Paper | Title | Other Keywords | Page |
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MOAO01 | Status of the IsoDAR High-current H+2 Cyclotron (HCHC-XX) Development | rfq, cyclotron, target, proton | 12 |
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The potential existence of exotic neutrinos beyond the three standard model neutrinos is an important open question in particle physics. IsoDAR is a cyclotron-driven, pure electron-antineutrino source with a well-understood energy spectrum. High statistics of anti-electron neutrinos can be produced by IsoDAR, which, when coupled with an inverse beta decay detector such as the LSC at Yemilab, is capable of addressing observed anomalies attributed to sterile neutrinos at the 5 σ level using electron-flavor disappearance. To achieve this high significance, the IsoDAR cyclotron must produce 10 mA of protons at 60 MeV. This is an order of magnitude more current than any commercially available cyclotron has produced. To achieve this, IsoDAR takes advantage of several innovations in accelerator physics, including the use of H2+ and RFQ direct injection, paving the way as a new high power accelerator technology. These high currents also allow for new experiments in dark matter, as well as high production rates of rare isotopes such as Ac225 and Ge68. | |||
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Slides MOAO01 [30.289 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-MOAO01 | ||
About • | Received ※ 24 March 2023 — Revised ※ 24 May 2023 — Accepted ※ 06 July 2023 — Issue date ※ 11 July 2023 | ||
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MOBI01 | Summary of the Snowmass’21 Workshop on High Power Cyclotrons and FFAs | cyclotron, proton, target, space-charge | 20 |
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In this talk, we summarize the presentations and findings of the "Workshop on High Power Cyclotrons and FFAs" that we held online in September 2021. The workshop was held as part of the 2021 Snowmass Community Exercise, in which the US particle physics community came together in a year-long effort to provide suggestions for a long-term strategy for the field, and the "Accelerators for Neutrinos" subpanel thereof. Topics that were discussed during our high-power cyclotron workshop were the application of cyclotrons in particle physics, specifically neutrino physics, and as drivers for muon production. Furthermore, as these same accelerators have important applications in the fields of isotope production and possibly in energy research, we have included those topics as well. Finally, we took a look at Fixed Field Alternating Gradient accelerators (FFAs) and their potential to become high-intensity machines. | |||
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Slides MOBI01 [1.885 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-MOBI01 | ||
About • | Received ※ 23 July 2023 — Revised ※ 03 August 2023 — Accepted ※ 14 August 2023 — Issue date ※ 11 October 2023 | ||
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MOBO02 | IMPACT: A Substantial Upgrade to the HIPA Infrastructure at PSI | target, proton, operation, cyclotron | 34 |
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The High Intensity Proton Accelerator complex (HIPA) at the Paul Scherrer Institute (PSI), Switzerland, delivers a 590 MeV CW proton beam with currents of up to 2.4 mA (1.4 MW) to several user facilities and experimental stations. Other than the two spallation targets for thermal/cold neutrons (SINQ) and for ultracold neutrons (UCN), the beam feeds two meson production targets, Target M and Target E, serving particle physics experiments and material research via seven secondary beam lines. IMPACT (Isotope and Muon Production with Advanced Cyclotron and Target technology) aims to expand the infrastructure at HIPA in two ways: by HIMB (High-Intensity Muon Beams), increasing the surface muon rate by a factor 100, and TATTOOS (Targeted Alpha Tumour Therapy and Other Oncological Solutions), producing promising radionuclides for simultaneous diagnosis and therapy of cancer in doses sufficient for clinical studies. HIMB and TATTOOS are located close to each other. HIMB has to fit into the existing main proton beam line towards Target E and SINQ, while TATTOOS will occupy an area in a new, adjacent building using 100 µA protons split from the main beam. TATTOOS will be a perfect complement to the existing radionuclide production at 72 MeV, adding a variety of difficult to produce nuclides at a large scale. For HIMB, the current Target M will be replaced by a four-fold thicker target (Target H) consisting of a graphite wheel optimized for surface muon production. In addition, both muon beam lines are improved regarding their transmission from target to experiment. Care is taken to reduce the losses to an acceptable level in the main existing proton beam line. Installation towards the implementation of IMPACT as new user facility is foreseen from 2027. | |||
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Slides MOBO02 [6.877 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-MOBO02 | ||
About • | Received ※ 14 January 2023 — Revised ※ 17 January 2023 — Accepted ※ 30 January 2023 — Issue date ※ 10 February 2023 | ||
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MOBO04 | Experimental Study on Proton Irradiation Effect of Gallium Nitride High Electron Mobility Transistor | proton, radiation, ECR, electron | 42 |
