Author: "T. Ido" / Language: undetermined - Searchworks@Jio Institute Digital Library Search Results

226 results on '"T. Ido"'

1. Design Considerations for the Implementation of a High-Field-Side Transient CHI System on QUEST

Author: R. Raman, K. Kuroda, K. Hanada, M. Ono, M. Hasegawa, T. Onchi, R. Ikezoe, H. Idei, T. Ido, and J. A. Rogers
Subjects: Nuclear and High Energy Physics, Condensed Matter Physics
Published: 2022
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2. Improvements to the High-Field-Side Transient CHI System on QUEST

Author: K. Kuroda, R. Raman, M. Hasegawa, T. Onchi, K. Hanada, M. Ono, B. A. Nelson, J. Rogers, R. Ikezoe, H. Idei, T. Ido, O. Mitarai, M. Nagata, S. Kawasaki, T. Nagata, A. Higashijima, S. Shimabukuro, I. Niiya, I. Sekiya, S. Kojima, K. Nakamura, Y. Takase, and S. Murakami
Subjects: Nuclear and High Energy Physics, Nuclear Energy and Engineering
Published: 2022
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3. Portable THz Frequency Standard using Difference-Frequency Generation of Acetylene-Stabilized Telecom Diode Lasers

Author: S. Nagano, M. Kumagai, and T. Ido
Published: 2022
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4. 8.56-GHz quasi-optical launcher system with incident-mode selectivity on the QUEST spherical tokamak

Author: H. Idei, M. Sakaguchi, K. Mishra, T. Onchi, R. Ikezoe, O. Watanabe, Y. Tanaka, T. Saito, T. Ido, and K. Hanada
Subjects: Nuclear Energy and Engineering, Mechanical Engineering, General Materials Science, Civil and Structural Engineering
Published: 2023
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5. Development of a heavy ion beam probe diagnostic for HL-2A tokamak

Author: H.R. Fan, L.T. Gao, A.D. Liu, G. Zhuang, T. Ido, M. Xu, J.C. Huang, J. Zhang, C.Q. Feng, C. Zhou, H. Liu, L. Nie, Y.X. Liu, B.Z. Fu, J.Q. Li, and W.D. Liu
Subjects: Instrumentation, Mathematical Physics
Abstract: A heavy ion beam probe (HIBP) is being developed and tested on the HL-2A tokamak. To focus on the turbulence measurement in high beta scenarios with the toroidal magnetic field of 1.35 T, a 500 kV thallium beam is chosen and optimized. The locations of the injection and detection system are determined based on the probing beam trajectory calculations. The status of the accelerator, sweep system, analyzer, and control system is described. Four pairs of sweep plates are positioned in both primary and secondary beamlines to actively control the beam trajectory, where the poloidal sweepers require a maximum of 15 kV voltages to be applied. A parallel-plate energy analyzer with multi-slits is supplied by 100 kV high voltage for the electric potential measurement. The signal intensity is also evaluated to be hundreds of nA levels, 5 × 107 V/A amplifiers are therefore designed. Software is also developed to include the data acquisition as well as the control and monitoring of HIBP subsystems.
Published: 2023
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6. Conceptual design of a heavy ion beam probe for the QUEST spherical tokamak

Author: T. Ido, M. Hasegawa, R. Ikezoe, T. Onchi, K. Hanada, H. Idei, K. Kuroda, and Y. Nagashima
Subjects: Instrumentation
Abstract: A heavy ion beam probe (HIBP) has been designed for the QUEST spherical tokamak to measure plasma turbulence and the profiles of electric potential profiles. Using a cesium ion beam with an energy of several 10 keV, the observable region covers most of the upper half of the plasma. Although the probe beam is deflected by the poloidal magnetic field produced by plasma current and poloidal coil currents, it can be detected under plasma current up to 150 kA by modifying the trajectories with two electrostatic sweepers. According to the numerical estimation of the intensity of the detected beam, sufficient signal intensity for measuring plasma turbulence can be obtained over almost the measurable area when the electron density is up to 1 × 1019 m−3, which is larger than the cut-off density of electron cyclotron heating in QUEST. The performance of the designed HIBP is sufficient to explore the mechanisms of heat and particle transport in magnetically confined plasmas, including the influence of plasma wall interactions, which is a goal of the QUEST project.
Published: 2022
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7. Adaptive Capon beamforming for lensless electron cyclotron emission imaging with high spatial resolution

Author: H. Idei, M. Fukuyama, S. Sakai, K. Mishra, K. Nishimura, R. Ikezoe, T. Onchi, T. Ido, and K. Hanada
Subjects: Diagnostic Imaging, Electrons, Cyclotrons, Instrumentation, Ultrasonography
Abstract: Electron cyclotron emission (ECE) imaging diagnostics incorporating a lensless approach have been developed for measurements involving active spatial selectivity and direction-of-arrival estimation. The Capon method for adaptive-array analysis was proposed to improve the spatial resolution of the two-dimensional ECE imaging technique. Broadband noise source emissions were used to simulate the ECE to verify the practical effectiveness of the Capon method in the ECE imaging. Multiple noise source emission positions were properly estimated with a high spatial resolution using the Capon method.
Published: 2022
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8. Behavior of geodesic acoustic mode and limit-cycle oscillation approaching L-H transition in JFT-2M tokamak

Author: T Kobayashi, M Sasaki, T Ido, K Kamiya, Y Miura, K Ida, and K Itoh
Subjects: Nuclear Energy and Engineering, turbulence, limit-cycle oscillation, geodesic acoustic mode, Condensed Matter Physics, L-H transition
Abstract: In this paper, a phenomenology of competing behavior between the geodesic acoustic mode (GAM) and the limit-cycle oscillation (LCO) is presented. Before the LCO occurs, the GAM can grow to the observable amplitude via the turbulent Reynolds stress force. Approaching the L-H transition, the LCO is excited and the GAM decays. In the LCO phase, the GAM driving force is possibly suppressed by the nonlocal turbulence amplitude modulation by the LCO.
Published: 2022
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9. Measurement of the Frequency Ratio of 115In+ ion Clock and 87Sr Optical Lattice Clock

Author: T. Ido, Nozomi Ohtsubo, Ying Li, K. Hayasaka, H. Hachisu, Nils Nemitz, and K. Matsubara
Subjects: Physics, symbols.namesake, Optical lattice, Zeeman effect, Orders of magnitude (time), Quadrupole, Clock rate, symbols, Hydrogen maser, Atomic physics, Frequency standard, Hyperfine structure
Abstract: The indium ion is one of the original candidates in the first proposal for single-ion clocks with systematic uncertainties at the 10-18 level [1]. In+ has an alkaline-earth-like electron configuration, with a 1S0 - 3P0 clock transition frequency that has a low sensitivity to magnetic fields. It has the highest clock frequency of all presently investigated optical clocks [2]. Such high transition energies give it a very small sensitivity to blackbody radiation (BBR), which causes problematic frequency shifts in most other clocks, including optical lattice clocks. Direct state detection and laser cooling on the 1S0 - 3P1 transition are a further advantage for an 115In+ clock. The electric quadrupole moments of the two clock states are orders of magnitude smaller than those for the 2S1/2 - 2D5/2 quadrupole transitions of alkaline-like ions (Ca+, Sr+, Yb+). This makes the transition frequency insensitive to the electric field gradients imposed by adjacent ions. With direct readout available, In+ is thus ideal for a multi-ion clock, which can overcome the inherent stability limitations of a single-ion system. Despite the appeal of the 115In+ ion for a high-performance optical clock, its adoption has been hampered by concerns about technical reliability. Only two groups previously measured the clock transition frequency with fractional uncertainties approaching 1e-14, reported 2000[3] and 2007[4]. In 2017, we measured the clock frequency with an uncertainty of 5e-15 [5], which prompted an update of the frequency value recommended by the International Committee for Weights and Measures (CIPM). This initial frequency determination was performed by averaging 36 measurements of the magnetically unresolved spectrum, and was limited by the systematic uncertainty of the first order Zeeman shift as well as the statistical uncertainty. We recently improved our In+ clock by direct laser stabilization to the clock transition and controlled magnetic field application to resolve Zeeman sublevels [6]. In this presentation, we report on the first frequency ratio measurement of an 115In+ single ion clock and a 87Sr optical lattice clock. The measurement employs two independent Er-doped fiber frequency combs which reference a common hydrogen maser that serves as a flywheel oscillator. From 89 000 s of measurement time, the frequency ratio is determined to be 2.952 748 749 874 863 3(23) with 7.7e-16 relative uncertainty. If we adopt the CIPM recommended value for the 87Sr clock frequency, we find 1 267 402 452 901 040.0(1.1) Hz for the absolute In+ clock frequency [7]. [1] H. G. Dehmelt, “Monoion oscillator as potential ultimate laser frequency standard,” IEEE Transactions on Instrumentation Meas. pp. 83–87 (1982). [2] F. Riehle, P. Gill, F. Arias, and L. Robertsson, “The CIPM list of recommended frequency standard values: guidelines and procedures,” Metrologia. 55, 188–200 (2018). [3] J. von Zanthier, T. Becker, M. Eichenseer, A. Y. Nevsky, C. Schwedes, E. Peik, H. Walther, R. Holzwarth, J. Reichert, T. Udem, T. W. Hansch, P. V. Pokasov, M. N. Skvortsov, and S. N. Bagayev, Opt. Lett. 25, 1729 (2000). [4] Y. Wang, R. Dumke, T. Liu, A. Stejskal, Y. Zhao, J. Zhang, Z. Lu, L. Wang, T. Becker, and H. Walther, Opt. Commun. 273, 526 (2007). [5] N. Ohtsubo, Y. Li, K. Matsubara, T. Ido, and K. Hayasaka, Opt. Express 25, 11725 (2017). [6] N. Ohtsubo, Y. Li, N. Nemitz, H. Hachisu, K. Matsubara, T. Ido, and K. Hayasaka, Hyperfine Interact. 240, 39 (2019). [7] N. Ohtsubo, Y. Li, N. Nemitz, H. Hachisu, K. Matsubara, T. Ido, and K. Hayasaka, Optics Letters, accepted
Published: 2021
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10. Risk profiles and one-year outcomes of patients with newly diagnosed atrial fibrillation in India: Insights from the GARFIELD-AF Registry

