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Publication
Featured researches published by Kazunari Yamada.
28th Linear Accelerator Conf. (LINAC'16), East Lansing, MI, USA, 25-30 September 2016 | 2017
Kazutaka Ozeki; Eiji Kako; Osamu Kamigaito; H. Nakai; Kazunori Okihira; Hiroki Okuno; N. Sakamoto; Katsuya Sennyu; Kenji Suda; Kensei Umemori; Yutaka Watanabe; Kazunari Yamada; Takeshi Yanagisawa
We report a general description of the cryomodule for the RIKEN superconducting quarter-wavelength resonator, the construction of which is now in progress and is aimed to be completed within this fiscal year.
13th Heavy Ion Accelerator Technology Conference (HIAT2015), Yokohama, Japan, 7-11 September 2015 | 2016
F. Suzaki; Yasushi Abe; Zhuang Ge; Kentaro Hiraishi; Yukina Ichikawa; Ikuma Kato; Hiroshi Miura; T. Moriguchi; D. Nagae; Sarah Naimi; Takuma Nishimura; Shun'ichiro Omika; A. Ozawa; S. Suzuki; Takeshi Suzuki; Natsuki Tadano; Yoshiyuki Tajiri; Yuuki Takeuchi; T. Uesaka; Masanori Wakasugi; T. Watanabe; Kazunari Yamada; Takayuki Yamaguchi; Y. Yamaguchi; Yasushige Yano; J. Zenihiro
Rare-RI Ring was constructed at RIKEN RIBF for precise isochronous mass spectrometry of unstable nuclei. In June 2015, we performed the first commissioning of the ring using 78Kr beam with the energy of 168 MeV/nucleon. We successfully carried out the individual injection which is one of the characteristics of the ring, and also we succeeded in the storage of 78Kr ions for a few seconds. We evaluated the performance of the resonant Schottky pick-up which was installed in the Rare-RI Ring. The purpose of the resonant Schottky pick-up is a monitor for tuning of the isochronous field in the ring. The resonant Schottky pick-up detected single 78Kr ions, where the frequency resolution was 1.29×10−6 (FWHM). The resolution is in the same order of the required isochronicity. The sensitivity and resolution of the resonant Schottky pick-up are sufficient for the tuning of isochronous optics.
13th Heavy Ion Accelerator Technology Conference (HIAT2015), Yokohama, Japan, 7-11 September 2015 | 2016
Takeshi Yanagisawa; Hiroshi Hara; Eiji Kako; Osamu Kamigaito; Ryuichi Matsuda; Akihiro Miyamoto; H. Nakai; Hiroki Okuno; Kazutaka Ozeki; N. Sakamoto; Katsuya Sennyu; Kenji Suda; Kensei Umemori; Yutaka Watanabe; Kazunari Yamada
MHIs activities for development of Superconducting Quarter Wave Resonator (QWR) are reported. MHI has experiences of developments and fabrications of several superconducting ellipse cavities. And now MHI is developing the superconducting QWR for heavy ion accelerators.
Proceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014) | 2015
F. Suzaki; J. Zenihiro; Y. Abe; A. Ozawa; Takeshi Suzuki; T. Uesaka; Masanori Wakasugi; Kazunari Yamada; Takayuki Yamaguchi; Y. Yamaguchi
Construction of a new storage ring called “Rare-RI Ring” was started in 2012 at RIBF. This project aims at precise isochronous mass measurements for extremely neutron-rich exotic nuclei in the r-process nucleosynthesis. To precisely tune the ion-optical condition to be isochronous, the resonant Schottky noise pick-up technique will be employed. We performed an off-line test of the resonant Schottky pick-up. Figure 1 shows the resonant Schottky pick-up that will be installed in the Rare-RI Ring. It consists of a pillbox-type resonant cavity electrically isolated from the beam pipe by a ceramic tube. A schematic view of the pick-up is shown in Fig. 2(a): a chamber shown in blue is the beam pipe and the shaded cylinder surrounding the beam pipe is the cavity equipped with two ports (yellow). The ports are movable plunger pistons that can adjust the resonance frequency (fres) of the eigenmode. Fig. 2(b) shows the cross-sectional view of the cavity, and the detailed structure of the gap can be seen at the center. The cavity itself is filled with air and has the shape of a pillbox with an