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As a third-generation semiconductor material, gallium nitride (GaN) has the advantages of high breakdown electric field, high electron saturation speed, high operating temperature and strong radiation resistance, and has broad application prospects in the aerospace field. As an important member of GaN-based electronic devices, GaN high electron mobility transistor (HEMT) is widely considered to be used in the power supply and other important systems of spacecraft. Therefore, GaN HEMT is of great significance for spacecraft to complete relevant setting tasks. However, GaN HEMT will inevitably be affected by space radiation environment when spacecraft perform related missions. Previous researches have shown that protons are the majority of high-energy particles in space environment. Therefore, relevant studies should focus on the effect of proton irradiation on the performance of GaN HEMT. Using 100 MeV high-current proton cyclotron, we investigated the proton irradiation effect of GaN HEMT, and proved the effect of proton energy on static electrical parameters of GaN. The research work in this paper lays a foundation for the future application of GaN HEMT in space missions. | |||
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Slides MOBO04 [2.860 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-MOBO04 | ||
About • | Received ※ 15 December 2022 — Revised ※ 14 February 2023 — Accepted ※ 17 February 2023 — Issue date ※ 18 April 2023 | ||
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MOPO013 | Experimental Study of Beam Energy Control at the TIARA AVF Cyclotron | cyclotron, controls, target, extraction | 83 |
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The TIARA AVF cyclotron provides a He beam for production of At-211 as one of many beam applications. The production rate of At-211 increases with the energy of the He beam, but contamination of Po-210 produced by radioactive decay of At-210, which is generated by the energy of above 29 MeV, must be prevented for medical applications. Therefore, the energy of the He beam must be precisely measured and controlled. A time-of-flight beam energy monitor in the straight beamline from the cyclotron was installed to measure the beam energy in real time. The beam energy was arbitrarily controlled within a range of about 1% by adjusting the cyclotron magnetic field and accelerating voltage, which are the possible causes of the beam energy change. Using this control, we investigated the rate of formation of At-211 and At-210 as the beam energy was varied. As a result, we confirmed the energy generating At-210 and both production rates increased with the energy of the He beam. | |||
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Poster MOPO013 [1.010 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-MOPO013 | ||
About • | Received ※ 27 December 2022 — Revised ※ 28 January 2023 — Accepted ※ 09 February 2023 — Issue date ※ 14 March 2023 | ||
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MOPO019 | Optimization of Rapid Magnetic Field Control of the CYCIAE-230 Cyclotron Beamline Magnets | controls, proton, cyclotron, power-supply | 106 |
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The magnetic field precise and rapid control of the beamline magnets is essential to the Energy Selection System (ESS) for the proton therapy facility. During the scanning of proton beam for therapy, the field of each beamline magnet should be precisely controlled within the set time, layer upon layer. The position of beam spot to the nozzle should undoubtedly be stable and unchanged during the process. In practice, however, due to the wide energy range of proton therapy (70 MeV-230 MeV), the dynamic response of the beamline magnets usually shows nonlinear performances at a different energy, e.g., the magnetic field may cause a significant overshoot for some specific beam energy if one ignores the nonlinear effect. More challenge is that the magnetic field drops too slowly between the energy steps, which compromises the overall performance of rapid intensity modulated scanning therapy. A dynamic PID parameter optimization method is reported in this paper to address this issue. According to the transfer function of each magnet, the entire energy range is divided into several steps. Then, the experiments are carried out to find the most suitable PID parameters for each energy step. Finally, the "beam energy - excitation current-PID parameters" lookup table (LUT) is generated and stored in the beamline control system BCS for automation. During the treatment, using the LUT allows the energy setting for beamline magnets to be adjusted automatically with the most appropriate PID parameter, guaranteeing the overall performance of rapid scanning therapy. The experimental results show the overall response time of all the beamline magnets reduced from several hundred milliseconds to less than 65 ms, which meets the design requirement of less than 80ms. | |||
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Poster MOPO019 [0.364 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-MOPO019 | ||
About • | Received ※ 06 January 2023 — Revised ※ 30 January 2023 — Accepted ※ 01 February 2023 — Issue date ※ 10 February 2023 | ||
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TUBO02 | Real Time Determinations of the Range and Bragg Peak of Protons with a Depth Profile Camera at HZB | proton, cyclotron, LabView, scattering | 126 |