Author: Jitendra PS. Sawhney, Veerappa A. Kothiwale, Vikas Bisne, Rajashekhar Durgaprasad, Praveen Jadhav, Manoj Chopda, Velam Vanajakshamma, Ramdhan Meena, Govindan Vijayaraghavan, Kamaldeep Chawla, Jagan Allu, Karen S. Pieper, A. John Camm, Ajay K. Kakkar, Jean-Pierre Bassand, David A. Fitzmaurice, Samuel Z. Goldhaber, Shinya Goto, Sylvia Haas, Werner Hacke, Lorenzo G. Mantovani, Frank Misselwitz, Alexander G.G. Turpie, Martin van Eickels, Freek W.A. Verheugt, Gloria Kayani, Keith A.A. Fox, Bernard J. Gersh, Hector Lucas Luciardi, Harry Gibbs, Marianne Brodmann, Frank Cools, Antonio Carlos Pereira Barretto, Stuart J. Connolly, Alex Spyropoulos, John Eikelboom, Ramon Corbalan, Dayi Hu, Petr Jansky, Jørn Dalsgaard Nielsen, Hany Ragy, Pekka Raatikainen, Jean-Yves Le Heuzey, Harald Darius, Matyas Keltai, Sanjay Kakkar, Jitendra Pal Singh Sawhney, Giancarlo Agnelli, Giuseppe Ambrosio, Yukihiro Koretsune, Carlos Jerjes Sánchez Díaz, Hugo Ten Cate, Dan Atar, Janina Stepinska, Elizaveta Panchenko, Toon Wei Lim, Barry Jacobson, Seil Oh, Xavier Viñolas, Marten Rosenqvist, Jan Steffel, Pantep Angchaisuksiri, Ali Oto, Alex Parkhomenko, Wael Al Mahmeed, David Fitzmaurice, D.Y. Hu, K.N. Chen, Y.S. Zhao, H.Q. Zhang, J.Z. Chen, S.P. Cao, D.W. Wang, Y.J. Yang, W.H. Li, Y.H. Yin, G.Z. Tao, P. Yang, Y.M. Chen, S.H. He, Ying Wang, Yong Wang, G.S. Fu, X. Li, T.G. Wu, X.S. Cheng, X.W. Yan, R.P. Zhao, M.S. Chen, L.G. Xiong, P. Chen, Y. Jiao, Y. Guo, L. Xue, F.Z. Wang, H. Li, Z.M. Yang, C.L. Bai, J. Chen, J.Y. Chen, X. Chen, S. Feng, Q.H. Fu, X.J. Gao, W.N. Guo, R.H. He, X.A. He, X.S. Hu, X.F. Huang, B. Li, J. Li, L. Li, Y.H. Li, T.T. Liu, W.L. Liu, Y.Y. Liu, Z.C. Lu, X.L. Luo, T.Y. Ma, J.Q. Peng, X. Sheng, X.J. Shi, Y.H. Sun, G. Tian, K. Wang, L. Wang, R.N. Wu, Q. Xie, R.Y. Xu, J.S. Yang, L.L. Yang, Q. Yang, Y. Ye, H.Y. Yu, J.H. Yu, T. Yu, H. Zhai, Q. Zhan, G.S. Zhang, Q. Zhang, R. Zhang, Y. Zhang, W.Y. Zheng, B. Zhou, Z.H. Zhou, X.Y. Zhu, S. Kakkar, J.P.S. Sawhney, P. Jadhav, R. Durgaprasad, A.G. Ravi Shankar, R.K. Rajput, K. Bhargava, R. Sarma, A. Srinivas, D. Roy, U.M. Nagamalesh, M. Chopda, R. Kishore, G. Kulkarni, P. Chandwani, R.A. Pothiwala, M. Padinhare Purayil, S. Shah, K. Chawla, V.A. Kothiwale, B. Raghuraman, G. Vijayaraghavan, V.M. Vijan, G. Bantwal, V. Bisne, A. Khan, J.B. Gupta, S. Kumar, D. Jain, S. Abraham, D. Adak, A. Barai, H. Begum, P. Bhattacharjee, M. Dargude, D. Davies, B. Deshpande, P. Dhakrao, V. Dhyani, S. Duhan, M. Earath, A. Ganatra, S. Giradkar, V. Jain, R. Karthikeyan, L. Kasala, S. Kaur, S. Krishnappa, A. Lawande, B. Lokesh, N. Madarkar, R. Meena, P. More, D. Naik, K. Prashanth, M. Rao, N.M. Rao, N. Sadhu, D. Shah, M. Sharma, P. Shiva, S. Singhal, S. Suresh, V. Vanajakshamma, S.G. Panse, Y. Koretsune, S. Kanamori, K. Yamamoto, K. Kumagai, Y. Katsuda, K. Sadamatsu, F. Toyota, Y. Mizuno, I. Misumi, H. Noguchi, S. Ando, T. Suetsugu, M. Minamoto, Hiroshi Oda, K. Shiraishi, S. Adachi, K. Chiba, H. Norita, M. Tsuruta, T. Koyanagi, H. Ando, T. Higashi, K. Okada, S. Azakami, S. Komaki, K. Kumeda, T. Murayama, J. Matsumura, Y. Oba, R. Sonoda, K. Goto, K. Minoda, Y. Haraguchi, H. Suefuji, H. Miyagi, H. Kato, Tadashi Nakamura, Tsugihiro Nakamura, H. Nandate, R. Zaitsu, Yoshihisa Fujiura, A. Yoshimura, H. Numata, J. Ogawa, H. Tatematsu, Y. Kamogawa, K. Murakami, Y. Wakasa, M. Yamasawa, H. Maekawa, S. Abe, H. Kihara, S. Tsunoda, Katsumi Saito, Kazuyuki Saito, T. Fudo, K. Obunai, H. Tachibana, I. Oba, T. Kuwahata, S. Higa, M. Gushiken, T. Eto, H. Yoshida, D. Ikeda, Yoshitake Fujiura, M. Ishizawa, M. Nakatsuka, K. Murata, C. Ogurusu, M. Shimoyama, M. Akutsu, I. Takamura, F. Hoshino, N. Yokota, T. Iwao, K. Tsuchida, M. Takeuchi, Y. Hatori, Y. Kitami, Yoichi Nakamura, R. Oyama, M. Ageta, Hiroyuki Oda, Y. Go, K. Mishima, T. Unoki, S. Morii, Yuhei Shiga, H. Sumi, T. Nagatomo, K. Sanno, K. Fujisawa, Y. Atsuchi, T. Nagoshi, T. Seto, T. Tabuchi, M. Kameko, K. Nii, K. Oshiro, H. Takezawa, S. Nagano, N. Miyamoto, M. Iwaki, Yuichiro Nakamura, M. Fujii, M. Okawa, Masahiko Abe, Masatake Abe, Mitsunori Abe, T. Saito, T. Mito, K. Nagao, J. Minami, T. Mita, I. Sakuma, T. Taguchi, S. Marusaki, H. Doi, M. Tanaka, T. Fujito, M. Matsuta, T. Kusumoto, S. Kakinoki, K. Ashida, N. Yoshizawa, J. Agata, O. Arasaki, M. Manita, M. Ikemura, S. Fukuoka, H. Murakami, S. Matsukawa, Y. Hata, T. Taniguchi, T. Ko, H. Kubo, M. Imamaki, M. Akiyama, M. Inagaki, H. Odakura, T. Ueda, Y. Katsube, A. Nakata, H. Watanabe, M. Techigawara, M. Igarashi, K. Taga, T. Kimura, S. Tomimoto, M. Shibuya, M. Nakano, K. Ito, T. Seo, S. Hiramitsu, H. Hosokawa, M. Hoshiai, M. Hibino, K. Miyagawa, Hajime Horie, N. Sugishita, Yukio Shiga, A. Soma, K. Neya, Tetsuro Yoshida, Tomoki Yoshida, M. Mizuguchi, M. Ishiguro, T. Minagawa, M. Wada, H. Mukawa, F. Okuda, S. Nagasaka, Y. Abe, Sen Adachi, Susumu Adachi, T. Adachi, K. Akahane, T. Amano, K. Aoki, T. Aoyama, H. Arai, S. Arima, T. Arino, H. Asano, T. Asano, J. Azuma, T. Baba, T. Betsuyaku, H. Chibana, H. Date, J. Doiuchi, Y. Emura, M. Endo, Y. Fujii, R. Fujiki, A. Fujisawa, Y. Fujisawa, T. Fukuda, T. Fukui, N. Furukawa, T. Furukawa, W. Furumoto, T. Goto, M. Hamaoka, N. Hanazono, K. Hasegawa, T. Hatsuno, Y. Hayashi, K. Higuchi, K. Hirasawa, H. Hirayama, M. Hirose, S. Hirota, M. Honda, Hideki Horie, T. Ido, O. Iiji, H. Ikeda, K. Ikeda, K. Ikeoka, M. Imaizumi, H. Inaba, T. Inoue, F. Iseki, A. Ishihara, N. Ishioka, N. Ito, T. Iwase, H. Kakuda, J. Kamata, H. Kanai, H. Kanda, M. Kaneko, H. Kano, T. Kasai, T. Kato, Y. Kato, Y. Kawada, K. Kawai, K. Kawakami, S. Kawakami, T. Kawamoto, S. Kawano, J. Kim, T. Kira, H. Kitazawa, H. Kitazumi, T. Kito, T. Kobayashi, T. Koeda, J. Kojima, H. Komatsu, I. Komatsu, Y. Koshibu, T. Kotani, T. Kozuka, Y. Kumai, T. Kumazaki, I. Maeda, K. Maeda, Y. Maruyama, S. Matsui, K. Matsushita, Y. Matsuura, K. Mineoi, H. Mitsuhashi, N. Miura, S. Miyaguchi, S. Miyajima, H. Miyamoto, A. Miyashita, S. Miyata, I. Mizuguchi, A. Mizuno, T. Mori, O. Moriai, K. Morishita, O. Murai, Sho Nagai, Shunichi Nagai, E. Nagata, H. Nagata, A. Nakagomi, S. Nakahara, M. Nakamura, R. Nakamura, N. Nakanishi, T. Nakayama, R. Nakazato, T. Nanke, J. Nariyama, Y. Niijima, H. Niinuma, Y. Nishida, Y. Nishihata, K. Nishino, H. Nishioka, K. Nishizawa, I. Niwa, K. Nomura, S. Nomura, M. Nozoe, T. Ogawa, N. Ohara, M. Okada, K. Okamoto, H. Okita, M. Okuyama, H. Ono, T. Ono, Y. Onuki Pearce, S. Oriso, A. Ota, E. Otaki, Y. Saito, H. Sakai, N. Sakamoto, Y. Sakamoto, Y. Samejima, Y. Sasagawa, H. Sasaguri, A. Sasaki, T. Sasaki, Kazuki Sato, Kiyoharu Sato, M. Sawano, S. Seki, Y. Sekine, Y. Seta, K. Sezaki, N. Shibata, Y. Shiina, H. Shimono, Y. Shimoyama, T. Shindo, H. Shinohara, R. Shinohe, T. Shinozuka, T. Shirai, T. Shiraiwa, Y. Shozawa, T. Suga, C. Sugimoto, Kazuo Suzuki, Keita Suzuki, Shu Suzuki, Shunji Suzuki, Susumu Suzuki, Y. Suzuki, M. Tada, A. Taguchi, T. Takagi, Y. Takagi, K. Takahashi, S. Takahashi, H. Takai, C. Takanaka, S. Take, H. Takeda, K. Takei, K. Takenaka, T. Tana, G. Tanabe, K. Taya, H. Teragawa, S. Tohyo, S. Toru, Y. Tsuchiya, T. Tsuji, K. Tsuzaki, H. Uchiyama, O. Ueda, Y. Ueyama, N. Wakaki, T. Wakiyama, T. Washizuka, M. Watanabe, T. Yamada, T. Yamagishi, H. Yamaguchi, Kenichi Yamamoto, Kentaro Yamamoto, Kunihiko Yamamoto, T. Yamamoto, M. Yamaura, M. Yamazoe, K. Yasui, Y. Yokoyama, K. Yoshida, T.W. Lim, C.K. Ching, C.G. Foo, J.H. Chow, D.D. Chen, F.R. Jaufeerally, Y.M. Lee, G. Lim, W.T. Lim, S. Thng, S.Y. Yap, C. Yeo, S. Oh, H.N. Pak, J.-B. Kim, J.H. Kim, S.-W. Jang, D.H. Kim, D.R. Ryu, S.W. Park, D.-K. Kim, D.J. Choi, Y.S. Oh, M.-C. Cho, S.-H. Kim, H.-K. Jeon, D.-G. Shin, J.S. Park, H.K. Park, S.-J. Han, J.H. Sung, J.-G. Cho, G.-B. Nam, Y.K. On, H.E. Lim, J.J. Kwak, T.-J. Cha, T.J. Hong, S.H. Park, J.H. Yoon, N.-H. Kim, K.-S. Kim, B.C. Jung, G.-S. Hwang, C.-J. Kim, D.B. Kim, J.J. Ahn, H.J. An, H. Bae, A.L. Baek, W.J. Chi, E.A. Choi, E.H. Choi, H.K. Choi, H.S. Choi, S. Han, E.S. Heo, K.O. Her, S.W. Hwang, E.M. Jang, H.-S. Jang, S. Jang, H.-G. Jeon, S.R. Jeon, Y.R. Jeon, H.K. Jeong, I.-A. Jung, Hyeon Jeong Kim, Hyun Ju Kim, Ji Seon Kim, Jung Sook Kim, J.A. Kim, K.T. Kim, M.S. Kim, Sang Hee Kim, Sang Hyun Kim, Y.-I. Kim, C.S. Lee, E.H. Lee, G.H. Lee, H.Y. Lee, H.-Y. Lee, K.H. Lee, K.R. Lee, M.S. Lee, M.-Y. Lee, R.W. Lee, S.E. Lee, S.H. Lee, S. Lee, W.Y. Lee, I.K. Noh, A.R. Park, B.R. Park, H.N. Park, J.H. Park, M. Park, Y. Park, S.-Y. Seo, J. Shim, J.H. Sim, Y.M. Sohn, W.S. Son, Y.S. Son, H.J. Song, H.K. Wi, J.J. Woo, S. Ye, K.H. Yim, K.M. Yoo, E.J. Yoon, S.Y. Yun, P. Angchaisuksiri, S. Chawanadelert, P. Mongkolwongroj, K. Kanokphatcharakun, S. Cheewatanakornkul, T. Laksomya, S. Pattanaprichakul, T. Chantrarat, S. Rungaramsin, S. Silaruks, W. Wongcharoen, K. Siriwattana, K. Likittanasombat, P. Katekangplu, W. Boonyapisit, D. Cholsaringkarl, B. Chatlaong, P. Chattranukulchai, Y. Santanakorn, P. Hutayanon, P. Khunrong, T. Bunyapipat, S. Jai-Aue, P. Kaewsuwanna, P. Bamungpong, S. Gunaparn, S. Hongsuppinyo, R. Inphontan, R. Khattaroek, K. Khunkong, U. Kitmapawanont, C. Kongsin, B. Naratreekoon, S. Ninwaranon, J. Phangyota, A. Phrommintikul, P. Phunpinyosak, K. Pongmorakot, S. Poomiphol, N. Pornnimitthum, S. Pumprueg, S. Ratchasikaew, K. Sanit, K. Sawanyawisuth, B. Silaruks, R. Sirichai, A. Sriwichian, W. Suebjaksing, P. Sukklad, T. Suttana, A. Tangsirira, O. Thangpet, W. Tiyanon, Y. Vorasettakarnkij, T. Wisaratapong, W. Wongtheptien, A. Wutthimanop, S. Yawila, A. Oto, A. Altun, I. Ozdogru, K. Ozdemir, O. Yilmaz, A. Aydinlar, M.B. Yilmaz, E. Yeter, Z. Ongen, M. Cayli, H. Pekdemir, M. Ozdemir, M. Sucu, T. Sayin, M. Demir, H. Yorgun, M. Ersanli, E. Okuyan, D. Aras, H. Abdelrahman, O. Aktas, D. Alpay, F. Aras, M.F. Bireciklioglu, S. Budeyri, M. Buyukpapuc, S. Caliskan, M. Esen, M.A. Felekoglu, D. Genc, B. Ikitimur, E.B. Karaayvaz, S. Kılıç Karataş, S. Okutucu, E. Ozcelik, A. Quisi, H. Sag, L. Sahiner, B.Y. Sayin, T. Seker, D. Uzun Alkan, E. Yildirim, R. Yildirim, F. Yilmaz, V. Yuksekdag, H.L. Luciardi, N. Vensentini, A.C. Ingaramo, G.A. Sambadaro, V. Fernandez Caputi, S.G. Berman, P. Dragotto, A.J. Kleiban, N. Centurion, G. Giacomi, R.A. Ahuad Guerrero, D. Conde, G. Zapata, L.A. Di Paola, J.L. Ramos, R.D. Dran, J. Egido, A.A. Fernandez, M.J. Fosco, S. Sassone, V.A. Sinisi, L.R. Cartasegna, M.A. Berli, O.A. Gomez Vilamajo, F. Ferroni, E.D. Alaguibe, A. Alvarez D'Amelio, C. Arabetti, L. Arias, J.A. Belardi, L. Bergesio, F. Berli, M. Berli, S. Borchowiec, C. Buzzetti, R. Cabrini, V. Campisi, A.L. Cappi, R. Carrizo, F. Colombo Berra, J.P. Costabel, O.J.A. Costamagna, A.A. Damonte, I.N. De Urquiza, F. Diez, M.F. 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Y., Angchaisuksiri, P., Chawanadelert, S., Mongkolwongroj, P., Kanokphatcharakun, K., Cheewatanakornkul, S., Laksomya, T., Pattanaprichakul, S., Chantrarat, T., Rungaramsin, S., Silaruks, S., Wongcharoen, W., Siriwattana, K., Likittanasombat, K., Katekangplu, P., Boonyapisit, W., Cholsaringkarl, D., Chatlaong, B., Chattranukulchai, P., Santanakorn, Y., Hutayanon, P., Khunrong, P., Bunyapipat, T., Jai-Aue, S., Kaewsuwanna, P., Bamungpong, P., Gunaparn, S., Hongsuppinyo, S., Inphontan, R., Khattaroek, R., Khunkong, K., Kitmapawanont, U., Kongsin, C., Naratreekoon, B., Ninwaranon, S., Phangyota, J., Phrommintikul, A., Phunpinyosak, P., Pongmorakot, K., Poomiphol, S., Pornnimitthum, N., Pumprueg, S., Ratchasikaew, S., Sanit, K., Sawanyawisuth, K., Silaruks, B., Sirichai, R., Sriwichian, A., Suebjaksing, W., Sukklad, P., Suttana, T., Tangsirira, A., Thangpet, O., Tiyanon, W., Vorasettakarnkij, Y., Wisaratapong, T., Wongtheptien, W., Wutthimanop, A., Yawila, S., Oto, A., Altun, A., Ozdogru, I., Ozdemir, K., Yilmaz, O., Aydinlar, A., Yilmaz, M. 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A., Bergesio, L., Berli, F., Berli, M., Borchowiec, S., Buzzetti, C., Cabrini, R., Campisi, V., Cappi, A. L., Carrizo, R., Colombo Berra, F., Costabel, J. P., Costamagna, O. J. A., Damonte, A. A., De Urquiza, I. N., Diez, F., Edén, M. F., Fanuele, M., Fernandez Voena, F., Foa Torres, M., Funosas, C., Giacomi, M. P., Gimenez, C. H., Gurfinkel, E. P., de L. M. Had, M., Hansen, V., Hrabar, A. D., Ingratta, M., Lopez, A., Maehara, G., Maffei, L., Martinelli, A., Martinelli, C., Matkovich, J., Mautner, B., Meirino, A., Munguia, R., Navarro, A., Novas, V., Perez Prados, G., Pontoriero, J., Potito, R. N., Ricotti, C., Rodriguez, M. A., Rolandi, F., Said Palladino, M. E., Salinger, M., Sanziani, L. S., Schygiel, P. O., Sossich, A., Tinto, J. F., Tonelli, L., Tufare, A. L., Vallejo, M., Yunis, M. E., Zillo, M., Zurbrigk, F. J., Barretto, A. C. P., Sobral Filho, D. C., Jaber, J., Armaganijan, D., Faria Neto, J., Steffens, A., Kunz Sebba Barroso de Souza, W., de Souza Neto, J. D., Ribeiro, J. M., Silveira Teixeira, M., Ferreira Rossi, P. R., Pires, L., Moreira, D., Moura Jorge, J. C., Menezes Lorga Filho, A., Bodanese, L. C., Westerlund Montera, M., Del Carlo, C. H., Da Rocha Rodrigues, T., Alves da Costa, F. A., Lopes, A., Lopes, R., Araújo, G. R., Fernandes Manenti, E. R., Kerr Saraiva, J. F., Ferreira Braga, J. C., Negri, A., Souto, L., Moncada, C., Bertolim Precoma, D., Roquette, F., Reis, G., Ramos Filho, R. A., Lanna Figueiredo, E., Vieira Botelho, R., Munhoz da Fontoura Tavares, C., Costantini Frack, C. R., Abdalla Saad, J., Finimundi, H. C., Pisani, C., Chemello, D., Pereira Martins, M., Broilo França, C. C., Alban, F., Aranha Rosito, G. B., de Moura Xavier Moraes Junior, J. B., Tumelero, R. T., Nigro Maia, L., Simões de Almeida, R., do Carmo Borges, N. C., Gomes Ferreira, L. G., Agliardi, P., Alves de Oliveira Gomes, J., Araujo, V., Arruda Nakazone, M., Barbosa, T., Barroso, S., Belisario Falchetto, E., Bellotti Lopes, H., Benez Teixeira Lemos, M. A., Biazus, G., Borges Queiroz, L., Camazzola, F. E., Caporale, M., Cardoso Boscato, S., Chieza, F., Chokr, M. O., Clemente Mingireanov, R., Codonho Góes, N., Correa, C., Costa, M., Costantini Ortiz, C., da Silva, L. S., da Silva Paulitsch, F., da Silveira, J. A., Daros, E., de Araújo, G. R., Del Monaco, M. I., Dias, C., Dias, M. A., Drummond Wainstein, A. P., Ely Pizzato, P., Esteves, D. C., Fabri, P., Félix Lorenzato Fonseca, T., Fernandes, E., Fonseca, C., Frack Costantini, C. R., Franchin Ferraz, R., Freire, F., Gottardo, P., Guanaes, D., Guizzardi, S., Hettwer Magedanz, E., Igansi, F., Jannuzzi, F., Junior, G., Komar, D., Lino, E. G., Lopes, D., Lourenço da Silva Júnior, O., Lustosa, E., Macagnan, A. P., Marinho, M. C., Mazzoni, M., Melo, G., Mortari, L., Mouco, O. M. C. C., Nanzer Vital, C., Ormundo, C., Oss Emmer, S., Palmegiani, E., Pavani, R., Pereira, L., Pereira, V. L., Perreira, R., Poletti, S., Quaia Fortunato, S. C., Queirantes, C., Ramos Pereira, N., Rech, R. L., Ribeiro, S., Rodrigues, A., Roesch, H., Ruaro Reichert, T., Santos, D., Santos, I., Santos, M., Seroqui, M. V., Silva, S., Soares, L., Spolaor, L., Stoll, C., Toazza Duda, N., Trama, L., Unterkircher, B., Valois, M. V., Vargas, T., Viana, T., Vicente, C., Vidal Armaganijan, L., Vieira Homem, R., Vieira Torres, L. G., Vila Boas, L., Villaça Guimarães Filho, F., Corbalan, R., Eggers, G., Bugueño Gutiérrez, C., Arriagada, G., Potthoff Cardenas, S., Stockins Fernandez, B. A. J., Conejeros, C., Houzvic, C., Marin Cuevas, P., Montecinos, H., Forero, A., Lanas, F., Larico Gómez, M., Charme Vilches, G., Rey, C., Astudillo, C., Aguilar, J., Campisto, Y., Lara, C., Molina, E., Munoz Oyarzon, J., Olguin, V., Vergara, M., Villan, C., Sánchez Díaz, C. J., Illescas Diaz, J., Leal Cantú, R., Ramos Zavala, M. G., Cabrera Jardines, R., Espinola Zavaleta, N., Villarreal Umaña, S., López Rosas, E., Llamas Esperón, G., Pozas, G., Cardona Muñoz, E., Matadamas Hernández, N., Leyva Rendón, A., García Hernández, N., de los Ríos Ibarra, M., Virgen Carrillo, L., López Villezca, D., Hernández Herrera, C., López Prieto, J. J., Gaona Rodríguez, R., Villeda Espinosa, E., Flores Martínez, D., Velasco Barcena, J., Yong, R., Rodríguez Briones, I., Leiva Pons, J. L., Álvarez López, H., Olvera Ruiz, R., Díaz de la Vega, C., Cantú Brito, C., Chuquiure Valenzuela, E., Reyes-Sanchez, R., Bazzoni Ruiz, A., Nandayapa Flores, O., Benavides Gonzalez, M., Arriaga Nava, R., Morales Cerda, J. D., Fierro Fierro, O., Fajardo Campos, P., Alfaro, T. A. A., Altamirano Bellorin, S., Avena, R., Chavarria, M., Espinosa, I., Flores Silva, F., Garcia Nava, R. H., Godoy, K., Gonzalez Felix, E. J., Gonzalez Garcia, C. L., Gonzalez Salas, L. G., Guajardo, P., Hernandez Gonzalez, S., Izquierdo, T., Mancilla Ortiz, M. C., Martinez Vasquez, D., Mendoza, N., Morales, J., Nikitina, N., Ochoa Aybar, S., Ortiz, A., Padilla Macias, P., Perez, F., Perez Sanchez, J. A., Piña Toledano, S., Ramos Gonzalez, M., Rivera Ramos, C., Roa Castro, V., Romero Cardona, G., Ruiz Cornejo, M., Salinas, A., Santana, G., Sida Perez, P., Tovar Castaneda, A. C., Trujillo Cortes, R., Brodmann, M., Lenz, K., Drexel, H., Foechterle, J., Hagn, C., Podczeck-Schweighofer, A., Huber, K., Winkler, M., Schneeweiß, B., Gegenhuber, A., Lang, W., Eichinger-Hasenauer, S., Kaserer, P., Sykora, J., Rasch, H., Pichler, M., Schaflinger, E., Strohmer, B., Breier, R., Ebner, K. -M., Eischer, L., Freihoff, F., Lischka-Lindner, A., Mark, T., Mirtl, A., Said, A., Stöcklöcker, C., Vogel, B., Vonbank, A., Wöhrer, C., Zanolin, D., Cools, F., Paparella, G., Vandergoten, P., Parqué, J. -L., Capiau, L., Vervoort, G., Wollaert, B., Desfontaines, P., Mairesse, G., Boussy, T., Godart, P., De Wolf, A., Voet, J., Heyse, A., Hollanders, G., Anné, W., Vercammen, J., Purnode, P., Blankoff, I., Faes, D., Balthazar, Y., Beutels, M., Maréchal, P., Verstraete, S., Xhaet, O., Striekwold, H., Thoeng, J., Hermans, K., Alzand, B., Ascoop, A. -K., Banaeian, F., Barbuto, A. -M., Billiaux, A. C., Blockmans, M., Bouvy, C., Brike, C., Capiau, H., Casier, T., Conde Y Bolado, A., De Cleen, D., De Coninck, M., de Vos, M., de Weerdt, N., Delforge, M., Delvigne, M., Denie, D., Derycker, K., Deweerd, E., Dormal, F., Drieghe, S., Everaert, M., Eykerman, T., Feys, E., Ghekiere, M., Gits, F., Hellemans, S., Helvasto, L., Jacobs, C., Lips, S., Mestdagh, I., Nimmegeers, J., Piamonte, V., Pollet, P., Postolache, A., Raepers, M., Raymenants, E., Richa, J., Rombouts, H., Salembier, J., Scheurwegs, C., Semeraro, O., Simons, N., Smessaert, C., Smolders, W., Stockman, I., Tahon, S., Thyssen, V., Tincani, G., Van Durme, F., Van Lier, D., Vandekerckhove, H., Vandekerckhove, Y., Vandenbroeck, D., Vandorpe, A., Vanhalst, E., Vanhauwaert, B., Vantomme, C., Vergauwen, L., Verloove, H., Vydt, T., Weyn, T., Jansky, P., Reichert, P., Spacek, R., Machova, V., Zidkova, E., Ludka, O., Olsr, J., Kotik, L., Plocova, K., Racz, B., Ferkl, R., Hubac, J., Kotik, I., Monhart, Z., Burianova, H., Jerabek, O., Pisova, J., Petrova, I., Dedek, V., Honkova, M., Podrazil, P., Spinar, J., Vitovec, J., Novak, M., Lastuvka, J., Durdil, V., Antonova, P., Bockova, L., Bultas, J., Chlumsky, J., Dastychova, L., Drasnar, T., Honek, J., Horejsi, M., Hubacova, V., Janska, L., Kopeckova, I., Kratochvilova, R., Krcova, E., Labrova, R., Lindourkova, A., Lipoldova, J., Lubanda, H., Ludkova, A., Mahdalikova, L., Majerníkova, M., Michalik, D., Potuznik, P., Prochazkova, E., Sulc, A., Sveceny, J., Valtova, M., Zidek, M., Zika, J., Nielsen, J., Nielsen, H., Husted, S., Hintze, U., Rasmussen, S., Bremmelgaard, A., Markenvard, J., Boerger, J., Solgaard, J., Simonsen, P., Loekkegaard, T., Bruun, M., Mertz, J., Domínguez, H., Skagen, K., Egstrup, K., Ibsen, H., Raymond, I., Bang-Hansen, T., Ellervik, C., Eriksen, E., Jensen, L., Jensen, M., Leth, M., Nygaard, A., Park, J., Schou, M., Therkelsen, A., Tilma, J., Vesterager, K., Raatikainen, P., Airaksinen, J., Arola, O., Koistinen, J., Nappila, H., Peltomäki, K., Rasanen, V., Vasankari, T., Le Heuzey, J. -Y., Galinier, M., Gottwalles, Y., Paganelli, F., Loiselet, P., Muller, J. -J., Koujan, M. B., Marquand, A., Destrac, S., Piot, O., Delarche, N., Cebron, J. -P., Boveda, S., Guenoun, M., Guedj-Meynier, D., Galley, D., Ohayon, J., Assouline, S., Zuber, M., Amarenco, P., Ellie, E., Kadouch, J., Fournier, P. -Y., Huberman, J. -P., Lemaire, M., Rodier, G., Milandre, L., Vandamme, X., Sibon, I., Neau, J. -P., Mahagne, M. H., Mielot, A., Bonnefoy, M., Churet, J. -B., Navarre, V., Sellem, F., Monniot, G., Boyes, J. -P., Doucet, B., Martelet, M., Obadia, D., Crousillat, B., Mouallem, J., Bearez, E., Nazeyrollas, P., Brugnaux, J. P., Fedorowsky, A., Casassus, F., Berneau, J. -B., Chemin, F., Falvo, N., Perron, J. -M., Poulard, J. -E., Barreau, A., Beltra, C., Corrihons, E., Decarsin, N., Dubois, B., Ducasse, E., Giry, X., Kemmel, A., Ledure, S., Lemaire, N., Robin, F., Rosolin, N., Sanchez, D., Suissa, A., Darius, H., Königer, G., Purr, J., Gerbaulet, U., Kellner, B. -T., Kopf, A., Schäfer, T., Zauzig, H., Riegel, P., Hohensee, H., Eißfeller, E., Eder, W., Rehling, G., Glatzel, D., Zutz, S., Heinz, G. -U., Menke, H., Pustelnik, A., Sandow, P., Ludwig, N., Wiswedel, H., Wildenauer, W., Axthelm, C., Schwarz, T., Babyesiza, A., Stuchlik, G., Zimny, H. -H., Kropp, M., Kahl, F., Caspar, A., Omankowsky, S., Läßig, T., Hartmann, H. -J., Lehmann, G., Bindig, H. -W., Hergdt, G., Reimer, D., Hauk, J., Dorsch, W., Dshabrailov, J., Michel, H., Rapp, K. -A., Vormann, R., Mayer, P., Horstmeier, U., Eissing, V., Hey, H., Leuchtgens, H., Lilienweiß, V., Kolitsch, K., Schubert, C., Lauer, H., Buchner, T., Brauer, G., Kamin, S., Müller, K., Abdel-Qader, M., Baumbach, S., Ebert, H. -H., Schwencke, C., Schellong, S., Bernhardt, P., Karolyi, L., Sievers, B., Haverkamp, W., Salbach, P., Röhnisch, J. -U., Schoen, S., Erdle, W., Mueller, T., Mueller, H., Mitrovic, V., Babjakova, Z., Bergner, K., Boehme, S., Bonin, K., Buckert, D., Busch, F., Dichristin, U., Diez, S., Fleck, A., Flint, K., Floegel, H., Fritz, C., Frommhold, R., Gehre, J., Geyer, J., Grytzmann, A., Hahn, M., Helgert, K., Hubert, K., Kirchner-Volker, K., Klein, V., Kroll, D., Krueger, A., Lehmann, R., Mann, L., Maselli, A., Menken, G., Mikes, K., Mortan, H., Nasser, N., Nicolaus, D., Plauskat, A., Pomper, L., Quietzsch, A., Ravenhorst, C., Reichelt, C., Reimer, C., Schaefer, B., Scharrer, S., Schirmer, K., Schmidt, K., Schoene, R., Schulze, J., Schuppe, M., Simon, S., Sommer, S., Spranger, K., Talkenberger, A., Tauber, K., Tetlak, A., Toennishoff, T., Voelkel-Babyesiza, R., Voigts, B., Weiser, U., Wesendorf, S., Wildenauer, S., Wolf, T., Wurziger, J., Zak, J., Zauzig, H. -D., Ziefle, S., Zincke, S., Keltai, M., Vangel, S., Szalai, G., Merkely, B., Kancz, S., Boda, Z., Nagy, A., Laszlo, Z., Matoltsy, A., Gaszner, B., Polgar, P., Habon, T., Noori, E., Juhasz, G., Kanakaridisz, N., Szentpeteri, I., Juhasz, F., Vertes, A., Papp, A., May, Z., Ferenczi, J., Egyutt, M., Kis, E., Engelthaler, G., Szantai, G., Fulop, E., Gombos, P., Gulyas, D., Jen, P., Kiralyhazine Gyorke, E., Kovacs, M., Kovacsne Levang, S., Marianna, S., Radics, Z., Sydó, N., Szalo, R., Szilagyi, A., Sztanyik, F., Vandrus, B., Agnelli, G., Ambrosio, G., Tiraferri, E., Santoro, R., Testa, S., Di Minno, G., Moia, M., Caimi, T. M., Martini, G., Tessitori, M., Cappelli, R., Poli, D., Quintavalla, R., Melone, F., Cosmi, F., Pizzini, A., Piseddu, G., Fanelli, R., Latella, C., Santi, R., Pancaldi, L., De Cristofaro, R., Palareti, G., De Blasio, A., Salerno Uriarte, J., Minetti, F., Pogliani, E. M., Lonati, L. M., Accogli, M., Ciampani, N., Malengo, S., Feola, M., Raisaro, A., Fattore, L., Grilli, P., Germini, F., Settimi, M., Alunni, M., Duranti, G., Tedeschi, L., Baglioni, G., Avanzino, G., Berardi, M., Pannacci, V., Giombolini, A., Nicoli, S., Scarponi, T., Allasia, B., Ricciarini, P., Nasorri, R., Argena, A., Bossolasco, P., Ronchini, P., Filippi, A., Tradati, F., Bulla, C., Donzelli, L., Foppa, L., Bottarelli, M. L., Tomasello, A., Mauric, A., Femiano, C., Reggio, R., Lillo, F., Mariani, A., Forcignanò, F., Volpe, M., D'Avino, M., Bongiorni, M. G., Severi, S., Capucci, A., Lodigiani, C., Salomone, E., Serviddio, G., Tondo, C., Golino, P., Mazzone, C., Iacopino, S., Pengo, V., Galvani, M., Moretti, L., Ambrosino, P., Banfi, E., Biagioli, V., Bianchi, A., Boggian, G., Breschi, M., Brusorio, S., Calcagnoli, F., Campagna, G., Carpenedo, M., Ciabatta, C., Ciliberti, G., Cimmino, G., D'Arienzo, C., Di Gennaro, L., Fedele, M., Ferrini, P. M., Granzow, K., Guazzaloca, G., Guerra, F., Lo Buglio, A., Longo, S., Macellari, F., Mesolella, E., Mollica Poeta, E., Occhilupo, P., Oriana, V., Rangel, G., Salomone, L., Scaccianoce, A., Scarone, C., Segreti, L., Sottilota, G., Villani, R., Zecca, C., ten Cate, H., Ruiter, J. H., Klomps, H., Bongaerts, M., Pieterse, M. G. C., Guldener, C., Herrman, J. -P., Lochorn, G., Lucassen, A., Adriaansen, H., The, S. H. K., Nierop, P. R., Hoogslag, P. A. M., Hermans, W., Groenemeijer, B. E., Terpstra, W., Buiks, C., Boersma, L. V. 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Subjects: Registrie, Male, Time Factors, Anticoagulant therapy, Arrhythmia, Atrial fibrillation, GARFIELD-AF, 030204 cardiovascular system & hematology, Electrocardiography, 0302 clinical medicine, Risk Factors, Anticoagulant therapy, Arrhythmia, Atrial fibrillation, GARFIELD-AF, Aged, Atrial Fibrillation, Female, Follow-Up Studies, Humans, Incidence, India, Prevalence, Prognosis, Prospective Studies, Survival Rate, Thromboembolism, Registries, Risk Assessment, Medicine, 030212 general & internal medicine, Prospective cohort study, Incidence (epidemiology), cardiovascular system, medicine.symptom, Cardiology and Cardiovascular Medicine, Risk assessment, Human, medicine.medical_specialty, Time Factor, RD1-811, Prognosi, Follow-Up Studie, 03 medical and health sciences, Internal medicine, Diseases of the circulatory (Cardiovascular) system, cardiovascular diseases, Risk factor, Survival rate, Fibrillation, business.industry, Risk Factor, ta3121, medicine.disease, Clinical trial, Prospective Studie, RC666-701, Surgery, Clinical and Preventive Cardiology, business
Abstract: Background: The Global Anticoagulant Registry in the FIELD–Atrial Fibrillation (GARFIELD-AF) is an ongoing prospective noninterventional registry, which is providing important information on the baseline characteristics, treatment patterns, and 1-year outcomes in patients with newly diagnosed non-valvular atrial fibrillation (NVAF). This report describes data from Indian patients recruited in this registry. Methods and results: A total of 52,014 patients with newly diagnosed AF were enrolled globally; of these, 1388 patients were recruited from 26 sites within India (2012–2016). In India, the mean age was 65.8 years at diagnosis of NVAF. Hypertension was the most prevalent risk factor for AF, present in 68.5% of patients from India and in 76.3% of patients globally (P
Published: 2018
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11. Conceptual design of a heavy ion beam probe diagnostic for HL-2M tokamak

