22 results on '"Kubo, S"'
Search Results
2. High-power and Steady-state Operation of ICRF Heating in the Large Helical Device.
- Author
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Mutoh, T., Seki, T., Saito, K., Kasahara, H., Seki, R., Kamio, S., Kumazawa, R., Kubo, S., Shimozuma, T., Yoshimura, Y., Igami, H., Takahashi, H., Ii, T., Makino, R., Nagaoka, K., Nomura, G., and Shinya, T.
- Subjects
ELECTRIC power ,CYCLOTRON resonance ,ELECTRIC impedance ,ELECTRON temperature ,ANTENNAS (Electronics) - Abstract
Recent progress in an ion cyclotron range of frequencies (ICRF) heating system and experiment results in a Large Helical Device (LHD) are reported. Three kinds of ICRF antenna pairs were installed in the LHD, and the operation power regimes were extended up to 4.5 MW; also, the steady-state operation was extended for more than 45 min in LHD at a MW power level. We studied ICRF heating physics in heliotron configuration using a Hand Shake type (HAS) antenna, Field Aligned Impedance Transforming (FAIT) antenna, and Poloidal Array (PA) antenna, and established the optimum minority-ion heating scenario in an LHD. The FAIT antenna having a novel impedance transformer inside the vacuum chamber could reduce the VSWR and successfully injected a higher power to plasma. We tested the PA antennas completely removing the Faraday-shield pipes to avoid breakdown and to increase the plasma coupling. The heating performance was almost the same as other antennas; however, the heating efficiency was degraded when the gap between the antenna and plasma surface was large. Using these three kinds of antennas, ICRF heating could contribute to raising the plasma beta with the second- and third-harmonic cyclotron heating mode, and also to raising the ion temperature as discharge cleaning tools. In 2014, steady-state operation plasma with a line-averaged electron density of 1.2 x 10
19 m-3 , ion and electron temperature of 2 keV, and plasma sustainment time of 48 min was achieved with ICH and ECH heating power of 1.2 MW for majority helium with minority hydrogen. In 2015, the higherpower steady-state operation with a heating power of up to 3 MW was tested with higher density of 3 x 1019 m-3 . [ABSTRACT FROM AUTHOR]- Published
- 2015
- Full Text
- View/download PDF
3. Electron Cyclotron ∕ Bernstein Wave Heating and Current Drive Experiments using Phased-array Antenna in QUEST
- Author
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Idei, H., primary, Zushi, H., additional, Hanada, K., additional, Nakamura, K., additional, Fujisawa, A., additional, Hasegawa, M., additional, Yoshida, N., additional, Sakamoto, M., additional, Watanebe, H., additional, Tokunaga, K., additional, Nagashima, Y., additional, Ejiri, A., additional, Sakaguchi, M., additional, Kalinnikova, E., additional, Ishiguro, M., additional, Tashima, S., additional, Fukuyama, A., additional, Igami, H., additional, Kubo, S., additional, Sharma, S. K., additional, Ryokai, T., additional, Liu, H. Q., additional, Isobe, M., additional, Nagaoka, K., additional, Nakanishi, H., additional, Nishino, N., additional, Kawasaki, S., additional, Nakashima, H., additional, Higashijima, A., additional, Takase, Y., additional, Maekawa, T., additional, Mitarai, O., additional, Kikuchi, M., additional, Toi, K., additional, Phillips, Cynthia K., additional, and Wilson, James R., additional
- Published
- 2011
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4. The Small Satellite “Tsubame” for Polarimetry of GRBs
- Author
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Toizumi, T., primary, Kawakami, K., additional, Tokoyoda, K., additional, Enomoto, T., additional, Yatsu, Y., additional, Kawai, N., additional, Nakamori, T., additional, Kataoka, J., additional, Kubo, S., additional, McEnery, J. E., additional, Racusin, J. L., additional, and Gehrels, N., additional
- Published
- 2011
- Full Text
- View/download PDF
5. Gamma-Ray Polarimetry of the Prompt Emission by IKAROS-GAP
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Yonetoku, D., primary, Murakami, T., additional, Sakashita, T., additional, Morihara, Y., additional, Kikuchi, Y., additional, Takahashi, T., additional, Gunji, S., additional, Mihara, T., additional, Kubo, S., additional, McEnery, J. E., additional, Racusin, J. L., additional, and Gehrels, N., additional
- Published
- 2011
- Full Text
- View/download PDF
6. Electron Bernstein wave heating and emission measurement through the very narrow O-X-B mode conversion window in the LHD.
