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MOPTS046 |
Upgrade of the 3-MeV LINAC for Testing of Accelerator Components at J-PARC |
960 |
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- Y. Kondo, K. Hirano, T. Ito, N. Kikuzawa, R. Kitamura, T. Morishita, H. Oguri, K. Ohkoshi, S. Shinozaki, K. Shinto
JAEA/J-PARC, Tokai-mura, Japan
- Z. Fang, Y. Fukui, K. Futatsukawa, K. Ikegami, T. Miyao, K. Nanmo, M. Otani, T. Shibata
KEK, Ibaraki, Japan
- T. Hori, Y. Nemoto, Y. Sato
Nippon Advanced Technology Co., Ltd., Tokai, Japan
- T. Ishiyama, Y. Sawabe
Mitsubishi Electric System & Service Co., Ltd, Tsukuba, Japan
- Y. Ito
Total Saport System Corp., Naka-gun, Ibaraki, Japan
- Y. Kato
Total Support Systems Corporation, Tokai-mura, Naka-gun, Ibaraki, Japan
- F. Kobayashi
ULVAC Human Relations, Ltd., Kanagawa, Japan
- D. Takahashi, R. Tasaki
KIS, Ibaraki, Japan
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We are now upgrading a 3-MeV linac at J-PARC. The old 30-mA RFQ is replaced by a spare one of the J-PARC 50-mA RFQ. The ion source is same as the J-PARC linac’s, therefore, the peak beam current is upgraded from 30 mA to 50 mA. This 3-MeV linac will be used for development of various accelerator components, such as beam dyagnostics devices, laser charge exchange equipments, new MEBT buncher, and so on. In this paper, present status of this 3-MeV test linac is presented.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-MOPTS046
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About • |
paper received ※ 30 April 2019 paper accepted ※ 23 May 2019 issue date ※ 21 June 2019 |
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MOPTS048 |
Longitudinal Measurements and Beam Tuning in the J-PARC Linac MEBT1 |
968 |
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- M. Otani
J-PARC, KEK & JAEA, Ibaraki-ken, Japan
- K. Futatsukawa, T. Miyao
KEK, Ibaraki, Japan
- K. Hirano, Y. Kondo, A. Miura, H. Oguri
JAEA/J-PARC, Tokai-mura, Japan
- Y. Liu
KEK/JAEA, Ibaraki-Ken, Japan
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J-PARC linac is operated with design peak current of 50 mA from October 2018. Recently we succeeded in establishing longitudinal measurement at MEBT1, with which the beam matching is being studied in MEBT1. In this poster, recent measurements and beam tuning results in MEBT1 will be presented.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-MOPTS048
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About • |
paper received ※ 30 April 2019 paper accepted ※ 20 May 2019 issue date ※ 21 June 2019 |
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TUPTS027 |
Progress of J-PARC LINAC Commissioning |
1990 |
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- Y. Liu
KEK/JAEA, Ibaraki-Ken, Japan
- Z. Fang, K. Futatsukawa, T. Miyao, M. Otani, T. Shibata
KEK, Tokai, Ibaraki, Japan
- T. Ito, A. Miura, T. Morishita, K. Moriya, K. Okabe, J. Tamura
JAEA/J-PARC, Tokai-mura, Japan
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After energy and intensity upgrade to 400MeV and 50mA respectively, J-PARC linac were ready for 1 MW beam power from RCS. J-PARC is now successfully operated at 50mA/400MeV for 500kW at neutron target, and on the way to 1MW. The next milestones 1.2 and 1.5MW from RCS are relying on feasibility and property of increase of peak current to 60 mA and the pulse width to 600us in linac. Beam studies were carried out at linac to study the initial beam parameters from ion source/RFQ, to find the optimized lattice and matching, to clarify beam loss source and to mitigate the loss/residue dose for the power upgrade.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-TUPTS027
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About • |
paper received ※ 17 May 2019 paper accepted ※ 23 May 2019 issue date ※ 21 June 2019 |
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WEPGW033 |
Development of the Bunch Shape Monitor Using the Carbon-Nano Tube Wire |
2543 |
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- R. Kitamura, N. Hayashi, K. Hirano, Y. Kondo, K. Moriya, H. Oguri
JAEA/J-PARC, Tokai-Mura, Naka-Gun, Ibaraki-Ken, Japan
- K. Futatsukawa, T. Miyao, M. Otani
KEK, Tokai, Ibaraki, Japan
- S. Kosaka, Y. Nemoto
Nippon Advanced Technology Co., Ltd., Tokai, Japan
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A bunch shape monitor (BSM) is one of the important instruments to measure the longitudinal phase space distribution. The information of the bunch length measured by the BSM is useful to tune phases of the accelerating cavities in the linear accelerator. For example, in the J-PARC linac, three BSM’s using the tungsten wire are installed and tested at the ACS section to measure the bunch shapes between the accelerating cavities. However, this conventional BSM is hard to measure the bunch shape of H− beam with 3 MeV at the beam transport between the RFQ and DTL sections, because the wire is broken around the center region of the beam. The new BSM using the carbon-nano-tube (CNT) wire is being developed to be able to measure the bunch shape of the H− beam with 3 MeV. One challenge to introduce the CNT wire for the BSM is the measure to the discharge. The careful attention should be paid to apply the high voltage of 10 kV to the CNT wire. The several measures are taken to suppress the discharge from the wire and operate the CNT-BSM. This presentation reports the current status of the development and future prospective for the CNT-BSM.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-WEPGW033
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About • |
paper received ※ 15 May 2019 paper accepted ※ 22 May 2019 issue date ※ 21 June 2019 |
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THPRB035 |
Development of Beam Window Protection System for J-PARC Linac |
3886 |
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- H. Takahashi, S. Hatakeyama, Y. Sawabe
JAEA/J-PARC, Tokai-mura, Japan
- T. Ishiyama, T. Suzuki
Mitsubishi Electric System & Service Co., Ltd, Tsukuba, Japan
- T. Miyao
KEK, Ibaraki, Japan
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In J-PARC Linac, beam study (including beam conditioning) is mainly performed using beam dump. A beam window is installed in the beam line to each beam dump. It is considered that the parameters of acceptable beam to able to be injected the beam window are the 50 mA current, the 100 micro-sec width and the 2.5 Hz repetition. On the other hand, at beam study of Linac, the beam with higher power than these parameters are not used. Therefore, the beam study was started and performed only after the operator checked that the beam parameters are within the acceptable values. However, at the beam study of 2018, a beam windows of 0-degree dump was cracked because the beam that exceeds acceptable parameters was injected due to human error. Then, beam study using 0-degree dump was impossible at all. And, in order not to cause such accident again, we began to develop the beam window protection system. Moreover, as soon as possible, implementation of the system was required. Therefore, we designed and developed this system by improving it based on the particle management system which can measure all 25 Hz beam. We have developed a beam window protection system that monitors the beam current for each shot and accumulated beam current for a prescribed time and inhibits the beam by MPS when either value exceeds the threshold. Moreover, we succeeded in developing and implementing this system in a short time. This paper is described about development and function test of beam window protection system.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-THPRB035
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About • |
paper received ※ 30 April 2019 paper accepted ※ 22 May 2019 issue date ※ 21 June 2019 |
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