Tanaka (National Institutes for Quantum Science and Technology (QST))
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The neutral beam injector for heating & current drive (HNB) for ITER requires the deuterium negative ion beam (D-) with 1 MeV, 40 A (200 A/m2) for 3600 s and hydrogen negative ion beam (H-) with 870 keV, 46 A (230 A/m2) for 1000 s. The required beam divergence angle is less than 7 mrad. Ensuring this beam divergence angle is essential to suppress...

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  67. Dr Vladlen Podolsky (Avalanche Energy)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Avalanche Energy is developing deuterium ion beams for the Orbitron fusion concept. For these and similar projects, modification of off-the-shelf high current ion sources enables affordable and rapidly accessible alternatives to custom-built systems. We have successfully operated the Veeco Mark 1 broad beam source on deuterium to create multi-keV energy ions. By applying custom optics and...

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  68. Sung-Ryul Huh (Korea Atomic Energy Research Institute)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    A cesium-free negative hydrogen/deuterium ion source system using two pulsed plasma sources has recently developed at Korea Atomic Energy Research Institute. The system operates with two alternate pulsing sequences related to the respective plasma sources, thereby switching the plasmas in the after-glow state in an alternating manner. As a result, the ion source system can offer a continuous...

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  69. Kaoru Ishikuro (Nagaoka University of Technology)
    Production of High Intensity Ion Beams
    Poster (by default)

    Applying a solenoidal magnetic field to a laser produced plasma is a method to increase the ion beam current supplied from a laser ion source. The purpose of this study is to investigate the ion charge state dependence of the beam current increase in the laser ion source by applying a solenoidal magnetic field. The plasma generated by a Nd:YAG laser was injected into a magnetic field generated...

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  70. Christopher Charles (TRIUMF)
    Production of Highly charged Ion Beams
    Poster (by default)

    We discuss the development of novel lanthanide beams at TRIUMF’s Off-Line Ion Sources (OLIS) Facility, focusing here on $^{140}$Ce$^{+n}$ for astrophysical research and molecule formation studies between halogens and lanthanides for electron dipole moment measurements. Cerium is the first lanthanide beam created at the OLIS facility by dual frequency electron cyclotron resonance (ECR) using a...

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  71. Masashi Kisaki (National Institutes for Quantum sience and Technology)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    Neutral beam system for heating & current drive (HNB) of ITER requires high power beams of 0.87 MeV and 46 A (230 Am-2) hydrogen negative ion (H-) for 1000 s, and of 1 MeV and 40 A (200 Am-2) deuterium negative ion (D-) for 3600 s. The H- ion beam demonstration toward 0.87 MeV and 230 A/m2 for 300 s, where the beam duration exceeds 50 s required in the initial HNB operation, is under progress...

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  72. Dr Suresh Saminathan (TRIUMF)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    A compact surface ion source was designed and commissioned for commissioning the low energy beam facilities of ARIEL facility at TRIUMF. The ion source was based on the principle of surface ionization, in which ions are generated from a neutral atom by impact with a solid surface. The design of the ion source considered several factors, including the type of ion beams, beam intensity, the beam...

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  73. Shadrach Hepner (Avalanche Energy Designs)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Avalanche Energy is developing deuterium ion beams for the Orbitron fusion concept. To understand the fusion output of the reactor, knowledge of the ion beam species and energy composition is paramount. We have successfully implemented a Thomson Parabola to determine the relative composition and energy spread of multiple species in the beam. To distinguish species within a wide range of masses...

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  74. Mr Behnam Ashrafkhani (University of Calgary)
    Key Technologies for Ion Sources
    Poster (by default)

    Laser ablation source (LAS) is an adaptable and efficient ion production technique for mass spectrometry, allowing for flexible analysis of various sample types. By depositing laser energy into the target, atoms or molecules in the sample are ionized. The development of a LAS for supplying stable isotopes to TRIUMF's TITAN platform enables novel studies, such as isotope abundance measurement...

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  75. Luigi Celona (INFN-LNS)
    Key Technologies for Ion Sources
    Poster (by default)

    An innovative plasma chamber for Electron Cyclotron Resonance Ion Sources has been developed at INFN and will soon be installed and tested with the AISHa (Advanced Ion Source for Hadrontherapy) ion source. It consists in inserting a particular liner into the existing chamber, which allows an electrical segmentation of the internal walls of the chamber. The purpose of this system is to reduce...

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  76. Richard Vondrasek (Argonne National Laboratory)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Responding to a request by the user community for higher beam intensities, an upgrade of the Argonne National Laboratory ECR2 ion source is in progress. The upgrade has three main constraints: 1) The overall source architecture as defined by the solenoid coils cannot change, 2) radial access to the plasma chamber has to be maintained, and 3) the amount of time the source can be shut down for...

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  77. Dr Robert Welton (ORNL-SNS)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The U.S. Spallation Neutron Source (SNS) is a state-of-the-art neutron scattering facility delivering the world’s most intense pulsed neutron beams to a wide array of instruments which are used to conduct investigations in many fields of science and engineering. Neutrons are produced by spallation reactions within a liquid Hg target bombarded by protons from a storage ring that is supplied by...

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  78. Wang Lu (Institute of Modern Physics)
    Production of Highly charged Ion Beams
    Poster (by default)

    With the successful development of inductive oven in 2019, there are three kinds of metal ovens at Institute of Modern Physics (IMP) now: low temperature oven, inductive high temperature oven and traditional mini-oven. To expand the range of temperature coverage, a new resistive medium temperature oven has been proposed in 2022 and fabricated in 2023. It is designed for the optimal working...

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  79. Junwei Xie (Institute Of Plasma Physics Chinese Academy Of Sciences)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    Neutral beam injection (NBI) is an indispensable auxiliary heating method used in thermonuclear magnetic confinement fusion devices. The Comprehensive Research Facility for Fusion Technology (CRAFT) needs a well-matched neutral beam injection system for experimental research. The condition that a high current beam with high beam energy is needed in the process of fusion can be satisfied by a...