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The cyclotron at HZB provides a 68 MeV proton beam for therapy as well as for experiments. By using a novel camera setup, the range of the proton beam is measured optically. The setup consists of a phantom, a luminescent layer inside and a CMOS camera. By measuring the emission of the luminescent layer, the Bragg peak and the range of the proton beam can be visualized for different energies. In contrast to a water bath, the camera system offers much shorter measurement times. A dedicated LabVIEW code offers various evaluation possibilities: the Bragg curve and the lateral beam profile are generated and displayed. The system is sensitive to energy differences of less than 400 keV. The results were obtained with a beam intensity of less than 10 pA/cm2 homogenous proton beam in front of the degrader. The measurement is done in real time and provides live feedback on changes such as beam energy and beam size. The results of the camera are presented and compared to water bath measurement. | |||
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Slides TUBO02 [3.388 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-TUBO02 | ||
About • | Received ※ 29 December 2022 — Revised ※ 24 January 2023 — Accepted ※ 09 February 2023 — Issue date ※ 20 June 2023 | ||
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WEAI02 | Upgrade of the RCNP AVF Cyclotron | cyclotron, ion-source, proton, extraction | 143 |
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The upgrade program of the RCNP K140 AVF cyclotron was started in 2019 to provide not only an intense light ion beam for short-lived RI production but also a high-quality intense beam for precision experiments in nuclear physics. Most of equipment besides the main coil, pole and yoke of the cyclotron magnet was replaced by new one. Especially the RF, injection and extraction systems were fully modified to increase a beam current. A new coaxial-type resonator was designed to cover a frequency range from 16 to 36 MHz for acceleration of staple particles using acceleration harmonic mode of h=2 and h=6. The acceleration voltage of ion sources was increased from 15 kV to 50 kV to enhance the beam intensity and to reduce the beam emittance for injecting a high-quality intense ion beam into the cyclotron. The central region of the cyclotron was fully redesigned to improve beam transmission from the LEBT system. Beam commissioning was started from May 2022, and a 28 MeV 4He2+ beam was supplied to produce a short-lived RI of At-211 used for the targeted alpha-particle therapy. A 65 MeV proton beam was successfully injected into the K400 ring cyclotron to provide a 392 MeV proton beam for production of a white neutron flux and a muon beam. Several ion beams have been already used for academic research and industrial applications. | |||
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Slides WEAI02 [9.428 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-WEAI02 | ||
About • | Received ※ 16 January 2023 — Revised ※ 27 January 2023 — Accepted ※ 01 February 2023 — Issue date ※ 20 April 2023 | ||
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WEAO01 | OPAL Simulation on the Beam Transmission in the Central Region of the Medical Cyclotron COMET at Paul Scherrer Institute | cyclotron, simulation, proton, ion-source | 148 |
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The use of the medical cyclotron COMET for FLASH proton therapy requires a high beam transmission from the ion source through the central region apertures. This paper first presents a model of the COMET cyclotron featuring a rotatable ion source, a movable puller, and an adjustable first fixed slit (FFS), implemented with the OPAL framework. The electromagnetic field is individual-ly created to match each specific configuration. The beam optics parameters, especially beam position and beam size upon approaching and after passing FFS, have been studied in detail. The OPAL simulations demon-strate that an optimal configuration of the ion source, the puller and the FFS is key to achieve a high beam trans-mission. An experimental test gave a 2.8 times higher intensity within COMET cyclotron with the modifications derived on the basis of the simulations: a 0.57 mm shift of puller and a 5.6° rotation of ion source. The simula-tions indicate that, with these modifications, the beam can still be centered and accelerated to the extraction energy of 250 MeV. Next step is to investigate the influ-ence of such modifications upon the acceleration and the extraction, again with an iterative approach combining simulations and experiments. | |||
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Slides WEAO01 [5.351 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-WEAO01 | ||
About • | Received ※ 13 December 2022 — Revised ※ 09 January 2023 — Accepted ※ 01 February 2023 — Issue date ※ 11 March 2023 | ||
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WEAO04 | Status of the HZB Cyclotron | radiation, cyclotron, proton, operation | 159 |
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For more than 20 years eye tumours are treated in collaboration with the Charité - Universitätsmedizin Berlin. The close co-operation between Charité and HZB permits joint interdisciplinary research. Irradiations with either a sharp, well focused or a broad beam, either in vacuum or in air are possible with a proton beam of 68 MeV maximum energy, or a helium beam of 90 MeV. In the past few years, we concentrated on beam delivery for FLASH experiments and the related dosimetry. Artificial lenses have been irradiated under normal and FLASH conditions to investigate possible changes in the transparency. Furthermore, radiation hardness tests solar of cells for space have been performed. A modernization project has been started in order to secure a long term and sustainable operation of our accelerator complex for therapy and research. The accelerator operation for therapy as well as on-going experiments and results will be presented. | |||
