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Journal Articles

Compact XFEL and AMO sciences; SACLA and SCSS

Yabashi, Makina*; Tanaka, Hitoshi*; Tanaka, Takashi*; Tomizawa, Hiromitsu*; Togashi, Tadashi*; Nagasono, Mitsuru*; Ishikawa, Tetsuya*; Harries, J.; Hikosaka, Yasumasa*; Hishikawa, Akiyoshi*; et al.

Journal of Physics B; Atomic, Molecular and Optical Physics, 46(16), p.164001_1 - 164001_19, 2013/08

 Times Cited Count:71 Percentile:95.16(Optics)

Journal Articles

Vacuum system of the 3-GeV RCS in J-PARC

Ogiwara, Norio; Kinsho, Michikazu; Kamiya, Junichiro; Yamamoto, Kazami; Yoshimoto, Masahiro; Hikichi, Yusuke; Kanazawa, Kenichiro; Mio, Keigo; Takiyama, Yoichi; Suganuma, Kazuaki; et al.

Vacuum, 84(5), p.723 - 728, 2009/12

 Times Cited Count:7 Percentile:30.19(Materials Science, Multidisciplinary)

To minimize the radiation exposure during maintenance, it is necessary to compose the 3-GeV RCS vacuum system with reliable components which have long life time in such a high level of radiation. In addition, it is necessary to keep the operating pressure with beam in ultra high vacuum for suppressing the pressure instability. Thus we should think of not only the outgassing mainly due to ion desorption but also the pumping efficiency. From the above, the vacuum system was designed. The ring is divided by the isolation valves into 6 sections, which can be pumped down independently. For avoiding any eddy current loss ceramic ducts are used in the bending and focusing magnets. These ducts are connected to the Ti ducts, putting the Ti bellows between. Here, we adopt pure Ti as a material for the ducts and bellows because of its small residual radioactivity. The ring is evacuated with 20 ion pumps (0.7 m$$^{3}$$/s) and 24 turbomolecular pumps (TMPs) (1.3 m$$^{3}$$/s), which are attached to the Ti ducts. The TMPs are used for not only rough pumping but also evacuation during the beam operation. Especially a collimator system for localizing beam losses in a restricted area is evacuated with the TMPs, because the outgassing from this region will be probably the largest. On the other hand, each arc section is pumped by 4 ion pumps and 2 TMPs. To realize the above system, we have developed some components such as large aperture ceramic ducts and TMPs with high radioactive-resistance, as well as several kinds of heat treatment to reduce the outgassing. Finally, we have realized the UHV without baking in the RCS and the beam operation has been succeeded until now.

Journal Articles

Interatomic Coulombic decay following the Auger decay; Experimental evidence in rare-gas dimers

Ueda, Kiyoshi*; Fukuzawa, Hironobu*; Liu, X.*; Sakai, Katsunori*; Pr$"u$mper, G.*; Morishita, Yuichiro*; Saito, Norio*; Suzuki, Isao*; Nagaya, Kiyonobu*; Iwayama, Hiroshi*; et al.

Journal of Electron Spectroscopy and Related Phenomena, 166-167, p.3 - 10, 2008/11

 Times Cited Count:23 Percentile:72.33(Spectroscopy)

Interatomic Coulombic decay (ICD) in Ar$$_2$$, ArKr and Kr$$_2$$ following Ar 2p or Kr 3d Auger decay has been investigated by means of momentum-resolved electron-ion-ion-coincidence spectroscopy. This sequential decay leads to Coulombic dissociation into dication and monocation. Simultaneously determining the kinetic energy of the ICD electron and the kinetic energy release between the two atomic ions, we could unambiguously identify the ICD channels. We find that, in general, spin conserved ICD, in which the singlet (triplet) dicationic state produced via the atomic Auger decay preferentially decays to the singlet (triplet) state, transferring the energy to the other atom, is faster than the spin-flip ICD, in which the Auger final singlet (triplet) dicationic state decays to the triplet (singlet) state.