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  80. Dr Suresh Saminathan (TRIUMF)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The ion source and injection system beamline is used to transport the $300\,$keV $\rm{H}^-$ beam from the ion source to the injection point of the $500\,$MeV cyclotron at TRIUMF. A new ion beam transport system has been designed to transport a highly intense and bright beam extracted from the $\rm{H}^-$ ion source. This new system will be installed at the new injection terminal for TRIUMF's...

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  81. Haifa Alyousef (Department of Physics, College of Science, Princess Nourah bint Abdulrahman University - P.O. Box 84428, Riyadh 11671, Saudi Arabia))
    Applications of Ion Sources
    Poster (by default)

    For this work, a cold cathode ion source with a Langmuir electric probe was constructed to produce an ion beam that could be successfully applied to a variety of applications. A steady discharge plasma media was produced by adjusting its operation conditions, such as the discharge voltages, electrode gap, as well as gas pressure. Additionally, the I-V plasma graph is recorded by inserting an...

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  82. Qi Wu (Institute of Modern physics,CAS)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    A transportable compact neutron source is under development for nondestructive testing of concrete structures such as bridges. It consists of a compact proton injector, a 2.5 MeV Radio-Frequency Quadrupole (RFQ) linac and lithium target. To meet the requirements of a 2.5 MeV RFQ linac, a new compact ion Source-LEBT integrated proton injector was developed at IMP. It includes a permanent magnet...

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  83. Takanori Shibata (KEK)
    Key Technologies for Ion Sources
    Poster (by default)

    We have been conducting the test of a new home-made internal antenna for the J-PARC RF-driven cesiated H$^-$ ion source. After the development of the first J-PARC-made antenna, the composition of the porcelain enamel coating of the antenna was changed to reduce possible outgassing of the impurities from the previous antenna coating. During the test of high-density plasma production by the new...

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  84. Miguel LEON LOPEZ (CIEMAT)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    Abstract:

    IRISC (Internal Radiofrequency Ion Source for Cyclotrons) is an innovative design of an internal ion source, primarily for producing H- ions, in which radiofrequency (RF) power is supplied to its electrodes for achieving electron emission. Theoretical work shows that both lower electrode sputtering and higher ion production efficiency may be achieved as compared to its standard...

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  85. Yasuyuki Ishii (National Institutes for Quantum Science and Technology)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    A penning ion source with a filament has been developed for a compact ion microbeam system to form submicron ion beam. A duoplasmatron-type ion source has, so far, been used for the system. However, the duoplasmatorn-type ion source is large power consumption as well as a large size. It is an obstacle to reduce the size of the system. As an ion source to overcome the demerits, a penning gauge...

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  86. Yasuyuki Morita (RIKEN)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The Nishina Center for Accelerator Science uses a pepperpot emittance monitor to measure the emittance of low-energy beams from ion sources. PPEM does not require moving slits, etc. Therefore, four-dimensional information of (x,x',y,y') can be measured in a short time. On the other hand, it is difficult to identify the origin of the spot. We are therefore attempting to identify the origin of...

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  87. Min Park (Korea institute of Fusion Energy)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    The current ion sources employed in the KSTAR (Korea Superconducting Tokamak Advanced Research) neutral beam injection system utilize conventional filament-driven multicusp ion sources. However, the primary limitations of this source arise from the usage of 12 tungsten filaments, leading to complexities and maintenance issues. To overcome these drawbacks, the development of an RF-driven ion...

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  88. Nagaaki Kamiguchi (Sumitomo Heavy Industries, Ltd.)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The cold cathode type PIG ion sources were often employed for compact cyclotrons with high magnetic field as internal source. The ion sources are preferable to conduct maintenance easily without vacuum break of cyclotrons to avoid long downtime. In this study, cold cathode PIG H+ ion source was developed with extraction mechanism along to main magnetic field direction for the spiral sector AVF...

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  89. Yahong XIE (Institute of Plasma Physics,Chinese Academy of Sciences)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    The Comprehensive Research Facility for Fusion Technology (CRAFT) is a large scientific device that is preferentially deployed for the construction of major national science and technology infrastructures. A radio frequency (RF) negative ion based neutral beam injection (NNBI) system with beam energy of 400 keV, beam power of 2 MW and beam duration of 100 s was designed to deliver energetic...

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  90. Lakshmy PS (Inter University Accelerator Centre)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The use of high intensity, heavy ions from an ECR ion source for heavy ion accelerators usually entails the employment of a low energy beam transport (LEBT) section and magnetic charge state analysis, but space charge can severely limit the transmission. It has been proposed [1] instead to use a Radio Frequency Quadrupole (RFQ) to efficiently address this problem. The stray magnetic field of...

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  91. Christopher Charles (TRIUMF)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Under operational conditions, high-voltage breakdown continues to occur inside the electron beam ion source (EBIS) at CANREB (the CANadian Rare isotope laboratory with Electron Beam ion source). Discharge tracks along components inside the high-vacuum together with data acquired during use of the system have isolated the most serious discharges to the collector trumpet (CT) region for a...

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  92. KEERTHI JAYAMANNA (TRIUMF)
    Production of Highly charged Ion Beams
    Poster (by default)

    In 2008, a SuperNanogan ECR ion source from PANTECHNIK was introduced in addition to an in-house developed microwave ion source and a surface ion source to complement the TRIUMF offline ion source facility to provide highly charged ions to ISAC experiments. Originally, it employed a 400 W Travelling Wave Tube Amplifier (TWTA) for RF heating, but less than 50 W was enough to produce all the...

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  93. Mamiko Sasao (Organization for Research Initiatives and Development, Doshisha University)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    The work function of plasma electrodes (PE) in negative hydrogen ion sources plays an important role to increase the H-/D- yields, and cesium (Cs) are currently used to control the work function. It has been known that a half monolayer (or less) Cs coverage shows the minimum work function, but it can be decreased more when the surface is immersed in a hydrogen plasma (Wada et al., 1990, and...

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  94. Dr Kyounghun Yoo (Institiute for Basic Science)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The Rare Isotope Accelerator complex for ON-line experiments (RAON) was constructed to produce more exotic rare isotopes (RI) by combining the ISOL and IF methods. In the ISOL facility, RIs are generated in the Target/Ion Source (TIS) module with the proton beam and extracted to the ISOL beamline. The properties of the RI ion beam transported through the ISOL beamline should be matched to the...