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Slides WEAO04 [3.928 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-WEAO04 | ||
About • | Received ※ 30 December 2022 — Revised ※ 15 January 2023 — Accepted ※ 01 February 2023 — Issue date ※ 04 May 2023 | ||
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WEBI02 | Compact Accelerator Based Epithermal Neutron Source and Its Application for Cancer Therapy | neutron, radiation, simulation, cyclotron | 176 |
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The world’s first accelerator based epithermal neutron source for clinical boron neutron capture therapy (BNCT) was designed, developed, and commissioned between 2008 to 2010 by Sumitomo Heavy Industries in collaboration with Kyoto University at the Kyoto University Institute for Integrated Radiation and Nuclear Science. The cyclotron-based accelerator device can accelerate a proton up to an energy of roughly 30 MeV. When the proton contacts the beryllium target, fast neutrons are created that travel through a beam shaping assembly made of calcium fluoride, lead, iron, and aluminum to lower the neutron energy to the epithermal region, which is ideal for BNCT (10 keV). With a proton current of 1 mA, the system is intended to produce epithermal neutron flux of up to 1.2×109 cm-2 s−1. In 2017, the same type of accelerator was installed at the Kansai BNCT Medical Center and in March 2020 the system received medical device approval in Japan (Sumitomo Heavy Industries, NeuCure® BNCT system). Soon after, BNCT for unresectable, locally advanced, and recurrent carcinoma of the head and neck region was approved by the Japanese government for reimbursement covered by the national health insurance system. Thus far, over 100 patients have been treated using this system. | |||
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Slides WEBI02 [8.080 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-WEBI02 | ||
About • | Received ※ 27 March 2023 — Revised ※ 22 May 2023 — Accepted ※ 06 July 2023 — Issue date ※ 17 July 2023 | ||
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WEBO05 | Upgrade of a Clinical Facility to Achieve a High Transmission and Gantry Angle-Independent Flash Tune | proton, cyclotron, simulation, radiation | 191 |
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Funding: This work is supported by the SNF grant 200822 In proton therapy, FLASH-RT, irradiation at ultra-high dose rates (>40 Gy/s) that can minimize radiation-induced harm to healthy tissue without reducing its ability to treat tumors, is a topic of great interest. However, in cyclotron-based proton therapy facilities, losses caused by the energy degradation process reduce the transmission to less than 1% for low energies, making it difficult to achieve high dose rates over the clinical range (70-230 MeV). We will demonstrate how an already existing clinical beamline can be converted into a FLASH beamline by beam optic changes only. To achieve maximum transmission, we have developed a new optics that transports the undegraded 250 MeV beam from the cyclotron to the isocenter. However, this has asymmetric emittance in the transverse planes, leading to gantry angle-dependent beam characteristics at the patient. Particle transport has been simulated with MINT (in-house matrix multiplication transport program with Monte Carlo simulations for scattering effects) and benchmarked with beam profile measurements. We used the method of σ matrix matching (M. Benedikt et al. 1997) to achieve gantry angle-independent optics. MINT simulations and beam profile measurements showed a good agreement, and with FLASH optics, we experimentally achieved almost 90% transmission at the patient, translating to a maximum current of 720 nA (>9000 Gy/s). Further, we demonstrate that using the matrix matching optimization criteria together with fine-tuning of the magnets, we could achieve gantry angle-independent beam profiles at the patient location. In conclusion, we demonstrated how an already existing cyclotron-based proton gantry can be adapted to achieve ultra-high dose rates at 250 MeV, enabling investigations of FLASH radiotherapy with protons. Since most of the modifications are performed on the beam optics, it is entirely transparent to clinical operations, making the method transferable to other facilities. |
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Slides WEBO05 [5.057 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-WEBO05 | ||
About • | Received ※ 31 December 2022 — Revised ※ 10 January 2023 — Accepted ※ 01 February 2023 — Issue date ※ 10 July 2023 | ||
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WEPO012 | Upgrade of Beam Diagnostic Systems at JULIC Cyclotron | cyclotron, diagnostics, operation, controls | 231 |