- Author
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Igami, H., Kubo, S., Shimozuma, T., Yoshimur, Y., Takahashi, H., Nishiura, M., Ogasawara, S., Makino, R., Idei, H., Nagasaki, K., Seki, T., Osakabe, M., and Mutoh, T.
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PLASMA Bernstein waves , *PLASMA waves , *CYCLOTRONS , *PLASMA devices , *PLASMA engineering - Abstract
In the large helical device (LHD), the theoretically predicted width of the ordinary-extraordinary-electron Bernstein wave (O-X-B) mode conversion (MC) window is comparable to the beam width and the power deposition is located in the off-axis region if the 77GHz fundamental electron cyclotron (EC) wave of is launched from an existing horizontal port antenna. In the experiment, the actual MC window location was looked for with changing the aiming. The effective aiming with that the increase of the stored energy was observed was two degrees apart from the location of the theoretical MC window at a maximum. Measurement of the waves originated from the thermally emitted EBW and radiated via the B-X-O mode conversion process is effective to improve the accuracy of the theoretical prediction with comparison between the theoretical and the experimental results. The theoretical prediction suggests that the width of the MC window of the fundamental 77GHz EC wave can be expanded if the lower port antenna is used. On the other hand, the MC window of the second harmonic 154GHz EC wave is blocked by horizontal port wall if another horizontal port antenna is used. It is required to move the final mirror of the quasi-optical antenna toward the plasma surface. Focusing of the beam at the plasma cutoff is (PC) also necessary for the effective mode conversion. [ABSTRACT FROM AUTHOR]
- Published
- 2014
- Full Text
- View/download PDF
7. Extension of High Te Regime with Upgraded ECRH System in the LHD.
- Author
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Takahashi, H., Shimozuma, T., Kubo, S., Yoshimura, Y., Igami, H., Ito, S., Kobayashi, S., Mizuno, Y., Okada, K., Mutoh, T., Nagaoka, K., Murakami, S., Osakabe, M., Yamada, I., Nakano, H., Yokoyama, M., Ido, T., Shimizu, A., Seki, R., and Ida, K.
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PLASMA instabilities ,PLASMA heating ,GYROTRONS ,HIGH temperatures ,STELLARATORS ,ELECTRON transport ,ELECTRIC fields ,ELECTRON temperature - Abstract
Enhancement of the output powEr pEr gyrotron has been plann
e d in the Large Helical Device (LHD). Three 77-GHz gyrotrons with an output powEr of more than 1 MW have been opEraTe d. In addition, a high powEr gyrotron with the frequency of 154 GHz (1 MW/5 s, 0.5 MW/CW) was ne wly 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 exTe nded due to the upgraded ECRH sysTe m such as the central electron Te mpErature Te0 = 13.5 keV with ne = 1x1019 m-3 . In the LHD, an electron-inTe rnaltransport barriEr (e-ITB) relaTe d to the production of high Te plasmas has been realized by strongly centre-focused ECRH. The electron thErmal confine ment clearly improved inside the e-ITB. The radial electric field was measured using the heavy ion beam probe. The formation of the positive Er was obsErved in the core region, which well agreed with the prediction of the ne oclassical transport theory. The ene rgy confine ment characTe ristics have been investigaTe d in the ECRH plasmas. It was found that highEr plasma stored ene rgy and lowEr radiation powEr was realized in the outward configuration. The plasma stored ene rgy of 530 kJ with ne = 3.2x1019 m-3 , which is the 1.7 times largEr than the previous record in the ECRH plasma in the LHD, has been successfully achieved. [ABSTRACT FROM AUTHOR]- Published
- 2014
- Full Text
- View/download PDF
8. Development of steady-state operation using ICH in the LHD.
- Author
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Kasahara, H., Seki, T., Saito, K., Seki, R., Yoshimura, Y., Kubo, S., Shimozuma, T., Igami, H., Takahashi, H., Nagasaki, K., Ueda, Y., Tokitani, M., Ashikawa, N., Shoji, M., Wakatsuki, T., Kamio, S., Tsuchiya, H., Tanaka, H., Yoshimura, S., and Tamura, N.