Author: Lin Nie, Wandong Liu, Jiquan Li, L.J. Cai, H.R. Fan, Zhe Liu, Chu Zhou, J.X. Li, A. D. Liu, Min Xu, Ge Zhuang, L.T. Gao, and T. Ido
Subjects: Electron density, Tokamak, Materials science, Mechanical Engineering, Attenuation, Plasma, Magnetic field, law.invention, Nuclear Energy and Engineering, law, Ionization, General Materials Science, Atomic physics, Beam (structure), Civil and Structural Engineering, Voltage
Abstract: The conceptual design of a heavy ion beam probe (HIBP) for HL-2M tokamak has been proposed to measure the plasma potential, electron density and their fluctuations to contribute to the understanding of advanced confinement modes and transport. Beam trajectory calculations are performed under 3D magnetic field and engineering conditions of the facility. By choosing the positions and angles of both primary and secondary beamlines, a wide region of observation area ( 0.1 r / a 0.9 ) is achieved with 2 MeV Tl + beam injection. The active trajectory control technique is used to obtain the poloidal sweep angle between − 10 ∘ and 10 ∘ . Then, the applied voltages of sweep plates are evaluated to be up to 25 kV. By integrating ionization and attenuation along beam paths, the detected signal level distribution in the plasma density condition n 0 = 5 × 10 19 m − 3 is higher than 100 nA with 100 μ A injection beam intensity in most of the plasma region, which ensures an acceptable signal-to-noise ratio for measurements.
Published: 2021
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12. On the Origin of Steep and Localized Radial Electric Field in the Transport Barrier at Plasma Edge