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The cyclotron JULIC is used as injector for the COSY storage ring since almost 30 years. Beams of polarized and unpolarised H− and D- ions are routinely accelerated using cyclotron HF system up to 45 and 55 MeV, respectively. Meanwhile, low energy beams from JULIC become more frequently used by the experimentalists, especially at the new low energy beam line, which connects cyclotron with the large Big Karl experimental hall. To meet the requirements of the cyclotron users a diagnostic system upgrade program has been started at the JULIC cyclotron. All destructive beam diagnostic systems (Faraday Cups) have been equipped with a new produced by CAEN TetrAMM based beam diagnostic systems. All TetrAMM devices are implemented into the common COSY Control System with EPICS readout and archiving environment. The cyclotron NMR field control system has been upgraded using the newest sensor from Metrolab (PT2026), which allows operation in complete field range of the JULIC cyclotron, without changing the sensor. A new Lock In-Amplifier based Data Acquisition System has been used for nondestructive beam intensity and position diagnostic at the Big Karl beam line. First tests have demonstrated possibility to measure current and position of the 10 nA DC beam using this technique. Since relatively long time cyclotron users were occasionally disturbed by unwanted 33 Hz noise at the output of the cyclotron. Using non-contact laser vibration measurements system OMETRON S16, vibrations in this frequency range were detected on the internal elements of the HF-System. The source of these vibrations, located in the cyclotron bunker, have been identified and removed. In this contribution, the status of the JULIC cyclotron diagnostic system upgrade project will be presented. | |||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-WEPO012 | ||
About • | Received ※ 31 December 2022 — Revised ※ 18 January 2023 — Accepted ※ 01 February 2023 — Issue date ※ 14 April 2023 | ||
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THAI02 | Stripping Extraction and Lorentz Dissociation | extraction, acceleration, cyclotron, proton | 252 |
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Stripping extraction of hydrogen molecular ions has gained interest in the cyclotron industry due to its high extraction efficiency. However, the magnetic field could result in undesired dissociation of the hydrogen anion/molecular ions during acceleration. This work summarizes and compares the Lorentz dissociation of several types of hydrogen ions, as well as other important aspects that are crucial when deciding the best candidate for stripping extraction in a cyclotron. | |||
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Slides THAI02 [1.633 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-THAI02 | ||
About • | Received ※ 01 June 2023 — Revised ※ 05 July 2023 — Accepted ※ 09 July 2023 — Issue date ※ 17 July 2023 | ||
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THPO001 | COLUMBUS - A Small Cyclotron for School and Teaching Purposes | cyclotron, vacuum, acceleration, simulation | 288 |
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In the early 2012 the project "COLUMBUS a small Cyclotron for School- and Teaching Purposes" started. Supported by the FZ Jülich and some German companies a small cyclotron was built at the University of Applied Sciences of Coburg, Germany. After the first beam was detected in 2014, the cyclotron was continuously improved and expanded. At the same time, an educational concept was developed that is based on the studies and curricula in Germany. Since then, the workshops and internships, which are the two columns of the concept, have enjoyed increasing popu-larity among students and, fortunately, among female students as well. Furthermore, future improvements of the accelerator and the educational concept are presented. | |||
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Poster THPO001 [2.651 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-THPO001 | ||
About • | Received ※ 30 November 2022 — Revised ※ 11 January 2023 — Accepted ※ 31 January 2023 — Issue date ※ 01 April 2023 | ||
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THPO005 | JULIC - Driver Accelerator for HBS | neutron, cyclotron, target, controls | 303 |
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At the Forschungszentrum Jülich (FZJ) the energy variable cyclotron JULIC is used as injector of the Cooler Synchrotron (COSY) and for low to medium current irradiations of different types. At the NESP-Target station a Target-Moderator-Reflector (TMR) -demonstrator of the proposed accelerator driven High Brilliance Neutron source (HBS) was set up with the Jülich Center of Neutron Science (JCNS). Beside showing the functionality of the TMR-Design the demonstrator gives the possibility to test new target materials, different types and concepts of moderators and at least the handling of irradiated targets and components. The TMR- target station is installed inside an Experimental area offering space for complex detector and component setups for nuclear and neutron related experiments like ToF-experiments or neutron imaging e.g. But it is used for other purposes like irradiation and electronic or detector tests as well. Additionally to the TMR, the extraction beamline from JULIC to the TMR was set up and equipped with a fast kicker and a 3-field permanent magnet, as foreseen in in HBS to deliver the beam to different target stations within a sophisticated pulsing scheme, synchronized with the beam pulsing done at JULIC, using fast deflection plates. This report briefly summarizes the history of JULIC and the activities for its future perspectives. | |||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-THPO005 | ||