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STEADY state conduction ,CYCLOTRONS ,ELECTRON cyclotron resonance heating ,ELECTRIC fields ,BOLOMETERS ,FUSION reactor divertors ,IONS ,ELECTRON temperature - Abstract
doi: Long-pulse discharge with the electron density n
e0 of 1 x 1019 m-3 , electron temperature Te0 of 2.5 keV, discharge length tdis of 19 minutes and heating power Pinject of 1MW, is demonstrated using the HAS antenna and the PA antenna for ion cyclotron heating (ICH) and increasing in the power of electron cyclotron heating (ECH). The HAS antenna is designed to phase dipole and excite ideal fast wave with parallel electric field kept small, and low impurity generation and accumulation are achieved on the steady-state discharge by weak parasitic heating around antennas. On the long-pulse discharge, the radiation measured by bolometer is kept smaller than 20% for injection power, and the heat load to divertor is approximately 60 % with low energetic particle losses. The heat load ratio to divertor is not as a function of injection power around 1MW, and energy confinement has been kept during the steady-state discharge. [ABSTRACT FROM AUTHOR]- Published
- 2014
- Full Text
- View/download PDF
9. Long Pulse ECH Plasma in LHD
- Author
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Kubo, S., primary
- Published
- 2005
- Full Text
- View/download PDF
10. Development of High-Power, Long-Pulse Gyrotrons and Its Application for High Electron Temperature, EBWH and ECCD Experiments on LHD.
- Author
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Yoshimura, Y., Kubo, S., Shimozuma, T., Igami, H., Takahashi, H., Nishiura, M., Ito, S., Kobayashi, S., Mizuno, Y., Okada, K., Takita, Y., Mutoh, T., Yamada, H., Komori, A., Kariya, T., Imai, T., Marushchenko, Nikolai B., and Turkin, Yuri
- Subjects
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GYROTRONS , *ELECTRON temperature , *PHYSICS experiments , *POWER resources , *FOCUSED ion beams , *ELECTRON distribution , *ELECTRIC heating , *ENERGY storage - Abstract
To sustain plasmas with higher parameters and with longer pulse duration in LHD, ECH system has been upgraded by introducing newly developed 77 GHz gyrotrons. The designed output power and operation duration time are over 1 MW for several seconds and 0.3 MW for continuous operation, respectively. Owing to the upgrade of gyrotrons and improved power supply operation procedure, total injection power of EC-waves to LHD increased up to 3.7 MW at the last LHD experimental campaign in 2010. Application of the high-power 77 GHz EC-waves of 3.4 MW as focused beams to the center of plasma with low line-average electron density of ∼0.2×1019 m-3 causes highly steep electron temperature profile and the central electron temperature reached up to 20 keV, which highly exceeds the former record of 15 keV. At higher density region of 1×1019 m-3, central electron temperature reached 8.6 keV. Additional electron Bernstein wave heatings, O-X-B and slow X-B heatings, using a 77 GHz ECH system caused clear increase in plasma stored energy even for the high-density plasmas over plasma cutoff (>7.35×1019 m-3) sustained with NBI. For the O-X-B scenario, the 77 GHz EC-wave was obliquely injected from low-field side in O-mode polarization, aiming at the point where high mode-conversion efficiency was expected. For realizing slow X-B scenario, new inner-vessel mirrors were installed in LHD just close to a helical coil, that is, at the high-field side (HFS) region. Using the inner-vessel mirror, X-mode waves were injected from HFS, showing evident increase in plasma stored energy. Oblique injection of long-pulse 0.77 MW/8 s 77 GHz wave with various N∥ clearly demonstrated ECCD in LHD. The EC-driven current changes its direction with the sign of N∥, and the highest EC-driven current reached up to 42 kA. [ABSTRACT FROM AUTHOR]