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  95. Jibo Li (Institute of Modern Physics, Chinese Academy of Sciences)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    Previous studies indicate that the biased disk enhances the charge state distribution (CSD) in the plasma in continuous wave (CW) mode and it also improves the ion flux towards the extraction in pulsed mode. However, in these studies the biased disk voltage is always shifted from 0 V to a certain value (or vice versa) with different timing, for an electron cyclotron resonance (ECR) ion source...

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  96. Katsuya Hayashi (Keio University)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    Recently, it has been observed in RF H- sources that the beam optics, for example, the beam divergence angle oscillates periodically[1]. Therefore, it is important to understand the effect of time-oscillation on the plasma meniscus in the downstream extraction region close to the extraction hole under the existence of a large amount of negative ions.
      As a first step for understanding...

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  97. Janilee Benitez (Lawrence Berkeley National Lab)
    Production of High Intensity Ion Beams
    Poster (by default)

    Recent superheavy element production research has involved the bombardment of heavy-element foils by high currents of neutron-rich ion beams having atomic numbers near 20 and energies near 5 MeV/nucleon. Production rates scale with incident current, and the 88-Inch Cyclotron at LBNL has demonstrated the ability to deliver over 2 pµA for some of these beams largely because of its injector: the...

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  98. Yushi Fujimura (Osaka Univ.)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    We have been studying efficient production of multicharged ions in an electron cyclotron resonance ion source (ECRIS). The gas mixing method, in which low Z gas is mixed into produced plasma, is known as a relatively simple method for highly efficient production of multicharged ions. In addition, it is expected that heating low Z ions selectively by ion cyclotron resonance (ICR) will further...

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  99. Engrhyt Rattanawongnara (SOKENDAI university)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Negative-ion density measurement in negative-ion sources is still in demand for improving the design and efficiency of the sources [1,2].
    A new analysis method called the 'electron reduction Langmuir probe model' is developed for an area that cannot use a laser-related measurement [3], such as inside the extraction hole.
    A validity check of the new analysis is performed in hydrogen and...

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  100. Ms Mana Miyagawa (Sumitomo Heavy Ibdustries,Ltd)
    Production of Highly charged Ion Beams
    Poster (by default)

    Kei3 is a prototype of compact ECR ion source developed for various ion production at QST-NIRS. It has confirmed that Kei3 has an ability to produce highly charged heavy ion, for example, carbon, neon and argon, but the beam current was not high enough. To improve this situation, we optimized microwave frequency and injection position in the plasma chamber.
    Microwave has a large effect to...

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  101. Fernando Alejandro Maldonado Millan (UVIC/TRIUMF)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The FEBIAD ion source is routinely used to produce radioactive ions of halogens, molecules, and noble gases in several ISOL facilities worldwide. At TRIUMF, an extensive numerical and experimental campaign has been performed to fundamentally understand the source while improving its reliability and overall performance. Particularly, the cathode temperature has been studied by pyrometric...

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  102. Minkeun Lee (Seoul National University)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    In this study, we conducted experimental study on a hot-cathode, multi-cusp electron source as charge neutralizer device for ion implanters. This device is divided into a plasma source area using a hot-cathode and magnetic multi-cusp, and a transport area that transports extracted electrons through an axial magnetic field by the electromagnet. We utilized a biased mesh to measure the quantity...

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  103. Kazumasa Takahashi (Nagaoka University of Technology)
    Production of High Intensity Ion Beams
    Poster (by default)

    Laser ion sources are expected to be used in various applications of heavy ion beam technology. The plasma direct injection scheme (DPIS) is a method used to accelerate high-current ion beams extracted from a laser ion source, which are then injected into a radio frequency quadrupole (RFQ) linear accelerator. In this study, a new injection method was demonstrated that avoids the RF field of...

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  104. Takanori Shibata (KEK)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    An internal antenna type RF driven negative hydrogen (H$^-$) ion source supplies beams to the J-PARC accelerator facility. The H$^-$ ion beam current exhibits high stability, while it fluctuates with less than 5% amplitude of the DC current when a Faraday cup measures the current extracted from the source mounted on a test stand. Two frequencies are identified as the main oscillation...

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  105. Alessio Galatà (INFN-Legnaro National Laboratories)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    The two-close frequency heating (TCFH) is a new implementation of the well-known two frequency heating. In TCFH, the two frequencies differ less than 200-300 MHz each other in order to establish two contiguous ECR resonance zones. TCFH has been proved to be a powerful technique to suppress plasma instabilities in Electron Cyclotron Resonance Ion Sources (ECRIS), as well as to improve their...

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  106. Taneli Kalvas (University of Jyväskylä, Department of Physics)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The formation of self-focused ion beam with a small diameter is proposed. The device for the formation of self-focused ion beam consists of a hollow anode and enveloped anode, separated from the anode by an insulator, gas delivery system. A discharge is supported by the voltage applied between the cathode and anode. The ion beam is self-focused by the spherical emission surface of emitting...

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  107. Ville Toivanen (Accelerator Laboratory, Department of Physics, University of Jyväskylä)
    Production of Highly charged Ion Beams
    Poster (by default)

    The CUBE-ECRIS is a recently commissioned permanent magnet electron cyclotron resonance (ECR) ion source developed at the university of Jyväskylä accelerator laboratory. The special features of the new ion source design include an unconventional quadrupole minimum-B magnetic field structure and a slit beam extraction system necessitated by the line-shaped plasma loss fluxes. The 10 GHz...

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  108. Hirotsugu Kashiwagi (QST)
    Applications of Ion Sources
    Poster (by default)

    The 400 kV ion implanter in Takasaki Ion Accelerators for Advanced Radiation Application (TIARA) is mainly used for research and developments in the field of material science, and it is necessary to produce beams of various ion species. Therefore, we are developing a laser ion source for an ion implanter on an offline test bench to produce beams of various ion species and to switch quickly...