Journal Articles

Titanium flanged alumina ceramics vacuum duct with low impedance

Kinsho, Michikazu; Saito, Yoshio*; Kabeya, Zenzaburo*; Ogiwara, Norio

Vacuum, 81(6), p.808 - 811, 2007/02

 Times Cited Count:7 Percentile:30.11(Materials Science, Multidisciplinary)

It was success to develop alumina ceramics vacuum ducts for the 3GeV-RCS of J-PARC at JAERI. There are two types of alumina ceramics vacuum ducts needed, one being 1.5m-long duct with a circular cross section of 378 mm inner diamater for use in the quadrupole magnet, the other being 3.5m-long and bending 15 degrees, with a race-track cross section for use in the dipole magnet. These ducts could be manufactured by joining several duct segments of 0.8 m in length by brazing. The alumina ceramics ducts have copper stripes on the outside surface of the ducts to reduce the duct impedance. The radio-frequency shield is designed as a high frequency pass filter, where eddy currents cannot be generated. In this shield one end of each strope is connected to a titanium flange with a capacitor to interrupt the eddy current loop. With this, the impedance of the duct with the radio-frequency shield was reduced within an allowable desgin limit. In order to reduce emission of secondary electrons when protons or electrons strike the surface, TiN film is coated on the inside surface of the ducts.

Journal Articles

Development of alumina ceramics vacuum chamber for J-PARC

Kinsho, Michikazu; Saito, Yoshio*; Kabeya, Zenzaburo*; Ogiwara, Norio

Shinku, 49(12), p.728 - 733, 2006/12

It was success to develop alumina ceramics vacuum duct for the 3GeV-RCS of J-PARC at JAERI. This duct has titanium flanges and the exterior RF shield to reduce duct impedance. The production process of the alumina ceramics vacuum duct could be established, and mass production has been performing.

Journal Articles

Alumina ceramics vacuum duct for the 3GeV-RCS of the J-PARC

Kinsho, Michikazu; Ogiwara, Norio; Saito, Yoshio*; Kabeya, Zenzaburo*

Proceedings of 2005 Particle Accelerator Conference (PAC '05) (CD-ROM), p.2604 - 2606, 2005/00

It was success to develop alumina ceramics vacuum ducts for the 3GeV-RCS of J-PARC at JAERI. There are two types of alumina ceramics vacuum ducts needed, one being 1.5m-long duct with a circular cross section for use in the quadrupole magnet, the other being 3.5m-long and bending 15 degrees, with a race-track cross section for use in the dipole magnet. These ducts could be manufactured by joining several duct segments of 0.5-0.8 m in length by brazing. The alumina ceramics ducts have copper stripes on the outside surface of the ducts to reduce the duct impedance. In order to reduce emission of secondary electrons when protons or electrons strike the surface, TiN film is coated on the inside surface of the ducts.

Journal Articles

Roundness and straightness measurement of ceramic beam ducts for the 3GeV-synchrotron of Japan-Proton Accelerator Research Complex

Nishizawa, Daiji*; Kinsho, Michikazu; Kanazawa, Kenichiro; Ogiwara, Norio; Saito, Yoshio*; Kubo, Tomio*; Sato, Yoshihiro*

Shinku, 47(4), p.339 - 343, 2004/05

no abstracts in English

Journal Articles

Development of alumina ceramics vacuum duct for the 3GeV-RCS of the J-PARC project

Kinsho, Michikazu; Saito, Yoshio*; Kabeya, Zenzaburo*; Tajiri, Keisuke*; Nakamura, Tomaru*; Abe, Kazuhiko*; Nagayama, Taketoshi*; Nishizawa, Daiji*; Ogiwara, Norio

Vacuum, 73(2), p.187 - 193, 2004/03

 Times Cited Count:17 Percentile:54.99(Materials Science, Multidisciplinary)

Alimina ceramics vacuum duct has been developing at JAERI for the 3GeV-RCS of the J-PARC project. There are two type of the alumina ceramics vacuum ducts, one is a 1.5m-long duct with a circular cross section for use in the quadrupole magnet, the other is a 3.5m-long being bending 15 degree with an elliptical cross section for use in the dipole magnet.These ducts could be manufactured by brazed jointing several duct segments of 0.5-0.8 m long. Since some electrically conductive boundary is necessary to form on the ceramics duct in order to reduce the duct impedance, the alumina ceramics ducts have copper stripes on the outside surface of the ducts. This is called for rf shielding system. The copper stripes as rf shielding is produced by an electroforming method. In order to reduce emitting secondary electrons when primary protons or electrons impinge onto the surface, TiN film is coated inside surface of the alumina ceramics duct.