- Published
- 2011
- Full Text
- View/download PDF
11. Electron Cyclotron / Bernstein Wave Heating and Current Drive Experiments using Phased-array Antenna in QUEST.
- Author
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Idei, H., Zushi, H., Hanada, K., Nakamura, K., Fujisawa, A., Hasegawa, M., Yoshida, N., Sakamoto, M., Watanebe, H., Tokunaga, K., Nagashima, Y., Ejiri, A., Sakaguchi, M., Kalinnikova, E., Ishiguro, M., Tashima, S., Fukuyama, A., Igami, H., Kubo, S., and Sharma, S. K.
- Subjects
ELECTRON cyclotron resonance sources ,ELECTRIC heating ,ELECTROMAGNETIC waves ,PHYSICS experiments ,PHASED array antennas ,PLASMA injection ,PERFORMANCE evaluation ,ELECTRIC discharges - Abstract
The phased-array antenna system for Electron Cyclotron/Bernstein Wave Heating and Current Drive experiments has been developed in the QUEST. The antenna was designed to excite a pure O-mode wave in the oblique injection for the O-X-B mode conversion experiments, and its good performances were confirmed at a low power level. The plasma current (<∼15 kA) with an aspect ratio of 1.5 was started up and sustained by only RF injection in the low-density operations. The long pulse discharge of 10 kA was also attained for 37 s. The new density window to sustain the plasma current was observed in the high-density plasmas. The single-null divertor configuration with the high plasma current (<∼25 kA) was attained in the 17 s plasma sustainment. [ABSTRACT FROM AUTHOR]
- Published
- 2011
- Full Text
- View/download PDF
12. ECH Power Deposition Study in the Collisionless Plasma of LHD
- Author
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Kubo, S., primary
- Published
- 2003
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- View/download PDF
13. Optimization of Electron Cyclotron Heating in LHD
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Kubo, S., primary
- Published
- 2003
- Full Text
- View/download PDF
14. Activities on Realization of High-Power and Steady-State ECRH System and Achievement of High Performance Plasmas in LHD.
- Author
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Shimozuma, T., Kubo, S., Yoshimura, Y., Igami, H., Takahashi, H., Ikeda, R., Tamura, N., Kobayashi, S., Ito, S., Mizuno, Y., Takita, Y., Mutoh, T., Minami, R., Kariya, T., Imai, T., Idei, H., Shapiro, M. A., Temkin, R. J., Felici, F., and Goodman, T.
- Subjects
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ELECTRON cyclotron resonance sources , *HIGH-density plasmas , *HEATING , *GYROTRONS , *CONTROLLED fusion - Abstract
Electron Cyclotron Resonance Heating (ECRH) has contributed to the achievement of high performance plasma production, high electron temperature plasmas and sustainment of steady-state plasmas in the Large Helical Device (LHD). Our immediate targets of upgrading the ECRH system are 5 MW several seconds and 1 MW longer than one hour power injection into LHD. The improvement will greatly extend the plasma parameter regime. For that purpose, we have been promoting the development and installation of 77 GHz/1–1.5 MW/several seconds and 0.3 MW/CW gyrotrons in collaboration with University of Tsukuba. The transmission lines are re-examined and improved for high and CW power transmission. In the recent experimental campaign, two 77 GHz gyrotrons were operated. One more gyrotron, which was designed for 1.5 MW/2 s output, was constructed and is tested. We have been promoting to improve total ECRH efficiency for efficient gyrotron-power use and efficient plasma heating, e.g. a new waveguide alignment method and mode-content analysis and the feedback control of the injection polarization. In the last experimental campaign, the 77 GHz gyrotrons were used in combination with the existing 84 GHz range and 168 GHz gyrotrons. Multi-frequency ECRH system is more flexible in plasma heating experiments and diagnostics. A lot of experiments have been performed in relation to high electron temperature plasmas by realization of the core electron-root confinement (CERC), electron cyclotron current drive (ECCD), Electron Bernstein Wave heating, and steady-state plasma sustainment. Some of the experimental results are briefly described. [ABSTRACT FROM AUTHOR]
- Published
- 2009
- Full Text
- View/download PDF
15. Study of CERC using newly installed 77 GHz Gyrotron in LHD.
- Author
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Takahashi, H., Shimozuma, T., Yokoyama, M., Ido, T., Kubo, S., Shimizu, A., Yoshimura, Y., Igami, H., and Mutoh, T.