Author: T. Kobayashi, T. Tokuzawa, S.-I. Itoh, Naohiro Kasuya, Shigeru Inagaki, T. Ido, Kensaku Kamiya, and Kimitaka Itoh
Subjects: Physics, Toroid, Tokamak, Turbulence, Dielectric, Plasma, Condensed Matter Physics, Curvature, 01 natural sciences, 010305 fluids & plasmas, Computational physics, law.invention, Nuclear magnetic resonance, Physics::Plasma Physics, law, Electric field, 0103 physical sciences, 010306 general physics, Bifurcation
Abstract: Theories to understand the steep and localized radial electric field in the edge of toroidal plasma, which appears in conjunction with H-mode, is revisited based on the electric field bifurcation model. Key elements in the models of the L-H transition (including the toroidal effects on the dielectric constant and the effects of the curvature of radial electric field on turbulence suppression) are assessed. Results are applied to tokamak and helical plasmas, for which data with high-resolution have been obtained recently. The status of quantitative tests on various mechanisms through comparison with experimental observations is also addressed. (© 2016 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)
Published: 2016
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13. Onset Condition of the Subcritical Geodesic Acoustic Mode Instability in the Presence of Energetic-Particle-Driven Geodesic Acoustic Mode

Author: K. Itoh, S.-I. Itoh, Y. Kosuga, M. Lesur, and T. Ido
Published: 2016
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14. RESEARCH-ARTILE Agricultural performance and genetic parameters for yield-related traits of sugar- and energy cane families derived from planned crosses

Author: A R Fernandes, Júnior, A A C, de Azeredo, R A, de Oliveira, J C Bespalhok, Filho, O T, Ido, E, Daros, and B P, Brasileiro
Subjects: Dietary Fiber, Plant Breeding, Sucrose, Polymorphism, Genetic, Quantitative Trait, Heritable, Hybridization, Genetic, Saccharum, Selective Breeding
Abstract: The forecast of a growing energy demand in the coming years has aroused particular interest in biomass for energy cogeneration, to diversify the energy matrix by using clean and renewable sources. To meet the new demands of the sugarcane industry, this study evaluated the agronomic performance and estimated genetic parameters for yield traits in sugar- and energy cane families derived from planned crosses. The cane families were assessed in the northwest of the State of Paraná, county of Paranavaí, in a randomized complete block design, with three replications. The evaluations were carried out 12 months after the first cut, in the ratoon cane cycle, in December 2014, under very unfavorable conditions for the crop, due to the low fertility and water-holding capacity of the soil. Besides, the crop was evaluated at the end of the harvest, when the agricultural and industrial quality of the crop is reduced. The following traits were evaluated at the plot level: soluble solids content, apparent sucrose content (PC), fiber content, tons of cane per hectare, tons of sucrose per hectare (TSH), and tons of fiber per hectare (TFH). High genetic variability was observed for all evaluated traits, with accuracy estimates from 0.69 (TSH) to 0.92 (PC), and high heritability (up to 0.84), indicating the possibility of genetic progress. The sugarcane families derived from crosses of Saccharum spontaneum and Saccharum robustum species with sugarcane hybrids had the highest fiber contents. Highest sugar contents were found in sugarcane families resulting from crosses of sugarcane clones and conventional cultivars. The TSH means were highest in the families F160 x MEX68-200 and RB855156 x RB987935. The highest genotypic mean for TFH was observed in the special polycross involving cultivar RB036066 with S. spontaneum accessions as pollen donors.
Published: 2017

15. P5826Lectin-like oxidized LDL receptor-1 (LOX-1) in cardiomyocytes (CMs) is involved in the pathogenesis of doxorubicin (DOX)-induced cardiomyopathy

Author: T. Ido, Tatsuya Sawamura, Akemi Kakino, Toshiki Tanaka, Takuma Aoyama, T. Shiraki, C. Yokoyama, and Shinya Minatoguchi
Subjects: medicine.medical_specialty, business.industry, Cardiomyopathy, medicine.disease, Pathogenesis, Internal medicine, Cardiology, Cancer research, Medicine, Doxorubicin, Cardiology and Cardiovascular Medicine, business, Receptor, Oxidized ldl, medicine.drug
Published: 2017
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16. MHD Modes Destabilized by Energetic Ions on LHD

Author: Kunihiro Ogawa, Katsumi Ida, T. Tokuzawa, Akihiro Shimizu, K. Toi, Satoshi Yamamoto, Satoru Sakakibara, Satoshi Ohdachi, S. Morita, Donald A. Spong, K. Nagaoka, A. Weller, F. Watanabe, Yasushi Todo, M. Isobe, Masaki Osakabe, T. Ido, K. A. Tanaka, K. Narihara, T. Ito, Noriyoshi Nakajima, and Masaki Nishiura
Subjects: Physics, Nuclear and High Energy Physics, 020209 energy, Mechanical Engineering, 02 engineering and technology, 01 natural sciences, 010305 fluids & plasmas, Ion, Nuclear Energy and Engineering, Physics::Plasma Physics, Physics::Space Physics, 0103 physical sciences, 0202 electrical engineering, electronic engineering, information engineering, Particle, General Materials Science, Magnetohydrodynamic drive, Magnetohydrodynamics, Atomic physics, Civil and Structural Engineering
Abstract: Energetic ion-driven magnetohydrodynamic instabilities such as Alfven eigenmodes (AEs), energetic particle modes (EPMs), and their impacts on energetic ion confinement are being studied on the Larg...
Published: 2010
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17. Overview of LHD Plasma Diagnostics