Journal Articles

Roundness and straightness measurement of ceramic beam ducts for the 3GeV-synchrotron of Japan-proton accelerator research complex

Nishizawa, Daiji*; Kinsho, Michikazu; Kanazawa, Kenichiro; Ogiwara, Norio; Saito, Yoshio*; Kubo, Tomio*; Sato, Yoshihiro*

Shinku, 47(4), p.339 - 343, 2004/02

Large aperture cylindrical beam ducts consisting of alumina ceramics will be used for the first time in the 3GeV-synchrotron of High Intensity Proton Accelerator Facility. It is necessary to evaluate roundness and straightness of ceramic ducts because we have to compensate contact area of the connected beam duct large as well as we have to compensate large enough beam aperture. We developed an apparatus of measuring roundness and straightness, and we completed data analysis method as well as measuring method. Then we are measuring and evaluating roundness and straightness of ceramic beam ducts. Now, we have newly made an ellipse ceramic duct for the 3GeV-synchrotron BM. This duct has ellipse cross-sections to satisfy with larger aperture that the beam dynamics requires. In this conference, we are going to present taken data and findings regarding form accuracy including roundness and straightness of the ellipse ceramic duct.

JAEA Reports

Absolute measurement of photon-flux using a multi-electrode ion chamber

Sano, Mutsumi*; Yoshigoe, Akitaka; Teraoka, Yuden; Saito, Norio*; Suzuki, Isao*

JAERI-Tech 2000-081, 21 Pages, 2001/02

JAERI-Tech-2000-081.pdf:0.79MB

no abstracts in English

Journal Articles

Application of the field emitter array to the vacuum measurements

Ogiwara, Norio; Suganuma, Kazuaki; Miyo, Yasuhiko; Kobayashi, Shinichi*; Saito, Yoshio*

Applied Surface Science, 146(1-4), p.234 - 238, 1999/00

 Times Cited Count:7 Percentile:42.18(Chemistry, Physical)

no abstracts in English

Journal Articles

Electron emission microscope for use in electron emission sites observations

Kobayashi, Shinichi*; *; *; Saito, Yoshio*; Ogiwara, Norio; R.V.Latham*

Applied Surface Science, 146(1-4), p.148 - 151, 1999/00

 Times Cited Count:1 Percentile:8.73(Chemistry, Physical)

no abstracts in English

JAEA Reports

None

Ikeda, Norio*; Sasaki, Nobuyuki*; Oshima, Kazuo*; Yamaguchi, Kohei*; Saito, Shigeyuki*; Abe, Yoriyuki*; Katano, Takashi*; Ueda, Akira*

JNC TJ7440 2005-071, 122 Pages, 1998/03

JNC-TJ7440-2005-071.PDF:5.9MB

no abstracts in English

Journal Articles

Retention and thermal release of oxygen implanted in boron carbide

Ogiwara, Norio; *; Saido, Masahiro; *; Saito, Yoshio*; *; *; *; *

Journal of Nuclear Materials, 220-222, p.748 - 751, 1995/00

 Times Cited Count:3 Percentile:36.75(Materials Science, Multidisciplinary)

no abstracts in English

Journal Articles

The Reaction of H$$_{2}$$O,O$$_{2}$$ and energetic O$$_{2+}$$ on boron carbide

Ogiwara, Norio; *; Saido, Masahiro; *; Saito, Yoshio*; *; *

Journal of Nuclear Materials, 212-215, p.1260 - 1265, 1994/00

 Times Cited Count:7 Percentile:56.56(Materials Science, Multidisciplinary)

no abstracts in English

Journal Articles

Oxygen gettering action of B/C materials

Ogiwara, Norio; *; Saido, Masahiro; Saito, Yoshio*; *

Shinku, 35(3), p.174 - 176, 1992/00

no abstracts in English

Oral presentation

Vacuum system of the 3 GeV-RCS in J-PARC

Ogiwara, Norio; Kinsho, Michikazu; Kamiya, Junichiro; Yamamoto, Kazami; Suganuma, Kazuaki; Yoshimoto, Masahiro; Saito, Yoshio*

no journal, , 

Oral presentation

Technology succession through assembling the dummy fuel assembly at the Irradiation Rig Assembling Facility (IRAF)

Itagaki, Wataru; Noguchi, Koichi; Endo, Norio; Nakamura, Toshiyuki; Ashida, Takashi; Saito, Takakazu; Someya, Hiroyuki*; Tomine, Hiroshi*; Kato, Jun*; Gunji, Masakatsu*

no journal, , 

no abstracts in English

Oral presentation

Emergency drills at J-PARC

Saito, Fumihiro; Kasugai, Yoshimi; Seki, Kazunari; Nakane, Yoshihiro; Tani, Norio; Sato, Koichi; Yamazaki, Hirohito*; Bessho, Kotaro; Numajiri, Masaharu

no journal, , 

no abstracts in English

19 (Records 1-19 displayed on this page)
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