- Subjects
GYROTRONS ,ELECTROMAGNETIC fields ,ELECTRONS ,SPIRAL computed tomography ,MAGNETIC fields - Abstract
We have investigated the transition to Core Electron-Root Confinement (CERC) using the 77 GHz ECRH system, which was newly installed in the Large Helical Device (LHD). The focal point scan of the ECRH was carried out shot by shot in the same poloidal surface along the magnetic field of 2.75 T, which is the fundamental resonance surface for 77 GHz ECRH. The formation of the steep gradient in the electron temperature and the change of the radial electric field from negative to positive value in the plasma core region were observed by the ECRH injection to ρ<0.5. The foot point of the peaked profile of the electron temperature appeared near the m/n = 2/1 rational surface, which was located at ρ∼0.5. These results imply that localized ECRH in the inner region within the lower order rational surface and/or the electron heat flux across the rational surface play important roles for the transition to CERC. We also confirmed that the calculated radial electric field from a neoclassical theory qualitatively agreed with the experimental results. [ABSTRACT FROM AUTHOR]
- Published
- 2009
- Full Text
- View/download PDF
16. ECH experiments aiming at further advanced operations in LHD.
- Author
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Igami, H., Kubo, S., Shimozuma, T., Inagaki, S., Nagasaki, K., Tanaka, H., Yoshimura, Y., Notake, T., Maekawa, T., Uchida, M., Miyazawa, J., Yamada, I., Narihara, K., Tamura, N., Ida, K., Mutoh, T., and Komori, A.
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PARTICLES (Nuclear physics) , *MAGNETIC fields , *CONTROLLED fusion , *PLASMA confinement , *MAGNETICS - Abstract
In the Large helical device (LHD), super dense core (SDC) regime [1] and high electron temperature regime with formation of the electron internal transport barrier (e-ITB) [2][3] have been studied strenuously. Electron cyclotron heating (ECH) and current drive (ECCD) in such regimes can be powerful tools for heating and control of the plasma confinement. In this paper, recent progress of ECH experiments aiming at further advanced operation in these regimes is reported. Study of fundamental ECH by electron Bernstein waves (EBWs) has been required in the SDC regime. Early experimental results of EBW-ECH by so-called O-X-B and X-B method are introduced. In a newly realized enhanced magnetic field configuration, the highest central electron temperature over 10 keV was obtained in electron cyclotron resonance (ECR) discharges. ECCD will be very important in both of high density and high temperature regimes. It has been progressed with the optimization of microwave injection and magnetic field configuration. Progress of ECCD experiment is shortly introduced. [ABSTRACT FROM AUTHOR]
- Published
- 2007
- Full Text
- View/download PDF
17. Long Pulse Plasma Heating Experiment by Ion Cyclotron Heating in LHD.
- Author
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Seki, T., Mutoh, T., Kumazawa, R., Saito, K., Watari, T., Nakamura, Y., Sakamoto, M., Watanabe, T., Kubo, S., Shimozuma, T., Yoshimura, Y., Igami, H., Ohkubo, K., Takeiri, Y., Oka, Y., Tsumori, K., Osakabe, M., Ikeda, K., Nagaoka, K., and Kaneko, O.