outer diameter of 750 mm and length of 200 mm. The inner diameter is 320 mm. The lower flanges ( see Fig. 1 ) are prepared for feedthroughs to take out signals from a loop coil that magnetically couples to the cavity field induced by the beam. Using a network analyzer, we measured the basic quantities characterizing the resonant cavity: the resonance frequency, the shunt impedance Rsh, and the unloaded Q factor Q0. To measure Rsh, the perturbation method was adopted. From the measurements, fres = 171.54(±0.44) MHz, Rsh = 169 kΩ, and Q0 = 1884 were obtained. For tuning the isochronous field settings, the proposed pick-up is required to have an excellent singleion sensitivity. By using the results of the off-line test, the output signal power corresponding to a single ion with charge q at resonance is estimated to be P = q × 2.8 × 10−21 W , and the power of thermal noise Pnoise is 7.1 × 10−19 W. For q ≥ 16, the signal power exceeds the noise floor, and the signal from the beam can be detected by the present Schottky pickup. Therefore, the performance is sufficient for precise tuning of isochronus field settings of the Rare-RI Ring. The resonant Schottky pick-up will be soon installed into the Rare-RI Ring. Detailed results of the off-line test and online beam performance test will be reported
Physica Scripta | 2015
F. Suzaki; Y. Abe; A. Ozawa; T. Suzuki; T. Uesaka; M. Wakasugi; Kazunari Yamada; Takayuki Yamaguchi; Y. Yamaguchi; J. Zenihiro
The Rare-RI Ring project has been launched at RIKEN. The Rare-RI Ring is a storage ring specially designed for the isochronous mass spectrometry of unstable nuclei. Precise mass measurements () are necessary to reveal the r-process path and, therefore, the ion-optical conditions must be tuned to yield isochronicity of order 10−6. For this purpose, we employ a highly sensitive resonant Schottky cavity as a probe for single-ion detection. Here, we first explain this technique theoretically and derive the necessary equations. Then, based on the results of off-line tests, we determine the sensitivity of the Schottky pick-up and estimate the intensities of the signals induced inside the cavity.
5th Int. Particle Accelerator Conf. (IPAC'14), Dresden, Germany, June 15-20, 2014 | 2014
T. Watanabe; Masaki Fujimaki; Nobuhisa Fukunishi; Hiroshi Imao; Osamu Kamigaito; Masayuki Kase; Misaki Komiyama; N. Sakamoto; Kenji Suda; Masanori Wakasugi; Kazunari Yamada
Hyperfine Interactions | 2010
M. Mihara; T. Izumikawa; H. Ueno; K. Matsuta; D. Nishimura; T. Nagatomo; T. Moriguchi; Y. Ito; D. Nagae; M. Fukuda; A. Yoshimi; Kazunari Yamada; M. Takechi; Yuichi Ichikawa; S. Momota; Y. Hirayama; T. Ohtsubo; S. Suzuki; T. Kubo; Y. Namiki; A. Ozawa; Y. Ishibashi; H. Oishi; K. Suzuki; I. Hachiuma; K. Namihira; D. Horikawa; T. Minamisono; T. Yamaguchi; T. Kuboki
Hyperfine Interactions | 2010
T. Nagatomo; H. Ueno; M. Mihara; K. Matsuta; A. Yoshimi; Yuichi Ichikawa; Kazunari Yamada; H. Kawamura; A. Ozawa; T. Moriguchi; Y. Ishibashi; K. Asahi; M. Uchida; K. Suzuki; Takashi Inoue; Y. Hasama; H. Iijima; T. Sumikama; M. Fukuda; T. Minamisono
21st Int. Conf. on Cyclotrons and Their Applications (Cyclotrons'16), Zurich, Switzerland, September 11-16, 2016 | 2017
Hiroki Okuno; Tomoyuki Dantsuka; Masaki Fujimaki; Nobuhisa Fukunishi; Hiroo Hasebe; Y. Higurashi; Eiji Ikezawa; Hiroshi Imao; Osamu Kamigaito; Masanori Kidera; Misaki Komiyama; Keiko Kumagai; Takeshi Maie; Makoto Nagase; Takashi Nagatomo; Takahide Nakagawa; Makoto Nakamura; Jun-ichi Ohnishi; Kazutaka Ozeki; N. Sakamoto; Kenji Suda; Akito Uchiyama; Shu Watanabe; T. Watanabe; Yutaka Watanabe; Kazunari Yamada; Hideyuki Yamasawa
21st Int. Conf. on Cyclotrons and Their Applications (Cyclotrons'16), Zurich, Switzerland, September 11-16, 2016 | 2017
Hiroshi Imao; Nobuhisa Fukunishi; Osamu Kamigaito; Masayuki Kase; Hiroki Okuno; N. Sakamoto; Kenji Suda; Kazunari Yamada; Yasushige Yano