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  109. Amith Hulikal Narayan (Oak Ridge National Laboratory), Baoxi Han (Oak Ridge National Laboratory), Robert Welton (Oak Ridge National Laboratory), Chris Stinson (Oak Ridge National Laboratory), Greg Terszakowec (Oak Ridge National Laboratory), Chip Piller (Oak Ridge National Laboratory), Vic Andzulis (Oak Ridge National Laboratory)
    Key Technologies for Ion Sources
    Poster (by default)

    The baseline RF-driven H- ion source configuration at the Spallation Neutron Source (SNS) facility uses a continuous wave (CW) 600 W 13.56 MHz RF system to ignite and maintain a low-intensity plasma inside the ion source vacuum chamber. After the continuous low-intensity 13.56 MHz plasma has been established, a pulsed (typical 1 ms pulse width and 60 Hz pulse repetition rate) 80 kW 2 MHz RF...

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  110. Dr Yuji Shimabukuro (University of California, Irvine)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    At TAE Technologies, a next-generation Field-Reversed Configuration (FRC), known as Copernicus, is being built. The current device, C-2W, has achieved steady-state beam-driven FRCs up to 30 ms using four 15 kV and four 40 kV NBIs(neutral beam injector)[1]. In order to increase FRC performance in the next generation device, both beam energy and beam power will be increased beyond these...

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  111. Ralitsa Mancheva (CERN, KU Leuven)
    Key Technologies for Ion Sources
    Poster (by default)

    Resonance laser ionization is an efficient and highly selective method for producing ions of a wide variety of elements. In the laser ion source of ISOLDE – RILIS (Resonance Ionization Laser Ion Source), the laser interaction with the atoms takes place inside a metal tube which is heated to temperatures of up to 2200 degrees Celsius. This heating induces electron emission from the metal walls,...

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  112. Wiktoria Wojtaczka (KU Leuven)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The ISOL (Isotope Separation On-Line) method has been widely used for the production of radioactive ion beams for nuclear physics research. The development of isotope extraction via molecular sidebands has gained significant interest in recent years [1,2,3] because of their potential to provide access to less volatile elements that are otherwise not possible to extract out of the target. In...

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  113. Sergey Kondrashev (Brookhaven National Laboratory)
    Key Technologies for Ion Sources
    Poster (by default)

    We have developed method of in situ effective pumping speed measurements based on injecting of small amount of gas into a volume of a vacuum chamber and subsequent recording of pressure burst decay time dynamics using Residual Gas Analyzer (RGA). Within the certain range, the pressure burst caused by injected gas will drop exponentially in time and exponential coefficient of such pressure...

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  114. Yushi Kato (Osaka Univ.)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    We have been experimentally measuring the charge state distribution of the multiply-charged ion current generated and extracted from an electron cyclotron resonance (ECR) ion source (ECRIS), and plasma parameters such as electron density, electron temperature, and space potential of the plasma in the ECRIS, and then investigating the correspondence between them. According to the accessibility...

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  115. Herman Kremers (University Medical Center Groningen)
    Key Technologies for Ion Sources
    Poster (by default)

    Due to the demand for intense high-charged stable ion beams for medical and nuclear physics a traveling-wave-tube (TWT) based RF generator has been installed and commissioned at the Advanced Electron Cyclotron Resonance Upgrade (AECR-U) ion source at the UMCG-PARTREC facility. The generator comprises 2 x 750W in-phase combining TWT RF generators with an output frequency range of 12.75-14.5...

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  116. Vladlen Podolsky (Avalanche Energy)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Avalanche Energy is developing deuterium ion beams for the Orbitron fusion concept. To deliver a maximized, focused beam to the reactor, some of our experiment configurations utilize a Veeco Mark 1 broad beam ion source. To focus this beam into a small aperture, carefully designed optics are vital, the design of which is a nontrivial process.
    The performance of the beam optics is a function...

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  117. Minkeun Lee (Seoul National University)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    In this study, plasma parameters and instability were measured using a single Langmuir probe in a hot cathode Penning ion gauge ion source. Experiments were performed with argon gas at an operating pressure of 1 mTorr. We observed an increase in electron temperature corresponding to an increase in discharge current. At the same time, we noted an increase in plasma instability with increasing...

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  118. Dr Emanuele Sartori (Università degli Studi di Padova)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    Most of the currently operating Negative ion Neutral Beam Injectors (N-NBIs) exploit filament-powered sources for the generation of beam ions. Being widely used in fusion experiments, the arc technology has been thoroughly investigated and optimized over the years, allowing to achieve excellent performances in terms of extracted beam optics.
    The source geometry, the magnetic field topology...

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  119. Christopher Charles (TRIUMF)
    Production of Highly charged Ion Beams
    Poster (by default)

    We describe the development of novel $^{31}$P$^{+n}$ and $^{133}$Cs$^{+n}$ beams for fundamental nuclear astrophysics research at TRIUMF’s ISAC (Isotope Separator and ACcelerator) complex. Both beams were individually created for different experiments, and for the first time at TRIUMF’s Off-Line Ion Sources (OLIS) facility by dual-frequency electron cyclotron resonance (ECR) using a...

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  120. Jungbae Bahng (Kangwon National University Hospital)
    Production of High Intensity Ion Beams
    Poster (by default)

    Ion beams are employed in various fields such as semiconductor manufacturing, surface modification, and material science. The uniformity of ion beams is crucial in many applications, but conventional ion sources that use a single filament often limit the uniformity and intensity of the ion beam. This paper presents a study that aims to optimize a multi-filament ion source to enhance the...

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  121. Fernando Alejandro Maldonado Millan (UVIC/TRIUMF)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The ISAC-FEBIAD ion source is an electron impact ion source typically used to ionize radioactive molecules or isotopes of elements with ionization potentials higher than 10 eV. The source key tuning parameters are the anode voltage that defines the electron energy, and the magnetic field that controls the electron density inside the anode volume. Both values are only varied in a small and...

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  122. Gabriel Tabacaru (Cyclotron Institute, Texas A&M University)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    Cyclotron Institute at Texas A&M University started a project to develop the reacceleration of radioactive ions using the two operational cyclotrons and a Charge Breeding ECR ion source. The radioactive ions are produced primarily via (p,n) reactions using the well-known IGISOL technique. The reaction products are transported into a Charge Breeder ECR ion source where their charge state is...