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CYCLOTRONS ,PARTICLE accelerators ,PLASMA heating ,HYDROGEN ions ,MAGNETICS ,ELECTRIC discharges - Abstract
It is very important to demonstrate the ability to sustain the plasma in a steady state on the Large Helical Device (LHD), which has external helical magnetic coils and is a superconducting device. The long pulse discharge experiment was carried out using the ion cyclotron range of frequencies (ICRF) heating mainly. The plasma discharge of 31 minutes and 45 seconds was achieved by a total injected heating energy of 1.3GJ. Swing of the magnetic axis to scatter the local heat load on the divertor plate was one of the key methods for the steady state operation. The repetitive hydrogen pellet injection was tried successfully to fuel the minority hydrogen ions for long pulse operation. © 2005 American Institute of Physics [ABSTRACT FROM AUTHOR]
- Published
- 2005
- Full Text
- View/download PDF
18. RF experiments in LHD
- Author
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Kubo, S., primary, Kumazawa, R., additional, Shimozuma, T., additional, Idei, H., additional, Yoshimura, Y., additional, Sato, M., additional, Mutoh, T., additional, Seki, T., additional, Watari, T., additional, Ohkubo, K., additional, Saito, K., additional, Takita, Y., additional, Kobayashi, S., additional, Ito, S., additional, Mizuno, Y., additional, Shinpo, F., additional, Nomura, G., additional, Kaneko, O., additional, Komori, A., additional, Yamada, H., additional, Ohyabu, N., additional, Kawahata, K., additional, Akaishi, K., additional, Emoto, M., additional, Funaba, H., additional, Goto, M., additional, Hamada, Y., additional, Ida, K., additional, Inagaki, S., additional, Inoue, N., additional, Kado, S., additional, Masuzaki, S., additional, Minami, T., additional, Miyazawa, J., additional, Morisaki, T., additional, Morita, S., additional, Murakami, S., additional, Mutoh, S., additional, Nagayama, Y., additional, Nakamura, Y., additional, Nakanishi, H., additional, Narihara, K., additional, Nishimura, K., additional, Noda, N., additional, Kobuchi, T., additional, Ohdachi, S., additional, Oka, Y., additional, Osakabe, M., additional, Ozaki, T., additional, Peterson, B. J., additional, Sagara, A., additional, Sakakibara, S., additional, Sakamoto, R., additional, Sasao, H., additional, Sasao, M., additional, Sato, K., additional, Shoji, M., additional, Sudo, S., additional, Suzuki, H., additional, Takeiri, T., additional, Tanaka, K., additional, Toi, K., additional, Tokuzawa, T., additional, Tsumori, K., additional, Tsuzuki, K., additional, Yamada, I., additional, Yamaguchi, S., additional, Yamazaki, K., additional, Yokoyama, M., additional, Watanabe, K. Y., additional, Motojima, O., additional, Fujiwara, M., additional, and Iiyoshi, A., additional
- Published
- 1999
- Full Text
- View/download PDF
19. Initial ICRF heating experiments on the LHD
- Author
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Kumazawa, R., primary, Mutoh, T., additional, Seki, T., additional, Saito, K., additional, Shimpo, F., additional, Nomura, G., additional, Ido, T., additional, Watari, T., additional, Cattanei, G., additional, Jikang, Xie, additional, Okada, H., additional, Ohkubo, K., additional, Sato, M., additional, Kubo, S, additional, Shimozuma, T., additional, Idei, H., additional, Yoshimura, Y., additional, Kaneko, O., additional, Takeiri, Y., additional, Oka, Y., additional, Tsumori, K., additional, Osakabe, M., additional, Ohyabu, N., additional, Kawahata, K., additional, Komori, A., additional, Yamada, H., additional, Akaishi, K., additional, Emoto, M., additional, Funaba, H., additional, Goto, M., additional, Hamada, Y., additional, Ida, K., additional, Inagaki, S., additional, Inoue, N., additional, Kado, S., additional, Masuzaki, S., additional, Minami, T., additional, Miyazawa, J., additional, Morisaki, T., additional, Morita, S., additional, Murakami, S., additional, Muto, S., additional, Nagayama, Y., additional, Nakamura, Y., additional, Nakanishi, H., additional, Narihara, K., additional, Nishimura, K., additional, Noda, N., additional, Kobuchi, T., additional, Ohdachi, S., additional, Ozaki, T., additional, Peterson, B. J., additional, Sagara, A., additional, Sasakibara, S., additional, Sakamoto, R., additional, Sasao, H., additional, Sasao, M., additional, Sato, K., additional, Shoji, M., additional, Sudo, S., additional, Suzuki, H., additional, Tanaka, K., additional, Toi, K., additional, Tokuzawa, T., additional, Tsuzuki, K., additional, Yamada, I., additional, Yamaguchi, S., additional, Yokoyama, M., additional, Watanabe, K. Y., additional, Motojima, O., additional, Fujiwara, M., additional, and Iiyoshi, A., additional