Author: Tsuyoshi Akiyama, Ryuichi Sakamoto, Hisamichi Funaba, Clive Michael, Mitsutaka Isobe, T. Tokuzawa, Akihiro Shimizu, Atsushi Mase, Leonid Vyacheslavov, Y. Nagayama, M. Emoto, K. A. Tanaka, S. Morita, Shigeru Inagaki, Motoshi Goto, Naoki Tamura, Masaki Osakabe, Satoru Sakakibara, Suguru Masuzaki, Kuninori Sato, T. Ido, Satoshi Ohdachi, Mamoru Shoji, Katsumi Ida, Shigeru Sudo, K. Toi, Shigeki Okajima, Sadatsugu Muto, E. V. Veshchev, Tomohiro Morisaki, Mamiko Sasao, Kazuo Kawahata, Y. Nakamura, K. Narihara, Masaki Nishiura, B.J. Peterson, Ichihiro Yamada, Mikiro Yoshinuma, Hideya Nakanishi, Y. Hamada, Andrei Sanin, and N. Ashikawa
Subjects: Physics, Superconductivity, Quantitative Biology::Biomolecules, Nuclear and High Energy Physics, business.industry, 020209 energy, Mechanical Engineering, Physics::Medical Physics, 02 engineering and technology, Diagnostic system, 01 natural sciences, 010305 fluids & plasmas, Large Helical Device, Data acquisition, Optics, Nuclear Energy and Engineering, Condensed Matter::Superconductivity, 0103 physical sciences, 0202 electrical engineering, electronic engineering, information engineering, General Materials Science, Plasma diagnostics, Atomic physics, business, Axial symmetry, Civil and Structural Engineering
Abstract: The Large Helical Device (LHD) is the world’s largest heliotron-type device with l = 2, m = 10 continuous superconducting helical coils and three pairs of superconducting poloidal coils. The major ...
Published: 2010
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18. Contribution of the Large Helical Device Plasmas to Alfvén Eigenmode Physics in Toroidal Plasmas

Author: Satoru Sakakibara, K. Nagaoka, Katsumi Ida, Satoshi Ohdachi, T. Ito, Masaki Osakabe, K. Narihara, T. Ido, Kunihiro Ogawa, F. Watanabe, K. A. Tanaka, T. Tokuzawa, Akihiro Shimizu, K. Toi, S. Morita, Masaki Nishiura, and Mitsutaka Isobe
Subjects: Physics, Large Helical Device, Toroid, Physics::Plasma Physics, Normal mode, Beta (plasma physics), Physics::Space Physics, Magnetic pressure, Plasma, Atomic physics, Condensed Matter Physics, Beam (structure), Ion
Abstract: In the large helical device (LHD) having three dimensional configuration, Alfven eigenmodes (AEs) destabilized by energetic ions are widely investigated using neutral beam heated plasmas with monotonic and non-monotonic rotational transform (ι/2π) profiles. In a plasma with monotonic ι/2π-profile, core-localized toroidicity-induced Alfven eigenmode (TAE) as well as global one are often observed. With the increase in the averaged toroidal beta value, defined as the ratio of total plasma pressure to toroidal magnetic pressure, core-localized TAE with low toroidal mode number becomes global. In a relatively high beta plasma with monotonic ι/2π-profile, two TAEs with different toroidal mode number often interact nonlinearly and generate another modes through three wave coupling. In a plasma with non-monotonic ι/2π-profile generated by intense counter neutral beam current drive, reversed shear Alfven eigenmode (RSAE) and geodesic acoustic mode (GAM) excited by energetic ions were observed for the first time in a helical plasma. Nonlinear coupling was also observed between RSAE and GAM.
Published: 2009
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19. In search of zonal flows by using direct density fluctuation measurements

Author: Yuichi Takase, Sanae I. Itoh, Kimitaka Itoh, Katsumichi Hoshino, T. Ido, Akihide Fujisawa, Masatoshi Yagi, Y.M. Miura, Akira Ejiri, K. Uehara, Yoshihiko Nagashima, and Kouji Shinohara
Subjects: Physics, Tokamak, Geodesic, business.industry, Turbulence, Mode (statistics), Zonal flow (plasma), Plasma, Condensed Matter Physics, Computational physics, law.invention, Core (optical fiber), Optics, Nuclear Energy and Engineering, Physics::Plasma Physics, law, Physics::Space Physics, business, Envelope (waves)
Abstract: A method for zonal flow study by using direct density fluctuation measurements is proposed. When ambient drift-wave turbulence is modulated by zonal flows (i.e. in the drift-wave-zonal flow systems), an envelope of the ambient density fluctuations has spectral peaks around zonal flow frequencies. A spectral peak at the geodesic acoustic mode (GAM) frequency is observed in the envelope of the ambient density fluctuations measured in edge plasma of the JFT-2M tokamak. The significant cross-bicoherence is also found between the ambient density fluctuations and its envelope in the GAM frequency. This result demonstrates that we can measure the GAM only by using density fluctuation data. This method provides a possibility of zonal flow research in burning core plasma by density fluctuation diagnostics such as microwave reflectometry.
Published: 2007
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20. Intermittent characteristics in coupling between turbulence and zonal flows

Author: Y. Yoshimura, K. Matsuoka, Sanae I. Itoh, Shinichi Ohshima, K. Nagaoka, H. Nakano, C. Takahashi, Kimitaka Itoh, T. Minami, Chihiro Suzuki, Tsuyoshi Akiyama, S. Okamura, Patrick Diamond, M. Isobe, T. Ido, Yoshihiko Nagashima, Akihiro Shimizu, S. Nishimura, Mamoru Kojima, Akihide Fujisawa, and H. Iguchi
Subjects: Physics, Coupling, Toroid, Scale (ratio), Turbulence, Mechanics, Plasma, Condensed Matter Physics, Physics::Fluid Dynamics, Wavelet, Classical mechanics, Nuclear Energy and Engineering, Physics::Plasma Physics, Electric field, Physics::Space Physics, Bicoherence
Abstract: An extended application of Gabour's wavelet to bicoherence analysis succeeds in resolving the instantaneous structure of three wave couplings between disparate scale electric field fluctuations in the high temperature core in a toroidal plasma device named the compact helical system. The obtained results quantify an intermittent linkage between turbulence and zonal flows—a highlighted issue in the present plasma research. This is the first demonstration that the intermittent nature of the three wave coupling should underlie the turbulence power modulation due to zonal flows.
Published: 2007
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21. Optical clock and ultracold collisions with trapped strontium atoms

Author: T. Ido, T. Zelevinsky, M.M. Boyd, Seth M. Foreman, Sebastian Blatt, Jun Ye, and A.D. Ludlow
Subjects: Physics, Nuclear and High Energy Physics, Optical lattice, Magnetic moment, Scattering length, Condensed Matter Physics, Atomic and Molecular Physics, and Optics, Magnetic field, Metastability, Physics::Atomic Physics, Physical and Theoretical Chemistry, Atomic physics, Spectral resolution, Ground state, Spectroscopy
Abstract: With microkelvin neutral strontium atoms confined in an optical lattice, we have achieved a fractional resolution of better than 5 x 10−15 on the1 S o −3 P o doubly forbidden 87Sr clock transition at 698 nm. Measurements of the clock line shifts as a function of experimental parameters indicate that the fractional uncertainties due to systematic shifts could be reduced below 10−15. The ultrahigh spectral resolution permitted resolving the nuclear spin states of the clock transition at small magnetic fields, leading to measurements of the 3 P o magnetic moment and metastable lifetime. In addition, photoassociation spectroscopy was performed on the narrow 1 S o −3 P 1 transition of 88Sr, revealing the least-bound state, and showing promise for efficient optical tuning of the ground state scattering length and production of cold molecules.
Published: 2007
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22. Compatibility of reduced activation ferritic steel wall with high performance plasma on JFT-2M

Author: K Tsuzuki, K Kamiya, K Shinohara, M Bakhtiari, H Ogawa, G Kurita, M Takechi, S Kasai, M Sato, H Kawashima, K Uehara, K Hoshino, Y Kusama, M Yamamoto, T Shibata, K Kikuchi, H Amemiya, Y Sadamoto, Y Nagashima, A Ejiri, T Hino, Y Hirohata, H Tsutsui, R Shimada, T Ido, Y Hamada, and the JFT-2M Group
Subjects: Nuclear and High Energy Physics, Fusion, Resistive touchscreen, Materials science, Ferromagnetism, Limiter, Growth rate, Plasma, Condensed Matter Physics, Molecular physics, Instability, Magnetic field
Abstract: In JFT-2M, the applicability of reduced activation ferritic steel to a fusion demonstration reactor has been demonstrated mainly concerning the ferromagnetic effect on plasma production, control, stability and confinement. The compatibility of the close ferritic wall with high-normalized beta plasmas has been investigated mainly because the demonstration reactor will utilize the wall stabilization effect. Due to improvements in the operation scenario and the modification of the guard limiter configuration, the region showing good compatibility was extended to the closer wall position (the wall position was normalized to the plasma minor radius; rwall/a~ 1.25) and the higher normalized beta (βN ~ 3.5), compared with the previous works with the relatively far wall position and stronger magnetic field (Tsuzuki K. et al 2003 Nucl. Fusion. 43 1288). A reduction in the growth rate of the instability was also observed in the close wall case, which presumably corresponds to the wall stabilization effect, similar to a resistive wall without ferromagnetism.
Published: 2006
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23. Activation cross-sections on cadmium: Proton induced nuclear reactions up to 80MeV

Author: F. Tárkányi, B. Király, F. Ditrói, S. Takács, J. Csikai, A. Hermanne, M.S. Uddin, M. Hagiwara, M. Baba, T. Ido, Yu.N. Shubin, and S.F. Kovalev
Subjects: Nuclear and High Energy Physics, Instrumentation
Published: 2006
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24. Turbulence and transport characteristics of a barrier in a toroidal plasma

Author: Patrick Diamond, S. Okamura, Mitsutaka Isobe, K. Nagaoka, Tsuyoshi Akiyama, Chihiro Suzuki, S.-I. Itoh, K. Matsuoka, K. Toi, S. Ohsima, T. Minami, Haruhisa Nakano, Akihiro Shimizu, Kimitaka Itoh, Yasuo Yoshimura, T. Ido, Yoshihiko Nagashima, C. Takahashi, Katsumi Ida, S. Nishimura, Akihide Fujisawa, Mamoru Kojima, and H. Iguchi
Subjects: Physics, Toroid, Turbulence, K-epsilon turbulence model, Magnetic confinement fusion, Plasma, Mechanics, Condensed Matter Physics, law.invention, Nonlinear Sciences::Chaotic Dynamics, Physics::Fluid Dynamics, Nuclear Energy and Engineering, Physics::Plasma Physics, law, Intermittency, Dispersion relation, Physics::Space Physics, Plasma diagnostics, Atomic physics
Abstract: Turbulence and zonal flow at a transport barrier are studied with twin heavy ion beam probes in a toroidal helical plasma. A wavelet analysis is used to extract turbulence properties, e.g. spectra of both density and potential fluctuations, the coherence and the phase between them and the dispersion relation. Particle transport estimated from the fundamental characteristics is found to clearly rise with their intermittent activities after the barrier is broken down. Time-dependent analysis reveals that the intermittency of turbulence is correlated with the evolution of the stationary zonal flow.
Published: 2006
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25. Wavelet and Fourier analysis of zonal flows and density fluctuations in JIPP T-llU tokamak plasmas

Author: Y Hamada, T Watari, A Nishizawa, T Ido, M Kojima, Y Kawasumi, K Toi, and the JIPPT-IIU Group
Subjects: Physics, Tokamak, Turbulence, Magnetic confinement fusion, Zonal flow (plasma), Condensed Matter Physics, law.invention, symbols.namesake, Amplitude, Nuclear Energy and Engineering, Physics::Plasma Physics, law, Fourier analysis, Physics::Space Physics, symbols, Electron temperature, Plasma diagnostics, Atomic physics
Abstract: Wavelet and two-dimensional Fourier analyses of local potential and density signals were conducted. These signals were obtained in the core region of tokamak plasmas by a multiple-sample-volume heavy ion beam probe. In the low-density Ohmic plasma where the electron temperature is much higher than that of the ions, the high-frequency (HF) zonal flow in geodesic acoustic mode frequency region is more energetic than the low-frequency zonal flow from 10 to 1000 Hz in terms of integrated intensity. This result is in sharp contrast to the results of ITG simulations of the tokamak plasmas. The HF zonal flow has a short lifetime (a few cycles). The wavelet spectra of density are much more chaotic than those of potential turbulence, changing the amplitude and frequency of the dominant modes more rapidly within the lifetime of the HF zonal flows. It was also found that HF parts of the density fluctuations are highly modulated by the HF zonal flows.
Published: 2006
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26. Observation of the interaction between the geodesic acoustic mode and ambient fluctuation in the JFT-2M tokamak