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  123. Eugenia Naselli (Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud (INFN, LNS))
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    Metals can be injected into electron cyclotron resonance ion sources (ECRIS) via many techniques, among which resistive ovens are used to vaporise neutral metals, later captured by the energetic plasma environment that will stepwise ionise them, hence giving multiply charged ion beams for accelerators. Recently, PANDORA, a novel ECR plasma trap, has been conceived to perform interdisciplinary...

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  124. Kengo Iwanaka (Keio University)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    Recently, the Research and development Negative Ion Source (RNIS) at National Institute for Fusion Science (NIFS) changed operation gas from hydrogen to deuterium. It is reported that the electron density differs by around three times with the operation gas [1]. The physical mechanism of the significant increase of the electron density is still not clear.
    In the previous studies [2], a...

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  125. Yuwen Yang (Institute of Plasma Physics,Chinese Academy of Sciences)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    A negative ion based neutral beam injection (NNBI) test facility is one of the significant components of Comprehensive Research Facility for Fusion Technology (CRAFT) in China. A quarter-size beam source for the CRAFT NNBI test facility has been developed firstly. It consists of a single driver RF plasma source and a negative ion accelerator. The typical extraction voltage is 4~8 kV and the...

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  126. Ram Swaroop (Central University of Punjab Bathinda Ghudda), Dr G.O Rodrigues (Inter University Accelerator Centre)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    Microwave plasmas fascinate researchers and scientists, yet it is a challenging field of research. The Central University of Punjab (CUPB) in Bathinda, established a 2450MHZ microwave flash design facility [1,2 ] to examine the properties of this peculiar kind of plasma. During ignition of the plasma, plasma shifting in the waveguide caused several problems. Even though microwave coupling and...

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  127. Rakhi (Indian Institute of Technology Ropar, 140001, India)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    The dynamic of self-organized nanopatterns on solid surfaces has been studied using low energy ion beam but it remains a central theme within ion beam sputtering still. The previous work for dynamical characterization has been focused on ion sputtering of Silicon surfaces using unconventional methods. To invoke new phenomena is not achievable using single fixed beam configuration.
    In this...

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  128. Rainer Rockenbauer
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    MedAustron is a synchrotron based ion beam therapy centre located in Lower Austria. Proton and carbon ion energies in the three treatment rooms range from 62-252 MeV and 120-400 MeV/u, respectively. A fourth non-clinical research room is used to commission helium ion beams, among other research activities.
    The injector features three identical electron cyclotron resonance ion sources from...

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  129. Olli Tarvainen (UK Science and Technology Facilities Council)
    Applications of Ion Sources
    Poster (by default)

    We present the status of the ion source and low energy beam transport prototyping activities for a single-ended heavy ion time-of-flight elastic recoil detection analysis (ToF-ERDA) equipment for depth profiling of light elements. The environmentally friendly concept is based on a permanent magnet ECR ion source and dipole magnet on a 500 kV platform without SF$_6$ insulation, producing high...

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  130. Philip Jackle (Simon Fraser University)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    Negative helium ions are typically created from positive helium ions which undergo double charge exchange with a neutral, atomic vapour, in a metallic vapour charge exchange apparatus. For high production rates of He⁻ (1 to 5%) alkali metals are used as the charge exchange material. However, alkali vapours are deleterious in vacuum systems, particularly ones with nearby electrodes for beam...

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  131. Fernando Alejandro Maldonado Millan (UVIC/TRIUMF)
    Production of Highly charged Ion Beams
    Poster (by default)

    Highly Charged Ions (HCIs) enable increased precision when measuring the masses of short-lived radioactive ions. The TRIUMF's Ion Trap for Atomic and Nuclear Science (TITAN) facility receives radioactive, singly charged ions (SCIs) from the ISAC facility before charge-breeding them to HCIs. Specifically, the TITAN Electron Beam Ion Trap (EBIT) generates the higher charge states, while the...

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  132. Dr Joele Mira (iThemba LABS - NRF)
    Production of High Intensity Ion Beams
    Poster (by default)

    The paper presents measurements on the production of ruthenium ion beams from high isotope purity using MIVOC method. The measurement was carried out at iThemba LABS using one of the two ECR ion source which is the copy of the Grenoble Test Source (GTS). Due to many existing isotopes with similar abundances of Ruthenium (96Ru abundance 5.5%, 98Ru abundance 1.9%, 99Ru abundance 12.7%, 100Ru...

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  133. Jiaqing Li (Institute of Modern Physics, Chinese Academy of Sciences)
    Key Technologies for Ion Sources
    Poster (by default)

    An all-permanent magnet electron cyclotron resonance ion source-LAPECR3 (Lanzhou All Permanent magnet Electron Cyclotron Resonance ion source No.3) had been developed as the dedicated C5+ ion injector of Heavy Ion Medical Machine (HIMM) accelerator facility since 2009 in China. The first HIMM demo facility was built in Wuwei city in 2015, and the facility had been officially licensed to treat...

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  134. Glynnis Mae Saquilayan (RIKEN)
    Production of High Intensity Ion Beams
    Poster (by default)

    Production of intense highly charged uranium (U) ion beam is strongly demanded to produce intense radioactive isotope (RI) beam at several accelerator facilities, because of its high efficiency of RI production with the in-flight fission of U ion. At RIKEN, intense highly charged U ion beam from ion source has been required for this purpose. To meet the requirement, in the beginning, we used...

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  135. lixuan Li
    Production of High Intensity Ion Beams
    Poster (by default)

    Intense highly charged uranium ion beam production is essential for heavy ion accelerators in operation and those under construction. Although metallic beam production is tricky, based on our earlier study, intense uranium beams can be expected when operating a third generation electron cyclotron resonance (ECR) ion source especially in afterglow mode with double frequency heating. In this...

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  136. Andrew Paul (D-Pace Inc.)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    Negative ion beams are used for a wide range of applications when tandem accelerators are leveraged. Research areas which utilize tandems include nuclear structure, environmental studies, and materials characterization. Tandem accelerators are also used for industrial applications such as ion implantation in semiconductor devices, as well as for medical applications such as Boron Neutron...