- Published
- 1999
- Full Text
- View/download PDF
20. RF heating experiments in CHS and RF development for LHD
- Author
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Watari, T., primary, Kumazawa, R., additional, Nishimura, K., additional, Mutoh, T., additional, Seki, T., additional, Masuda, S., additional, Shoji, T., additional, Simbo, F., additional, Ido, T., additional, Akiyama, R., additional, Ando, A., additional, Ejiri, A., additional, Fujisawa, A., additional, Idei, H., additional, Ida, K., additional, Iguchi, H., additional, Isobe, M., additional, Iwase, M., additional, Kubo, S., additional, Minami, T., additional, Matsuoka, K., additional, Morisaki, T., additional, Morita, S., additional, Mutoh, S., additional, Murakami, S., additional, Narihara, K., additional, Okamura, S., additional, Ozaki, T., additional, Sasao, M., additional, Takahashi, C., additional, Kawamoto, T., additional, Tanaka, K., additional, Xu, J., additional, Noterdaeme, J. M., additional, Rasmussen, D. A., additional, Lyon, J. F., additional, Wilgen, J. B., additional, Greenwood, D. E., additional, Hoffman, D. J., additional, Jaeger, E. F., additional, and Murakami, M., additional
- Published
- 1997
- Full Text
- View/download PDF
21. High power local ECH in CHS
- Author
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Kubo, S., primary, Idei, H., additional, Iwase, M., additional, Ohkubo, K., additional, Minami, T., additional, Yamada, I., additional, Narihara, K., additional, Tanaka, K., additional, Wilgen, J. B., additional, Murakami, M., additional, Rasumussen, D. A., additional, Nishimura, K., additional, Okamura, S., additional, and Matsuoka, K., additional
- Published
- 1996
- Full Text
- View/download PDF
22. Confinement Studies with ECH Plasmas in ATF
- Author
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Murakami, M., primary, Bigelow, T. S., additional, Goldfinger, R. C., additional, Wilgen, J. B., additional, Baylor, L. R., additional, Rasmussen, D. A., additional, England, A. C., additional, Aceto, S., additional, Baity, F. W., additional, Batchelor, D. B., additional, Bell, G. L., additional, Bell, J. D., additional, Carreras, B. A., additional, Colchin, R. J., additional, Crume, E. C., additional, Dominguez, N., additional, Dory, R. A., additional, Dunlap, J. L., additional, Dyer, G. R., additional, Fowler, R. H., additional, Gandy, R. F., additional, Glowienka, J. C., additional, Goulding, R. H., additional, Hanson, G. R., additional, Harris, J. H., additional, Hiroe, S., additional, Hoffman, D. J., additional, Horton, L. D., additional, Howe, H. C., additional, Hutchinson, D. P., additional, Isler, R. C., additional, Jernigan, T. C., additional, Kaneko, H., additional, Kubo, S., additional, Kwon, M., additional, Langley, R. AL., additional, Lee, D. K., additional, Likin, K. M., additional, Lyon, J. F., additional, Ma, C. H., additional, Morita, S., additional, Ochando, M. A., additional, Okada, H., additional, Paul, S. F., additional, Qualls, A. L., additional, Rome, J. A., additional, Sapozhnikov, A. V., additional, Sarksyan, K. A., additional, Sato, M., additional, Schwelberger, J. G., additional, Shats, M. G., additional, Shepard, T. D., additional, Simpkins, J. E., additional, Thomas, C. E., additional, Uckan, T., additional, Vander Sluis, K. L., additional, Wade, M. R., additional, Wing, W. R., additional, and Zielinski, J. J., additional
- Published
- 1992
- Full Text
- View/download PDF
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