About • | Received ※ 07 December 2022 — Revised ※ 18 January 2023 — Accepted ※ 17 February 2023 — Issue date ※ 27 February 2023 | ||
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THPO011 | Effect of 90 MeV Proton Irradiation on Spleen Injury in C57BL/6J Mice | radiation, proton, controls, cyclotron | 324 |
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Funding: the Continuous Basic Scientific Research Project (No.WDJC-2019-11) Proton therapy has become one of the most important physiotherapies for tumors in the world, which can greatly improve the cure rate of tumors that are ineffective by conventional treatments. In addition, proton is also the main source of radiation in space environment. Therefore, it is of great scientific significance to use accelerators to carry out basic research on proton radiotherapy and space radiobiology, which can provide technical support and basic data for the optimal design of proton therapy and risk assessment of personnel in space environment. In this study, C57 mice were irradiated with 0, 0.2, 0.5 and 2 Gy by 90 MeV protons from 100 MeV cyclotron of China Institute of Atomic Energy. The mice were killed one day after irradiation. Body weight change and spleen organ coefficient were calculated. The expression of DNA damage-related protein γ H2AX was detected by western blotting. The results showed that compared with the control group, the body weight of mice in each irradiation group had no significant change, and the spleen organ coefficient decreased, indicating that the spleen atrophied after proton radiation, especially in 2 Gy. The results of Western blotting showed that the expression of γ H2AX in spleen increased significantly on the 1 day after irradiation, especially in 0.5 and 2 Gy, indicating that the spleen DNA damage was the serious on the 1 day after proton radiation. |
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Poster THPO011 [0.625 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-THPO011 | ||
About • | Received ※ 10 February 2023 — Revised ※ 13 February 2023 — Accepted ※ 18 February 2023 — Issue date ※ 27 June 2023 | ||
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THPO018 | FFAG Activity in Japan and Future Projects | target, proton, radiation, injection | 344 |
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The current activities of FFAG in Japan will be presented as well as future projects using energy recovery internal target scheme in the FFAG ring. | |||
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Poster THPO018 [2.641 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-THPO018 | ||
About • | Received ※ 18 January 2023 — Revised ※ 05 February 2023 — Accepted ※ 28 February 2023 — Issue date ※ 10 May 2023 | ||
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THPO019 | Control of a Cyclotron and an ECR Ion Source Using Bayesian Optimization Method | ion-source, brightness, LEBT, ECR | 347 |
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An enormous number of parameters are tuned during accelerator operation. The tuning is ultimately dependent on the operator’s knowledge and experience. Therefore, there is a risk that tuning time and accuracy may vary depending on the operator. This tuning difficulty is an extremely important issue when implementing accelerometers in society, such as in medical applications. In this study, we developed an automatic tuning method using Bayesian optimization, one of the machine learning technique. The aim is to realize a tuning method that can supply beams in a short time with good reproducibility and comparable to manual tuning. | |||
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Poster THPO019 [0.700 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-THPO019 | ||
About • | Received ※ 21 December 2022 — Revised ※ 29 January 2023 — Accepted ※ 09 February 2023 — Issue date ※ 12 February 2023 | ||
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FRBO03 | The Study of the Isochronous Magnetic Field and the Equilbrum Orbit of CS-30 Cyclotron | cyclotron, target, radiation, extraction | 378 |
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The CS-30 accelerator of the Institute of Nuclear Science and Technology of Sichuan University is a three-fan accelerator with constant angular width (45 degrees) at small radius and blade thickness increasing with radius at larger radius. In this paper, the magnetic field is analyzed, and the static equilibrium orbit, revolution frequency, oscillation frequencies and other data are calculated. These functions can be integrated to guide the accurate magnet numerical model setup of the existing CS-30 accelerator, which can be used in de education demonstration and experimental phenomena analysis. The optimization algorithm is innovatively introduced in the static equilibrium orbit calculation, which reduces the dependence of the results on the initial value and significantly improves the calculation speed. The calculation method presented in this paper is suitable for all cyclotrons.
*Summary of technical training for CS-30 cyclotron |
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Slides FRBO03 [2.662 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-CYCLOTRONS2022-FRBO03 | ||
About • | Received ※ 02 February 2023 — Revised ※ 03 February 2023 — Accepted ※ 09 February 2023 — Issue date ※ 21 May 2023 | ||
Cite • | reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml) | ||