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  137. Takeshi Kanesue (Brookhaven National Laboratory)
    Applications of Ion Sources
    Poster (by default)

    The LION2 is being constructed to replace the existing LION, which is a laser ablation ion source to provide various species of heavy ions for Relativistic Heavy Ion Collider (RHIC) and NASA Space Radiation Laboratory (NSRL) at BNL. LION and LION2 provide singly charged heavy ions, which are transported and then trapped by an electron beam ion source, so called Extended-EBIS, for further...

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  138. Mathieu Cavenaile (TRIUMF)
    Production of Highly charged Ion Beams
    Poster (by default)

    The CANadian Rare isotope facility with Electron-Beam ion source (CANREB) at TRIUMF is set to deliver rare isotope beams in high charge states. In the Electron Beam Ion Source (EBIS) ions are charge-bred by collisions with an electron beam of up to 500 mA. A strong magnetic field (up to 6T) maximizes the overlap between ions and electron beam and increases the breeding efficiency. Ion...

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  139. Pierre Chauveau (GANIL)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The SPIRAL1 facility provides post-accelerated radioactive ion beams (RIBs) since 2001. Initially limited to isotopes of gaseous elements, SPIRAL1 has been upgraded over the last decade to produce radioactive ions of condensable elements. It does so by using both a hot 1+ ion source and an ECR Charge Breeder where the latter is used to increase the ion charge state for post-acceleration. The...

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  140. Xinyu Wang (Institute of Modern Physics, Chinese Academy of Sciences)
    Key Technologies for Ion Sources
    Poster (by default)

    To investigate the coupling efficiency between microwave with frequency above 20 GHz and plasma in an electron cyclotron resonance (ECR) ion source, a movable Vlasov launcher has been developed at Institute of Modern Physics (IMP). The beam intensity and axial bremsstrahlung were simultaneously measured with SECRAL-II (Superconducting ECR ion source with Advanced design in Lanzhou No. II) ion...

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  141. Dr Kyounghun Yoo (Institiute for Basic Science)
    Production of Highly charged Ion Beams
    Poster (by default)

    Highly charged ions (HCIs) are currently utilized in numerous fundamental and applied sciences, including astrophysics, dark matter search, optical clocks, semiconductor lithography, and quantum dot fabrication, to name just a few examples. At UNIST, a tabletop electron beam ion trap (EBIT) has been developed for creating and studying HCIs. The UNIST-EBIT compresses the electron beam by 72...

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  142. Fabio Maimone (GSI Helmholtzzentrum für Schwerionenforschung)
    Production of Highly charged Ion Beams
    Poster (by default)

    At GSI the CAPRICE ECRIS is in operation to deliver high-charge state ion beams from gaseous and metallic elements to the accelerator facility. In order to fulfill the demand for higher intensity and stability of high-charge state ions, a test campaign has been carried out at the ECR test bench. The objective of the measurements was the enhancement of ion source performance in terms of...

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  143. Yongjian Xu (Institute of plasma physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Unidirectional carbon fiber-carbon matrix (CFC) composite can be used to diagnose the main features of a particle beam such as its power, divergence and uniformity. Diagnostic calorimeter based on CFC has been developed by the research team of neutral beam injection (NBI) around the world because of its high space resolution. At ASIPP, a negative ion source based neutral beam injector is under...

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  144. Jens Lassen (TRIUMF)
    Applications of Ion Sources
    Poster (by default)

    The current status of the TRIUMF resonant ionization laser ion source (T RILIS) is that isotopes from 42 different elements have been delivered successfully and are part of the RILIS portfolio with ionization schemes for another 7 elements ready to be deployed on-line. As such the resonant ionization laser ion source is an indispensable ion source at TRIUMF’s isotope separator and accelerator...

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  145. Jake McLain (Argonne National Laboratory)
    Production of High Intensity Ion Beams
    Poster (by default)

    The ECR2 and ECR3 ion sources at the Argonne Tandem Linac Accelerator System (ATLAS) operate with two microwave frequencies, improving their performance over single frequency operation. A typical method for transmitting both microwave frequencies is by having two separate frequency generators with their own corresponding amplifiers. These amplifiers transmit their microwaves into the ion...

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  146. Takanori Shibata (J-PARC center / High Energy Accelerator Research Organization (KEK))
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    Temporal oscillation of the negative hydrogen ion ($\text{H}^-$) beam phase space in Radio Frequency (RF) ion source is a serious problem which causes increase in the beam divergence angle in the fusion application or unexpected beam loss due to Twiss mismatch in the accelerator application. Physical mechanism of the oscillation is investigated by a simple 3D Particle-In-Cell (PIC) model. The...

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  147. Hirotsugu Kashiwagi (QST)
    Production of High Intensity Ion Beams
    Poster (by default)

    The Laser Ion Source (LIS) can generate ion beams of various elements, including metals with high melting points. Since rapid beam switching is possible by loading multiple solid targets, we are developing LIS with the goal of mounting it in the 400 kV ion implanter, which requires a wide variety of ion species.
    LIS can generate a high current ion beam by increasing laser energy. Also, by...

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  148. Brad Schultz (TRIUMF)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The CANadian Rare isotope facility with Electron Beam ion source (CANREB) is part of the new Advanced Rare IsotopE Laboratory (ARIEL) at TRIUMF. CANREB can accept stable or rare isotope beams from a variety of ion sources. The injected beams are pulsed using a radiofrequency quadrupole cooler/buncher, and energy adjusted using a pulsed drift tube for injection into an electron beam ion source...

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  149. Dr Hyock-Jun Son (FRIB/MSU)
    Production of Highly charged Ion Beams
    Poster (by default)

    The Reaccelerator (ReA) of the Facility for Rare-Isotope Beams (FRIB) employs an Electron-Beam Ion Trap (EBIT) as a charge breeder to reaccelerate rare-isotope beams to several MeV/u. The ReA EBIT uses a Pierce-type electron gun with its cathode partially immersed in the fringe field of a 4-T superconducting solenoid. A barium-impregnated tungsten dispenser cathode is used to produce an...