Author: T Ido, Y Miura, K Hoshino, K Kamiya, Y Hamada, A Nishizawa, Y Kawasumi, H Ogawa, Y Nagashima, K Shinohara, Y Kusama, and JFT-2M group
Subjects: Physics, Nuclear and High Energy Physics, Tokamak, Statistics::Applications, Geodesic, Separatrix, Plasma, Condensed Matter Physics, Radial direction, Statistics::Computation, law.invention, Heavy ion beam, Amplitude, Physics::Plasma Physics, law, Statistics::Methodology, Atomic physics, Coherence (physics)
Abstract: The electrostatic and density fluctuation are measured simultaneously with a heavy ion beam probe. The electrostatic fluctuation with the geodesic acoustic mode (GAM) frequency is observed in L-mode plasmas and not in H-mode plasmas. The poloidal and radial structure is consistent with the GAM. So the fluctuation is concluded to be the GAM.The amplitude of the GAM changes in the radial direction; it is small near the separatrix, has a maximum at 3 cm inside the separatrix and decreases again to 5 cm inside the separatrix.The GAM and the temporal behaviour of the ambient density fluctuation show a significant coherence, and the phase of modulation of the ambient density fluctuation tends to delay the potential oscillation of the GAM. It is clearly verified that the GAM affects ambient fluctuation and also the local particle transport through modulation of the amplitude of the ambient fluctuation.
Published: 2006
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27. Geodesic–acoustic-mode in JFT-2M tokamak plasmas

Author: T Ido, Y Miura, K Kamiya, Y Hamada, K Hoshino, A Fujisawa, K Itoh, S-I Itoh, A Nishizawa, H Ogawa, Y Kusama, and JFT-2M group
Subjects: Physics, Tokamak, Statistics::Applications, Magnetic confinement fusion, Plasma, Condensed Matter Physics, Statistics::Computation, Computational physics, law.invention, Temperature gradient, Amplitude, Nuclear Energy and Engineering, Physics::Plasma Physics, law, Electric field, Statistics::Methodology, Plasma diagnostics, Atomic physics, Coherence (physics)
Abstract: The characteristics of geodesic–acoustic-mode (GAM) are investigated through direct and simultaneous measurement of electrostatic and density fluctuations with a heavy ion beam probe.The amplitude of the GAM changes in relation to the radial position; it is small near the separatrix, reaches a local maximum at 3 cm inside the separatrix and then decreases again to 5 cm inside the separatrix. The frequency is constant in the range, though the predicted GAM frequency varies according to the temperature gradient. The correlation length is about 6 cm and comparable to the structure of the amplitude of the GAM. The results indicate the GAM has a radial structure which reflects the local condition at about 3 m inside the separatrix.The phase relation between the GAM oscillation indicates that the GAM is a radial propagating wave.The interaction between the GAM and the ambient density fluctuation is shown by the high coherence between the GAM oscillation and the temporal behaviour of the ambient density fluctuation. Moreover, the phase relation between the electric field fluctuation of the GAM ( ) and the amplitude of the density fluctuation indicates that the modulation of the ambient density fluctuation delays the . The causality between the GAM and the modulation of the density fluctuation is revealed.
Published: 2006
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28. Characteristics of Plasma Operation with the Ferritic inside Wall and Its Compatibility with High-Performance Plasmas in JFT-2M

Author: Haruyuki Kimura, Kazuya Uehara, Ryuichi Shimada, N. Isei, Y.M. Miura, Yamamoto Masahiro, Y. Hamada, T. Shibata, Kazuhiro Tsuzuki, Yuji Yamauchi, Satoshi Kasai, Hiroshi Amemiya, Yoshihiko Nagashima, Masayasu Sato, K. Kikuchi, Mohammad Reza Bakhtiari, Katsumichi Hoshino, K. Shinohara, Hisato Kawashima, Y. Kusama, Kensaku Kamiya, Y. Hirohata, Tomoaki Hino, Kentaro Yamaguchi, Hiroaki Ogawa, G. Kurita, T. Ido, and Hiroaki Tsutsui
Subjects: Nuclear and High Energy Physics, Structural material, Tokamak, Materials science, 020209 energy, Mechanical Engineering, Nuclear engineering, technology, industry, and agriculture, Magnetic confinement fusion, 02 engineering and technology, Plasma, 01 natural sciences, 010305 fluids & plasmas, law.invention, Nuclear physics, Nuclear Energy and Engineering, Ferromagnetism, law, Impurity, Beta (plasma physics), 0103 physical sciences, 0202 electrical engineering, electronic engineering, information engineering, General Materials Science, Plasma stability, Civil and Structural Engineering
Abstract: Compatibility between plasma and reduced activation ferritic steel, which is the leading candidate for the structural material of a fusion demonstration reactor, has been investigated in the Advanced Material Tokamak EXperiment (AMTEX). Ferritic plates (FPs) were installed progressively in the JFT-2M tokamak. The effect of ferromagnetism on plasma production, control, confinement, and stability has been investigated. Impurity release behavior has also been investigated. Even when the inside vacuum vessel wall was fully covered with the FPs and the tokamak plasma was operated close to the wall, no deleterious effect was observed, and the normalized beta could be increased up to ~3.5. Thus, encouraging results are obtained for application of this material to the demonstration reactor.
Published: 2006
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29. Reduced divertor heat loads, plasma shape effects, and radial electric field structures in JFT-2M HRS H-mode plasmas

Author: K Kamiya, H Kawashima, T Ido, N Oyama, M Bakhtiari, S Kasai, Y Kusama, Y Miura, H Ogawa, K Tsuzuki, K Uehara, and JFT-2M Group
Subjects: Nuclear and High Energy Physics, Materials science, Divertor, Magnetic confinement fusion, Plasma, Condensed Matter Physics, symbols.namesake, Heat flux, Plasma shaping, Electric field, symbols, Langmuir probe, Plasma diagnostics, Atomic physics
Abstract: A key feature of the 'high recycling steady' (HRS) H-mode regimes is the reduction of the transient heat load to the divertor target due to large ELMs. The heat flux to the divertor targets measured by means of a Langmuir probe in the scrape-off layer on the target plate is about ~0.3 MW m−2 in the typical HRS plasmas, which is very small in comparison with the transient heat load in the ELMy H-mode discharge. In addition, the effects of the plasma shaping on the access to and improved plasma performance of HRS H-mode regimes have been investigated. Furthermore, simultaneous measurements of both density fluctuations and potential profiles at the plasma edge region using a heavy ion beam probe are also presented.
Published: 2006
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30. Overview of confinement and MHD stability in the Large Helical Device

Author: H. Nozato, Hideya Nakanishi, T. Saida, Suguru Masuzaki, H. Funaba, P. R. Goncharov, A. Nishizawa, J. Miyazawa, Nobuyoshi Ohyabu, Hiroe Igami, O. Motojima, Tsuyoshi Akiyama, Shin Kubo, Y. Nagayama, Shigeru Inagaki, N. Noda, T. Uda, K. Nishimura, Satoshi Ohdachi, Kimitaka Itoh, M. Emoto, Naoki Tamura, Yasuo Yoshimura, T. Tokuzawa, Takaaki Fujita, K. Saito, N. Ashikawa, Osamu Kaneko, Satoshi Yamamoto, A. Wakasa, Kazuo Kawahata, T. Minami, Yoshihide Oka, Masaki Osakabe, T. Ido, Masayuki Yokoyama, Masahide Sato, Takashi Mutoh, Shigeki Okajima, Motoshi Goto, Tomohiro Morisaki, Sadatsugu Muto, Ryuichi Sakamoto, K. Narihara, K.Y. Watanabe, Tetsuo Seki, Sadayoshi Murakami, Y. Nakamura, K. Matsuoka, Mikiro Yoshinuma, Y. Narushima, Mitsutaka Isobe, Hiroshi Yamada, Ichihiro Yamada, Masaki Nishiura, Yoshiteru Sakamoto, Mizuki Sakamoto, T. Watari, B.J. Peterson, Kenji Tanaka, H. Kawazome, Mamoru Shoji, Katsumi Ida, Takashi Notake, T. Fukuda, K. Yamazaki, S. Morita, Hidenobu Takenaga, Akihiko Isayama, Takashi Shimozuma, N. Takeuchi, K. Toi, T. Kobuchi, Yuki Torii, Ryuhei Kumazawa, S. Sudo, Katsunori Ikeda, Y. Takeiri, Akio Sagara, Kunizo Ohkubo, A. Komori, Katsuyoshi Tsumori, Satoru Sakakibara, T. Ozaki, C. D. Beidler, Kuninori Sato, Mamiko Sasao, and K. Ishii
Subjects: Nuclear and High Energy Physics, Thermonuclear fusion, Tokamak, Materials science, Plasma parameters, Divertor, Magnetic confinement fusion, Condensed Matter Physics, Neutral beam injection, law.invention, Large Helical Device, Physics::Plasma Physics, law, Beta (plasma physics), Atomic physics
Abstract: The Large Helical Device is a heliotron device with L = 2 and M = 10 continuous helical coils with a major radius of 3.5–4.1 m, a minor radius of 0.6 m and a toroidal field of 0.5–3 T, which is a candidate among toroidal magnetic confinement systems for a steady state thermonuclear fusion reactor. There has been significant progress in extending the plasma operational regime in various plasma parameters by neutral beam injection with a power of 13 MW and electron cyclotron heating (ECH) with a power of 2 MW. The electron and ion temperatures have reached up to 10 keV in the collisionless regime, and the maximum electron density, the volume averaged beta value and stored energy are 2.4 × 1020 m−3, 4.1% and 1.3 MJ, respectively. In the last two years, intensive studies of the magnetohydrodynamics stability providing access to the high beta regime and of healing of the magnetic island in comparison with the neoclassical tearing mode in tokamaks have been conducted. Local island divertor experiments have also been performed to control the edge plasma aimed at confinement improvement. As for transport study, transient transport analysis was executed for a plasma with an internal transport barrier and a magnetic island. The high ion temperature plasma was obtained by adding impurities to the plasma to keep the power deposition to the ions reasonably high even at a very low density. By injecting 72 kW of ECH power, the plasma was sustained for 756 s without serious problems of impurities or recycling.
Published: 2005
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31. Zonal flows in the geodesic acoustic mode frequency range in the JIPP T-IIU tokamak plasmas

Author: Y Hamada, A Nishizawa, T Ido, T Watari, M Kojima, Y Kawasumi, K Narihara, K Toi, and JIPPT-IIU Group
Subjects: Physics, Nuclear and High Energy Physics, Tokamak, Magnetic confinement fusion, Plasma, Zonal flow (plasma), Condensed Matter Physics, Plasma oscillation, law.invention, Amplitude, Physics::Plasma Physics, law, Electric field, Plasma diagnostics, Atomic physics
Abstract: Large potential oscillations were detected in JIPPT-IIU tokamak plasmas in a wide range of plasma cross-sections in measurements using a multi-sample-volume heavy ion beam probe. These oscillations have large amplitudes reaching a few hundreds of volts and their frequencies are in the range of the geodesic acoustic mode (GAM). They are found over a wide range of plasma cross-sections and commonly have m = 0 structures. As they were Fourier analysed, it was found that the central frequency is higher in the core of the plasma and lower in the edge of the plasma. These observations agree with the properties of theoretically predicted GAM oscillations. It was also found that the frequency spectrum is peaked in the core and broad in the edge, which may have something to do with damping mechanisms of the GAM. The phase relation between the density and the electric field fluctuations was studied extensively in terms of the cross-correlation function. The level of the density fluctuation was low as it should be, and the expected 90° phase difference was found in a limited radial domain.
Published: 2005
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32. Coherent edge fluctuation measurements in H-mode discharges on JFT-2M

Author: Y Nagashima, K Shinohara, K Hoshino, A Ejiri, K Tsuzuki, T Ido, K Uehara, H Kawashima, K Kamiya, H Ogawa, T Yamada, S Shiraiwa, S Ohara, Y Takase, N Asakura, N Oyama, T Fujita, S Ide, H Takenaga, Y Kusama, Y Miura, and JFT-2M group
Subjects: Materials science, Separatrix, business.industry, Mode (statistics), Phase (waves), Plasma, Edge (geometry), Condensed Matter Physics, Intensity (physics), symbols.namesake, Optics, Nuclear Energy and Engineering, symbols, Langmuir probe, Transient (oscillation), Atomic physics, business
Abstract: Results of coherent edge fluctuation measurements using three diagnostics (a reciprocating Langmuir probe, a two channel O-mode reflectometer, and fast magnetic probes) in H-mode discharges on JFT-2M are presented. In discharges in which a high recycling steady (HRS) H-mode phase is obtained through a transient phase with slightly enhanced Dα intensity, two types of coherent fluctuations are observed. The higher frequency mode (around 300 kHz) is the high frequency mode (HFM) observed in the HRS H-mode (Kamiya K et al 2003 9th IAEA Tech. Meeting H-mode Workshop Topic B-14). The lower frequency mode has a frequency of around 80 kHz. The HFM is detected by a Langmuir probe over a wide region in the SOL, as well as by the reflectometer and magnetic probes. However, the HFM is not detected by the higher frequency (38 GHz) channel of the reflectometer after the HRS transition, suggesting that the HFM is not located deeply inside the plasma. The 80 kHz mode is detected by both channels of the reflectometer and by a Langmuir probe, but not by magnetic probes, suggesting that it is an electrostatic mode. In contrast to the HFM, the 80 kHz mode is detected by the Langmuir probe only near the separatrix during the transient phase, which leads to either the HRS phase or the ELMy phase, and is similar to the fluctuations reported in Shinohara K et al (1998 J. Plasma Fusion Res. 74 607).
Published: 2004
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33. Recent diagnostic developments on LHD