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  150. Clayton Dickerson (Argonne National Laboratory)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    CARIBU (Californium Rare Isotope Breeder Upgrade) is a source of neutron-rich fission fragments from a plating of 252Cf. Operating for over a decade, CARIBU has provided unique beams for stopped and reaccelerated experiments. Unfortunately, consistently generating a thin plating of Cf has proved very difficult. To eliminate this risk and increase the overall intensity of n-rich ions, ATLAS...

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  151. Dr Seongjin Heo (Institute for Basic Science (IBS))
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The beamline of Isotope Separation On-Line (ISOL) system at RAON was constructed. The produced ions from the Target Ion Source (TIS) are cooled and bunched using the Radio Frequency Quadrupole Cooler Buncher (RFQ CB) to improve the charge breeding efficiency of the Electron Beam Ion Source (EBIS) charge breeder and the performance of the Multiple-Reflection Time-of-Flight Mass Spectrometer...

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  152. Robert Scott (Argonne National Laboratory)
    Applications of Ion Sources
    Poster (by default)

    The Argonne Tandem Linac Accelerator System (ATLAS) at Argonne National Laboratory typically operates 24 /7 with weekly ion beam changes and an annual 1 month maintenance period. Due to recent installations and upgrades at ATLAS, user demands for new beams and higher intensities have expanded an already diverse operational envelope of both electron cyclotron resonance ion sources (ECRIS), ECR2...

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  153. Haifa Alyousef (Department of Physics, College of Science, Princess Nourah bint Abdulrahman University - P.O. Box 84428, Riyadh 11671, Saudi Arabia))
    Applications of Ion Sources
    Poster (by default)

    In this study, we address the the effects of low energy hydrogen ion beam irradiation on the optical characteristics of polymeric nanocomposite films for used in optoelectronics devices. The composite films are irradiated using broad beam cold cathode ion source with hydrogen ion energy ranging from 1 to 6 keV. The techniques of X-ray diffraction, Fourier transform infrared spectrum, as well...

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  154. Ms Lakshmy PS (Inter University Accelerator Centre)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    P. S. Lakshmy*, Mukesh Kumar, R.K.Gurjar, Ruby Santhi and G.Rodrigues
    Inter University Accelerator Centre, Aruna Asaf Ali Marg, New Delhi, India.

    The 18 GHz High Temperature Superconducting (HTS) Electron Cyclotron Resonance Ion Source [1] is the main positive ion injector for the upcoming, High Current Injector (HCI) Programme which is presently being commissioned at IUAC, New Delhi. In...

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  155. Anthony Cooper (TAE Technology)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    TAE Technologies pursues an alternative approach to magnetically confined fusion with the advanced, beam-driven field-reversed configuration (FRC) [1]. Heating, current drive, and partial fueling from neutral beam injection are essential to sustainment of the FRC plasma [2]. The next generation device, Copernicus, aims to achieve the D-T reactor relevant plasma performance with a hydrogen...

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  156. Dr Caichao JIANG (Institute of Plasma Physics, Chinese Academy of Sciences)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    In order to meet the requirement of the neutral beam long pulse operation for CFETR and fusion reactor, it is urgent to carry out the research of high power RF ion source. As the extracted area of ion source is bigger, multi-driver is an inevitable choice. According to the structure of multi-driver, some problem such as, disturb between adjacent drivers and plasma uniformity, will occur. These...

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  157. Takeshi Kanesue (Brookhaven National Laboratory)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    A solenoid magnetic field along the expanding laser-produced plasma is an essential technique of a laser ablation ion source, which can increase ion beam current at beam extraction by a factor of 2. Solenoid field is also practically important for beam operation to control beam current without changing the condition of laser ablation. However, the motion of laser-produced plasma influenced by...

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  158. Moenir Sakieldien (iThemba LABS)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    At iThemba Laboratory for Accelerator Based Sciences (LABS), a Penning Ionization Gauge (PIG) Ion Source is used for proton production. The accelerated proton beam impinges on a target, and after chemical extraction and purification, is used to manufacture a range of radioisotopes. The accelerated proton beam is also used to study various low-cross section nuclear physics processes. Over the...

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  159. Masao Nakao (Gunma University)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    In Gunma University Heavy Ion Medical Center, carbon ion therapy has been performed since 2010. The carbon ion (C4+) for the injector is made with KeiGM ion source. There is another KeiGM ion source in Gunma University for the both the purpose of a reserve machine and for research and development. A wire-slit type emittance monitor has already been installed as a beam diagnostic...

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  160. Bing Tang
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The Beijing Radioactive ion beam facility Isotope Separator On-Line(BRISOL)is a radioactive ion beam facility based on a 100MeV cyclotron providing 200μA proton beam bombarding the thick target to produce radioactive nuclei, which are transferred into an ion source to produce singly charged ion beams. A surface ion source had been developed for BRISOL, and the first radioactive beams (37K+,...

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  161. Xie Ma (China Institute of Atomic Energy)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    On-line Isotope separator of Beijing radioactive ion-beam facility(BRISOL) produces medium and short-lived radio-isotope beams by irradiating a target with a 200-𝜇A 100-MeV proton beam provided by a cyclotron. Recently, UCx targets have been developed at BRISOL. At fisrt, lanthanum carbide has been chosen as an analogy for uranium carbide, so that air sensitive target material processing can...

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  162. Xufeng Peng (Institute of plasma physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences), Jianglong Wei (Institute of Plasma Physics, Chinese Academy of Sciences)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    The suppression of co-extracted electrons has always been one of the key problems in the operation of negative ion sources, as the co-extracted electrons not only cause energy waste, but also create a great heat load on the extraction grid (EG). A positive bias is usually applied to the plasma grid (PG) to reduce the co-extracted electron current. There are several ways to connect the bias...

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  163. Augustin Dubois, Olivier Delferriere (CEA-Saclay), Olivier Tuske (CEA SAclay, France)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Since 1995, the Laboratory for Accelerator Studies and Development at CEA Saclay specializes in producing ECR intense light Ion Sources, for high intensity proton or deuteron. The initial source SILHI designed for IPHI accelerator was the root of the sources provided to laboratories around the world, such as IFMIF, FAIR or SPIRAL2. In parallel, the Ion Source team started a new R&D program on...

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  164. Stephane Melanson (D-Pace)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    The TRIUMF licensed H$^{-}$ ion source is known to produce 15 mA of H$^{-}$ ions, but some applications, such as those using higher energy research cyclotrons, require the injection of both positive and negative ions. Furthermore, when using a tandem accelerator, there would be a benefit in using an ion source that can directly extract H$^{-}$ and He$^{+}$. In this case, a charge exchange...

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  165. Shixiang Peng (Peking University)
    Production of High Intensity Ion Beams
    Poster (by default)

    A miniaturized 2.45GHz microwave ion source (MIS) with plasma chamber of 30 mm x 40 mm and has the ability to produce more than 20 mA CW hydrogen ion beam with 180 W microwave power has been built at Peking University(PKU)[1]. To understand the plasma evolution mechanism of MIS, a hybrid discharge heating (HDH) mode that contains a surface wave plasma (SWP) ignition discharge process and an...

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  166. Sergiy Trotsenko (GSI Helmholtzzentrum für Schwerionenforschung GmbH)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    The HITRAP facility, located at the GSI Helmholtzzentrum für Schwerionenforschung GmbH in Darmstadt, Germany, is designed to decelerate, cool and transport heavy, highly charged ions (HCI) created by the GSI accelerator complex to various attached experiments. The system consists of a two-stage deceleration structure, an interdigital H-type linac (IH) and a radio-frequency quadrupole (RFQ),...

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  167. Joseph Tan (National Institute of Standards & Technology)
    Production of Highly charged Ion Beams
    Poster (by default)

    A room-temperature electron beam ion source/trap has been designed and constructed at the National Institute of Standards & Technology (NIST). Its peak magnetic field of 0.67 T is generated in an extremely compact architecture by embedding strong rare-earth (NdFeB) magnets within the drift tubes, which are partly constructed of electrical iron. Six ports in the midplane are available to...

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  168. Reinhard Heinke (CERN)
    Radioactive Ion Beam Sources and Charge Breeders
    Poster (by default)

    The Resonance Ionization Laser Ion Source RILIS, employing laser radiation in a hot cavity ion source diretly coupled to an isotope production target, has become a principal method for provision of radioactive ion beams at facilities world-wide, such as at CERN-ISOLDE or -MEDICIS. Stepwise resonant excitation and subsequent detachment of an electron via element-unique atomic shell transitions...

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  169. Mr Omorjit Singh Khwairakpam (INFN-LNL; University of Siena)
    Applications of Ion Sources
    Poster (by default)

    SPES is a 2°-generation ISOL facility in the last stage of construction in INFN-LNL, Italy. One of the many developmental activities carried out inside SPES project is a thermally optimized ion source (IS). The SPES surface ion source (made of Ta) was successfully tested in 2017 [1].
    In the beginning of 2023, the same SPES-IS has been used to test its performance as a resonance ionization...

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  170. Jeongil Heo (Institute for Basic Science)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    RAON(Rare isotope Accelerator complex for ON-line experiments) is a heavy ion accelerator that is being built in Daejeon, South Korea. RAON plans to operate a 28 GHz ECRIS(Electron Cyclotron Resonance Ion Source) with fully superconducting magnet and a 14.5 GHz ECR ion source with fully permanent magnet. The 14.5 GHz ECRIS was manufactured by PANTECHNIK and installed in our beam line in...

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  171. Hirotsugu Kashiwagi (QST)
    Production of High Intensity Ion Beams
    Poster (by default)

    In a laser ion source (LIS), a target material in a vacuum chamber absorbs focused laser energy to produce a dense plasma, from which the beam is extracted. The LIS can generate plasma from a variety of solid targets, and the ion species can be easily changed by replacing or mounting multiple target samples. Based on this feature, we are developing a LIS for ion implanters requiring a wide...

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  172. Alessio Galatà (INFN-Legnaro National Laboratories)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    In mass spectrometry of exotic ion beams a cold ion beam is required, to achieve a mass resolution goal of 1:20000, which is a typical requirement for nuclear physics studies of isobaric ions. In the radiofrequency (rf) quadrupole cooler (RFQC), which is a kind of linear ion trap, rf fields and ion-gas collisions may give considerable increase or decrease of the beam transverse emittance and...

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  173. Zehua Jia (imp)
    Beam Formation, Extraction, Transport, and Diagnostics
    Poster (by default)

    Due to the unique magnetic field structure of the Electron Cyclotron Resonance (ECR) ion source, conventional idealized beam models cannot adequately reproduce the state of high charge state ion beams extracted from it. Consequently, beam transport designs based on idealized models exhibit suboptimal performance in efficiently generating high-quality beams during practical transport. Advanced...

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  174. Dr KEERTHI JAYAMANNA (TRIUMF)
    Negative Ion Sources and Sources for Fusion Facilities
    Poster (by default)

    TRIUMF’s 500 MeV cyclotron has been powered by an arc discharge H− ion source developed in-house 30 years ago. Since then, new additions to TRIUMF, like ISAC, have required increasing amounts of beam current from the cyclotron. The ARIEL facility will also require an additional 100 μA, in addition to the existing 300 μA required by the current beam lines. To meet the growing intensity demands...

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  175. Kouki Iwahara (Osaka Univ.)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    We have been researching about efficient generation of multiply-charged Ar ion on electron cyclotron resonance ion source (ECRIS). Confining the plasma magnetically, ECRIS is one of the major ion sources on accelerators because it is possible to generate plasma efficiently by introducing microwaves. On conventional ECRIS, microwaves are introduced from upstream side of the mirror field at the...

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  176. Yuting Lu (Institute of Modern Physics, Chinese Academy of Sciences)
    Fundamental Processes in Ion Sources, Plasma
    Poster (by default)

    The spatially-resolved X-ray spectrum of laser-produced Al plasma near the target surface has been obtained in the energy range of 1.5-2.2 keV using a compact flat crystal spectrometer. The widely-used temperature and density diagnostics, the line ratios of Lyα/Heβ and IC/Heα, were measured and compared with the calculation results of a steady-state collisional-radiative model, so that the...

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