Author: S Sudo, Y Nagayama, B J Peterson, K Kawahata, T Akiyama, N Ashikawa, M Emoto, M Goto, Y Hamada, K Ida, T Ido, H Iguchi, S Inagaki, M Isobe, T Kobuchi, A Komori, Y Liang, S Masuzaki, T Minami, T Morisaki, S Morita, S Muto, Y Nakamura, H Nakanishi, M Narushima, K Narihara, M Nishiura, A Nishizawa, S Ohdachi, M Osakabe, T Ozaki, R O Pavlichenko, S Sakakibara, K Sato, M Shoji, N Tamura, K Tanaka, K Toi, T Tokuzawa, K Y Watanabe, T Watanabe, H Yamada, I Yamada, M Yoshinuma, P Goncharov, D Kalinina, T Kanaba, T Sugimoto, A Ejiri, Y Ono, H Hojo, K Ishii, N Iwama, Y Kogi, A Mase, M Sakamoto, K Kondo, H Nagasaki, S Yamamoto, N Nishino, S Okajima, T Saida, M Sasao, T Takeda, S Tsuji-Iio, D S Darrow, H Takahashi, Y Liu, J F Lyon, A Yu Kostrioukov, V B Kuteev, V Sergeev, I Viniar, A V Krasilnikov, A Sanin, L N Vyacheslavov, D Stutman, M Finkenthal, O Motojima, and LHD Group
Subjects: Physics, Plasma parameters, business.industry, Divertor, Bolometer, Polarimeter, Condensed Matter Physics, Laser, Photon counting, law.invention, Large Helical Device, Optics, Nuclear Energy and Engineering, law, Plasma diagnostics, business
Abstract: Standard diagnostics for fundamental plasma parameters and for plasma physics are routinely utilized for daily operation and physics studies in the large helical device (LHD) with high reliability. Diagnostics for steady-state plasma are under intensive development, especially for Te, ne (yttrium–aluminium garnet (YAG) laser Thomson, CO2 laser polarimeter), data acquisition in steady-state and heat-resistant probes. To clarify the plasma properties of the helical structure, two- or three-dimensional diagnostics are being aggressively developed: tangential cameras (fast SX TV, photon counting CCD, Hα TV); tomography (tangential SX CCD, bolometer); imaging (bolometer, ECE, reflectometer). Divertor and edge physics are important key issues for steady-state operation. Diagnostics for neutral flux (Hα array, Zeeman spectroscopy) and ne (fast scanning probe, Li beam probe, pulsed radar reflectometer) are also in advanced stages of development. In addition to these, advanced diagnostics are being intensively developed in LHD through domestic and international collaborations.
Published: 2003
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34. High performance tokamak experiments with a ferritic steel wall on JFT-2M

Author: K. Shinohara, A. Amemiya, Kazuya Uehara, Tomoaki Hino, Haruyuki Kimura, Y. Hamada, Toru Ogawa, Satoshi Kasai, Shigeo Yatsu, Hiroaki Ogawa, Akira Tsushima, Naoyuki Kayukawa, M. Yamamoto, Masayasu Sato, Katsumichi Hoshino, Shinichi Nomura, K. Miyachi, Naoyuki Fukumoto, Ryuichi Shimada, T. Shibata, Kazuhiro Tsuzuki, Hisato Kawashima, T. Ito, H. Ajikawa, Kensaku Kamiya, Y.M. Miura, T. Ido, Hironobu Niimi, Y. Sadamoto, Akira Ejiri, Yuko Hirohata, Masayoshi Nagata, Hiroaki Tsutsui, H. Sasao, K. Kikuchi, Yoshihiko Nagashima, Tadao Uyama, Mohammad Reza Bakhtiari, Y. Kusama, and N. Isei
Subjects: Nuclear and High Energy Physics, Tokamak, Materials science, Magnetic structure, Nuclear engineering, Ripple, Plasma, Edge (geometry), Condensed Matter Physics, Ion, law.invention, Nuclear physics, law, Impurity, Beta (plasma physics)
Abstract: Compatibility between the plasma and low activation ferritic steel, which is a candidate material for fusion demonstration reactors, has been investigated step by step in the JFT-2M tokamak. We have entered the third stage of the Advanced Material Tokamak EXperiment (AMTEX), where the inside of the vacuum vessel wall is completely covered with ferritic steel plates ferritic inside wall (FIW). The effects of a FIW on the plasma production, impurity release, the operation region, and H-mode characteristics have been investigated. No negative effect has been observed up to now. A high normalized beta plasma of βN ~ 3, having both an internal transport barrier and a steady H-mode edge was obtained. A remarkable reduction in ripple trapped loss from 0.26 MW m−2 (without ferritic steel) to less than 0.01 MW m−2 was demonstrated by the optimization of the thickness profile of FIW. A code to calculate fast ion losses, taking into account the full three-dimensional magnetic structure was developed, and values obtained using the code showed good agreement with experimental results. Thus, encouraging results are obtained for the use of this material in the demo-reactor.
Published: 2003
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35. Recent diagnostic developments on LHD

Author: S Sudo, T Ozaki, N Ashikawa, M Emoto, M Goto, Y Hamada, K Ida, T Ido, H Iguchi, S Inagaki, M Isobe, K Kawahata, K Khlopenkov, T Kobuchi, Y Liang, S Masuzaki, T Minami, S Morita, S Muto, Y Nagayama, H Nakanishi, K Narihara, A Nishizawa, S Ohdachi, M Osakabe, B J Peterson, S Sakakibara, M Sasao, K Sato, M Shoji, N Tamura, K Tanaka, K Toi, T Tokuzawa, K Watanabe, T Watanabe, I Yamada, LHD Team, P Goncharov, A Ejiri, S Okajima, A Mase, S Tsuji-Iio, T Akiyama, J F Lyon, L N Vyacheslavov, and A Sanin
Subjects: Nuclear Energy and Engineering, Condensed Matter Physics
Published: 2003
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36. Repeated use of molten carbonate catalysts for gasification of carbonaceous materials by carbon dioxide

Author: H. Itoh, Shigeo Goto, and T. Ido
Subjects: Materials science, General Chemical Engineering, Catalyst support, Batch reactor, Industrial catalysts, Inorganic chemistry, General Chemistry, Catalysis, chemistry.chemical_compound, chemistry, medicine, Carbonate, Graphite, Eutectic system, Activated carbon, medicine.drug
Abstract: Reactions of carbonaceous materials (activated carbon, graphite, and lignin) with carbon dioxide were carried out at 973 K using alkali metal carbonates (m.p. 891∼1164 K) and eutectic mixtures of these compounds (m.p. 669∼787 K) as catalysts. The reaction occurred when the carbonate catalysts were physically mixed with carbonaceous materials and the melting points of the catalysts were lower than the reaction temperature. However, the reaction did not proceed with physically mixed catalysts when the melting points of the catalysts were higher than the reaction temperature. Repeated use of the molten catalyst was also studied to investigate the possibility of continuous gasification of carbonaceous materials. After the activated carbon (or lignin) was consumed in a batch reactor, the same amount was added in the reactor containing the catalyst and the reaction started again. It was found that the eutectic molten catalyst could be reused without any loss of its catalytic activity by repeating this operation.
Published: 2003
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37. Postprocessing algorithm for particle-tracking velocimetry based on ellipsoidal equations

Author: Yuichi Murai, T. Ido, and Fujio Yamamoto
Subjects: Fluid Flow and Transfer Processes, Differential equation, Computer science, Computational Mechanics, General Physics and Astronomy, Velocimetry, Vorticity, Vortex, Physics::Fluid Dynamics, Continuity equation, Flow (mathematics), Mechanics of Materials, Particle tracking velocimetry, Boundary value problem, Algorithm, ComputingMethodologies_COMPUTERGRAPHICS
Abstract: Accurate postprocessing methods are required in order to analyze the detailed flow structures from the scattered data of particle-tracking velocimetry (PTV). In particular, vorticity distributions and stream functions are not reasonably obtained by conventional methods. This paper proposes a new postprocessing algorithm based on ellipsoidal differential equations; this method utilizes data as discrete boundary conditions. The results obtained by the proposed algorithm fully satisfy the equation of continuity and simultaneously correspond well with the raw data. The performance of the algorithm is examined by applying it to two-dimensional vortex flows and isotropic turbulent flows. The results reveal that the present algorithm has the highest accuracy among several conventional methods for detecting vorticity and streamlines.
Published: 2002
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38. The 7th Asia-Pacific Transport Working Group (APTWG) meeting

Author: K. Ida, D.F. Kong, T. Fujita, T. Ido, W.H. Ko, and S. Maeyama
Subjects: Plasma, Nuclear and High Energy Physics, MHD, transport, turbulence, blob, 0103 physical sciences, 010306 general physics, Condensed Matter Physics, 01 natural sciences, 010305 fluids & plasmas
Abstract: This conference report summarizes the contributions to, and discussions at, the 7th Asia-Pacific Transport Working Group Meeting held at Nagoya University, Japan, during 5–8 June 2017. The topics of the meeting were organized under four main headings: (1) turbulence and blob at the boundary of magnetic topology, (2) model reduction and experiments for validation, (3) mode competition in turbulence and MHD driven by energetic particle, (4) mechanism determining plasma flows and their impact on transport and MHD. The Young Researchers Forum which was held in this meeting is also described in this report.
Published: 2017
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39. A combined loop-SPE method for the automated preparation of [11C]doxepin

Author: C. Pascali, Anna Bogni, Ren Iwata, T. Ido, Kazuhiko Yanai, Kiichi Ishiwata, and Motohisa Kato
Subjects: Methyl triflate, Chromatography, Chemistry, Organic Chemistry, Extraction (chemistry), Doxepin, Biochemistry, Chemical synthesis, High-performance liquid chromatography, Analytical Chemistry, Loop (topology), Yield (chemistry), Drug Discovery, medicine, Radiology, Nuclear Medicine and imaging, Solid phase extraction, Spectroscopy, medicine.drug
Abstract: A simple and versatile loop-solid phase extraction (SPE) method was developed for the automated preparation of [11C]doxepin, a histamine H1 receptor antagonist, from [11C]methyl triflate ([11C]MeOTf). This labeling agent was passed through a Teflon or Tefzel loop coated internally with a film of the precursor solution. The reaction products were then flushed from the loop to a short SPE column, where they were concentrated and then injected onto a semi-preparative HPLC column simply by switching an injection valve. By applying this combined loop-SPE technique the whole procedure turned out to be easily automated. The formation of [11C]methylated doxepin ([11C]methyldoxepin) was observed and the ratio of doxepin to methyldoxepin was found to be clearly correlated with the mass ratio of nordoxepin to MeOTf. This observation highlights the importance of [11C]MeOTf specific activity in the [11C]methylation of secondary amines. Using this method, [11C]Doxepin was prepared in over 40% radiochemical yield from high specific activity [11C]MeOTf. Copyright © 2002 John Wiley & Sons, Ltd.
Published: 2002
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40. A study of high-energy ions produced by ICRF heating in LHD

Author: Yuki Torii, Ryuichi Sakamoto, Mitsutaka Isobe, Akio Sagara, Kenji Saito, Motoshi Goto, Masami Fujiwara, N. Ashikawa, O. Motojima, K. Nishimura, T. Tokuzawa, J. Miyazawa, A. Kato, B.J. Peterson, Tomo-Hiko Watanabe, H. Funaba, Atsushi Fukuyama, T. Yamamoto, Osamu Kaneko, S. Sudo, Nobuyoshi Ohyabu, Soichiro Yamaguchi, A. V. Krasilnikov, Tetsuo Seki, Y. Zhao, Y. Nakamura, Mitsuhiro Yokota, Hiroshi Yamada, C.\\' Zhang, Ichihiro Yamada, Masayuki Yokoyama, T. Watari, Ryuhei Kumazawa, K. Toi, Satoshi Ohdachi, Kimitaka Itoh, Masahide Sato, S. Morita, Hideya Nakanishi, T. Ozaki, Hajime Suzuki, Katsunori Ikeda, Satoru Sakakibara, Mamiko Sasao, Kazuo Kawahata, Kuninori Sato, Mamoru Shoji, Katsumi Ida, N. Noda, Takashi Shimozuma, Suguru Masuzaki, K. Akaishi, Y. Hamada, A. Komori, Fujio Shimpo, K.Y. Watanabe, Sadatsugu Muto, Masaki Osakabe, T. Ido, Shin Kubo, Yasuo Yoshimura, K. Narihara, S. Murakami, Yoshihide Oka, Kunizo Ohkubo, Katsuyoshi Tsumori, Kenji Tanaka, Goro Nomura, N. Takeuchi, T. Minami, Takashi Mutoh, Tomohiro Morisaki, S. Yamamoto, N. Inoue, Shigeru Inagaki, Takashi Notake, Hiroshi Idei, Y. Nagayama, M. Emoto, K. Yamazaki, and Y. Takeiri
Subjects: Range (particle radiation), Materials science, Cyclotron, Plasma, Condensed Matter Physics, law.invention, Ion, Large Helical Device, Distribution function, Nuclear Energy and Engineering, law, Particle, Atomic physics, Neutral particle
Abstract: This paper reports on the behaviour of high-energy ions created by ion cyclotron range of frequency (ICRF) heating on the Large Helical Device (LHD). In the third experimental campaign conducted in 1999, it was found that minority heating has good heating performance, and high-energy particles were observed. In the fourth campaign in 2000, the temporal behaviour of high-energy ions was investigated in the minority heating regime using turnoff or modulation of ICRF power. The time evolution of the high-energy particle distribution was measured using a natural diamond detector (NDD) and a time-of-flight neutral particle analyser (TOF-NPA). It was found that the count number of higher-energy particles declines faster than that of lower-energy particles after ICRF turnoff. In the modulation experiments, the phase difference of the flux of high-energy particles with respect to the ICRF power modulation increased with energy. These results were explained qualitatively by the Fokker-Planck equation with a simple model. The pitch-angle dependence of the distribution function was also measured in the experiment by changing the line of sight of the TOF-NPA, and an anisotropy of the high-energy tail was found. This anisotropy was reproduced by solving the bounce-averaged Fokker-Planck equation. The second harmonic heating was conducted successfully for the first time in the LHD in high-β plasma, and high-energy particles were also detected in this heating regime.
Published: 2001
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41. Relations among potential change, fluctuation change and transport barrier in the JFT-2M tokamak

Author: Y. Miura, T. Ido, K. Kamiya, Y. Hamada, and JFT-2M Group
Subjects: Physics, Nuclear and High Energy Physics, Tokamak, Plasma, Sawtooth wave, Transport barrier, Condensed Matter Physics, law.invention, Heavy ion beam, law, Potential change, Jump, Rectangular potential barrier, Atomic physics
Abstract: Potential and density/temperature fluctuations at the L-H transition are measured by the heavy ion beam probe on JFT-2M. It has been observed that the timescale of the potential change is as fast as 10-100??s when the input power (Pin) is larger than the L-H threshold power (Pth). When Pin ~ Pth, the confinement is improved gradually step by step with sawtooth crashes. After a few sawtooth crashes, the potential drops rapidly to the level of the ELM free H mode. From the gradual change of the potential, assuming that dEr/dr is a key to forming and sustaining the transport barrier, the criterion of dEr/dr is less than (1.2?0.4) ? 103?kV/m2. At an ELM just before the H-L transition, the potential inside the separatrix also shows a rapid positive jump. The timescales of the positive jump and of the recovery of the potential to its negative value are about 40 and 150??s, respectively. Before the H-L transition, the time between ELMs and/or dithering transition becomes shorter and the plasma finally goes back to the L?mode.
Published: 2001
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42. Liquid impedance matching system for ion cyclotron heating

Author: T. Ido, T. Watari, G. Nomura, Tetsuo Seki, F. Paoletti, Yuanzhe Zhao, Ryuhei Kumazawa, G. Cattanei, Takashi Mutoh, Kenji Saito, Fujio Shimpo, and S. Bernabei
Subjects: Materials science, business.industry, Cyclotron, Impedance matching, Tuner, Stub (electronics), law.invention, Large Helical Device, Nuclear magnetic resonance, law, Transmission line, Optoelectronics, Nuclear fusion, business, Instrumentation, Voltage
Abstract: Ion cyclotron heating has been established as one of the heating schemes in nuclear fusion research and its use in steady state plasma heating in various devices is being considered. The optimal technology for steady state ion cyclotron range of frequency heating has not been firmly established. This article reports on the liquid stub tuner which was newly developed in research and development activities on the large helical device. It demonstrated high performance in real use in experiments. Two different impedance-matching systems based on the liquid stub tuner are studied: one is a triple liquid stub tuner system and the other is a single stub tuner system with a liquid phase shifter. The characteristics of the two systems are compared from the points of view of how wide a frequency range is covered, and how great the reduction of the voltage in the transmission line is.
Published: 2001
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43. Protective effect of riluzole on MPTP-induced depletion of dopamine and its metabolite content in mice

Author: Tsutomu Araki, T. Ido, Mitsunobu Matsubara, Y. Itoyama, T. Kumagai, and Yutaka Imai
Subjects: Male, medicine.medical_specialty, Time Factors, Dopamine, Dopamine Agents, Striatum, Receptors, N-Methyl-D-Aspartate, Biochemistry, Neuroprotection, Sodium Channels, Mice, Cellular and Molecular Neuroscience, chemistry.chemical_compound, Internal medicine, medicine, Animals, Neurons, Riluzole, Dose-Response Relationship, Drug, Chemistry, MPTP, Dopaminergic, Brain, Pargyline, Corpus Striatum, nervous system diseases, Mice, Inbred C57BL, Neuroprotective Agents, Endocrinology, nervous system, 1-Methyl-4-phenyl-1,2,3,6-tetrahydropyridine, 3,4-Dihydroxyphenylacetic Acid, NMDA receptor, Neurology (clinical), Dizocilpine Maleate, medicine.drug
Abstract: The neuroprotective effects of riluzole (2-amino-6-trifluoromethoxy benzothiazole), a Na+ channel blocker with antiglutamatergic activity, MK-801, a blocker of N-methyl-D-aspartate (NMDA) receptors and monoamine oxidase (MAO) inhibitor pargyline were compared in the model of 1-methyl-4-phenyl-1,2,3,6-tetrahydropyridine (MPTP)-induced depletion of dopamine and its metabolite 3, 4-dihydroxyphenylacetic acid (DOPAC) levels in mice. The mice received four intraperitoneal injections of MPTP (10 mg/kg) at 1-hr intervals and then the brains were analyzed at 1, 3 and 7 days after the treatments. Dopamine and DOPAC levels were significantly decreased in the striatum from 1 day after MPTP treatments. A severe depletion in dopamine and DOPAC levels was found in the striatum 3 and 7 days after MPTP treatments. Riluzole dose-dependently antagonized the MPTP-induced decrease in dopamine and DOPAC levels in the striatum. Pargyline also protected against MPTP-induced decrease in dopamine levels in the striatum. However, this drug showed no significant change in the striatal DOPAC levels. On the other hand, MK-801 failed to protect against MPTP-induced decrease in dopamine levels in the striatum. However, MK-801 reversed the MPTP-induced decrease in DOPAC levels. These results suggest that riluzole can protect against MPTP-induced striatal dopamine and DOPAC depletion in mice. This protective effect may be caused by inactivation of voltage-dependent Na+ channels by riluzole. Furthermore, the present study suggests that the activation of NMDA receptors does not mainly contribute to MPTP-induced neurodegeneration, whereas MAO, especially MAO type B(MAO-B) plays a crucial role in MPTP-induced degeneration of the nigrostriatal dopaminergic neuronal pathway.
Published: 2000
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44. Temporal behaviour of the potential and fluctuations at the L-H transition on JFT-2M

Author: A. Nishizawa, Y. Hamada, Y.M. Miura, T Ido, Kensaku Kamiya, and Y. Kawasumi
Subjects: Materials science, Heavy ion beam, Nuclear Energy and Engineering, Scale (ratio), Potential change, Atomic physics, Condensed Matter Physics, Power (physics)
Abstract: Potential and density/temperature fluctuations at the L-H transition are measured by a heavy ion beam probe (HIBP) on JFT-2M. It has been observed that the time scale of potential change is as fast as 10-100 µs when the input power (Pin) is larger than the L-H threshold power (Pth). When Pin = Pth, the confinement is improved step by step, with sawteeth crashes accompanied by a decrease of potential. After a few sawteeth crashes, the potential drops rapidly to the level of the ELM-free H-mode. At that time, the density/temperature fluctuations are suppressed simultaneously. The observations of the temporal behaviour of the potential and fluctuations in such an L-H transition are reported.
Published: 2000
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45. Liquid stub tuner for ion cyclotron heating

Author: T. Watari, G. Nomura, J. M. Noterdaeme, Yang-Ping Zhao, T. Seki, R. Kumazawa, F. Sinpo, T. Mutoh, and T. Ido
Subjects: Materials science, Loop antenna, business.industry, RF power amplifier, Cyclotron, Impedance matching, Feedthrough, Tuner, Stub (electronics), law.invention, Large Helical Device, Nuclear magnetic resonance, law, Optoelectronics, business, Instrumentation
Abstract: Ion cyclotron range of frequency (ICRF) heating on the large helical device (LHD) is characterized by high power (up to 12 MW) and steady state operation (30 min). The LHD is a helical device (with a major radius of 3.9 m and a minor radius of 0.6 m) with superconducting coil windings (l=2, m=10). The main purpose of physical research is to investigate currentless and disruption-free plasma. Research and development for steady state ICRF heating has been carried out in recent years: A high rf power transmission system consisting of stub tuners, a ceramic feedthrough, and an ion cyclotron heating loop antenna has been developed. In addition, steady state operation of a rf oscillator has been achieved at a power higher than 1 MW. A liquid stub tuner has been proposed as an innovation. The liquid stub tuner makes use of the difference between the rf wavelengths in liquid and in gas due to the different relative dielectric constants. The liquid stub tuner has been experimentally proved to be a reliable rf com...
Published: 1999
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46. Steady-State Tests of High-Voltage Ceramic Feedthroughs and Coaxial Transmission Line for ICRF Heating System of the Large Helical Device

Author: Fujio Simpo, Jean-Marie Noterdaeme, T. Watari, T. Ido, Y. Zhao, Tetsuo Seki, Ryuhei Kumazawa, Goro Nomura, and Takashi Mutoh
Subjects: Materials science, Steady state, business.industry, 020209 energy, Cyclotron, General Engineering, Feedthrough, High voltage, 02 engineering and technology, Plasma, 01 natural sciences, 010305 fluids & plasmas, law.invention, Large Helical Device, Heating system, law, visual_art, 0103 physical sciences, 0202 electrical engineering, electronic engineering, information engineering, visual_art.visual_art_medium, Optoelectronics, Ceramic, business
Abstract: Steady-state ion cyclotron range of frequency (ICRF) heating technologies have been developed to heat plasma for >30 min in the Large Helical Device (LHD). Steady-state-operation tests of high volt...
Published: 1999
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47. Steady State Test at High RF Voltage on Transmission System for Ion Cyclotron Heating

Author: Ryuhei Kumazawa, Yangping Zhao, Jean-Marie Noterdaeme, Fujio Shinpo, Takashi Mutoh, Tetsuo Seki, T. Ido, Gorou Nomura, and Tetsuo Watari
Subjects: Materials science, business.industry, Loop antenna, RF power amplifier, Cyclotron, Pulse duration, Tuner, law.invention, Stub (electronics), Large Helical Device, Nuclear magnetic resonance, law, Optoelectronics, business, Voltage
Abstract: Ion Cyclotron Range of Frequency (ICRF) heating on Large Helical Device (LHD) is characterized by its high power (up to 12MW) and by steady state operation (30 minutes). The LHD is a helical device (with a major radius of 3.9 m and a minor radius of 0.6m) with super-conducting coil windings (l=2, m=10). The main physical purpose is to investigate currentless and disruption-free steady state plasmas. Research and development for ICRF heating have been carried out in recent years. A high RF power transmission system has been developed, which consists of stub tuners, ceramic feed-through and ICRF heating loop antenna. The RF transmission system was tested and withstood 58kV for 10 seconds and 40kV for 30 minutes. The RF voltage corresponds in the case of a plasma loading resistance, 5Ω to a transmitted RF power capability of 3.4MW and 1.6MW. In addition, a pre-matching stub tuner was very effective in reducing the RF voltage. The reduction rate was confirmed to be one third, which leads to a higher ICRF injection efficiency because of reduction of RF power loss in the transmission system. Furthermore a proper procedure to effectively carry out aging of the RF antenna was found in terms of selecting the RF pulse length, repetition rate and RF voltage.
Published: 1999
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48. A case of corticobasal degeneration studied with positron emission tomography

Author: H, Nagasawa, T, Imamura, H, Nomura, M, Itoh, and T, Ido
Abstract: We measured cerebral blood flow, oxygen metabolism, glucose utilization, and dopamine metabolism in the brain of a patient with corticobasal degeneration using positron emission tomography (PET). The clinical picture is distinctive, comprising features referable to both cortical and basal ganglionic dysfunction. Brain imagings of glucose and dopamine metabolism can demonstrate greater abnormalities in the cerebral cortex and in the striatum contralateral to the more affected side than those of blood flow and oxygen metabolism. This unique combination study measuring both cerebral glucose utilization and dopamine metabolism in the nigrostriatal system can provide efficient information about the dysfunctions which are correlated with individual clinical symptoms, and this study is essential to diagnosis of corticobasal degeneration.
Published: 2014

49. PET study in a patient with spinocerebellar degeneration before and after long-term administration of thyrotropin releasing hormone

Author: H, Tanji, H, Nagasawa, T, Hayashi, H, Onodera, T, Fujiwara, M, Itoh, T, Ido, and Y, Itoyama
Abstract: We studied the chronic effect of thyrotropin releasing hormone (TRH) in a patient with spinocerebellar degeneration by measuring cerebral metabolic rate for glucose (CMRG1c) using 2-[18F]fluoro-2-deoxy-D-glucose (18FDG) and positron emission tomography (PET). A 56-year-old female, who had suffered from progressive ataxia for 2 years, was treated by intravenous administration of 2 mg TRH for 3 weeks, and CMRG1c of the brain was measured before and after treatment. CMRG1c was markedly decreased in the cerebellum and there was no significant difference before and after the treatment, i.e. mean CMRG1c values were 4.92 and 4.90 mg/100 g/min, and the ratios of the cerebellum versus the frontal cortex were 0.50 and 0.51, respectively. The degree of disequilibrium of her body examined with stabilography became better by the 19th day and further improved by the 26th day after the start of TRH treatment. Based on the present study we conclude that long-term administration of TRH did not improve CMRG1c in the cerebellum, but evidently improved the sway of gravity center by stabilography. We speculate that the chronic effect of TRH was not necessarily due to an improvement of cerebellar function, because TRH receptors are widely distributed throughout the central nervous system.
Published: 2014

50. Extension of high Te regime with upgraded ECRH system in the LHD

Author: H. Takahashi, T. Shimozuma, S. Kubo, Y. Yoshimura, H. Igami, S. Ito, S. Kobayashi, Y. Mizuno, K. Okada, T. Mutoh, K. Nagaoka, S. Murakami, M. Osakabe, I. Yamada, H. Nakano, M. Yokoyama, T. Ido, A. Shimizu, R. Seki, K. Ida, M. Yoshinuma, T. Kariya, R. Minami, T. Imai, and null LHD experiment group
Subjects: Physics, Large Helical Device, law, Gyrotron, Electric field, Electron temperature, Electron, Plasma, Radiation, Atomic physics, Energy (signal processing), law.invention
Abstract: Enhancement of the output power per gyrotron has been planned in the Large Helical Device (LHD). Three 77-GHz gyrotrons with an output power of more than 1 MW have been operated. In addition, a high power gyrotron with the frequency of 154 GHz (1 MW/5 s, 0.5 MW/CW) was newly installed in 2012 and the total injection power of ECRH reached 4.6 MW. The operational regime of ECRH plasma on the LHD has been extended due to the upgraded ECRH system such as the central electron temperature T{sub e0} = 13.5 keV with n{sub e} = 1×10{sup 19}m{sup −3}. In the LHD, an electron-internal-transport barrier (e-ITB) related to the production of high T{sub e} plasmas has been realized by strongly centre-focused ECRH. The electron thermal confinement clearly improved inside the e-ITB. The radial electric field was measured using the heavy ion beam probe. The formation of the positive E{sub r} was observed in the core region, which well agreed with the prediction of the neoclassical transport theory. The energy confinement characteristics have been investigated in the ECRH plasmas. It was found that higher plasma stored energy and lower radiation power was realized in the outward configuration. The plasma stored energy of 530more » kJ with n{sub e} = 3.2×10{sup 19}m{sup −3}, which is the 1.7 times larger than the previous record in the ECRH plasma in the LHD, has been successfully achieved.« less
Published: 2014
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