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Dive into the research topics where C. Takahashi is active.

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Featured researches published by C. Takahashi.


Fusion Technology | 1990

Compact Helical System physics and engineering design

K. Nishimura; K. Matsuoka; Masami Fujiwara; K. Yamazaki; Jiro Todoroki; T. Kamimura; Tsuneo Amano; Heiji Sanuki; S. Okamura; M. Hosokawa; H. Yamada; S. Tanahashi; Shin Kubo; Y. Takita; Tatsuo Shoji; O. Kaneko; Harukazu Iguchi; C. Takahashi

This paper reports on the Compact Helical System designed for research on transport in a low-aspect-ratio helical system. The machine parameters were chosen on the basis of a physics optimization study. Considerable effort was devoted to reducing error fields from current feeds and crossovers. The final machine parameters are as follows: major radius of 1 m; minor radius of the helical field coil of 0.313 m; plasma aspect ratio A{sub p} = 5; pole number and toroidal period number of the helical field coil of l = 2 and m = 8, respectively; and helical pitch modulation of {alpha}{sup *} = 0.3.


Physics of Plasmas | 2000

Experimental study of the bifurcation nature of the electrostatic potential of a toroidal helical plasma

A. Fujisawa; H. Iguchi; T. Minami; Y. Yoshimura; Kenji Tanaka; K. Itoh; H. Sanuki; S. Lee; M. Kojima; S.-I. Itoh; M. Yokoyama; S. Kado; S. Okamura; R. Akiyama; K. Ida; M. Isobe; S. Nishimura; M. Osakabe; I. Nomura; A. Shimizu; C. Takahashi; K. Toi; K. Matsuoka; Y. Hamada; M. Fujiwara

The bifurcation nature of the electrostatic structure is studied in the toroidal helical plasma of the Compact Helical System (CHS) [K. Matsuoka et al., Proceedings of the 12th International Conference on Plasma Physics and Controlled Nuclear Fusion Research, Nice, 1988 (International Atomic Energy Agency, Vienna, 1989), Vol. 2, p. 411]. Observation of bifurcation-related phenomena is introduced, such as characteristic patterns of discrete potential profiles, and various patterns of self-sustained oscillations termed electric pulsation. Some patterns of the electrostatic structure are found to be quite important for fusion application owing to their association with transport barrier formation. It is confirmed, as is shown in several tokamak experiments, that the thermal transport barrier is linked with electrostatic structure through the radial electric field shear that can reduce the fluctuation resulting in anomalous transport. This article describes in detail spatio-temporal evolution during self-sust...


Nuclear Fusion | 1999

Confinement physics study in a small low aspect ratio helical device: CHS

S. Okamura; K. Matsuoka; R. Akiyama; D. S. Darrow; A. Ejiri; A. Fujisawa; M. Fujiwara; M. Goto; K. Ida; H. Idei; H. Iguchi; N. Inoue; M. Isobe; K. Itoh; S. Kado; K. Khlopenkov; T. Kondo; S. Kubo; A. Lazaros; S. Lee; G. Matsunaga; T. Minami; S. Morita; S. Murakami; Noriyoshi Nakajima; N. Nikai; S. Nishimura; I. Nomura; S. Ohdachi; K. Ohkuni

Variation of the plasma position relative to the centre of the helical coil winding is a very effective means of controlling the MHD stability and the trapped particle confinement in heliotron/torsatron systems, but improving one of these two characteristics with this parameter simultaneously has a detrimental effect on the other. The inward shifted configuration is favourable for drift orbit optimization but is predicted to be unstable according to the Mercier criterion. Various physics problems, such as electric field structure, plasma rotation and MHD phenomena, have been studied in the Compact Helical System (CHS) with a compromise intermediate position. With this standard configuration, CHS has yielded experimental results that contribute to the understanding of general toroidal confinement physics and low aspect ratio helical systems. In the recent experiments, it was found that a wide range of inward shifted configurations give stable plasma discharges without any restriction to the special pressure profile. Such an enhanced range of operation made it possible to study experimentally the drift orbit optimized configuration in heliotron/torsatron systems. The effect of configuration improvement was studied with plasmas in a low collisionality regime.


Nuclear Fusion | 2007

Steady-state operation and high energy particle production of MeV energy in the Large Helical Device

T. Mutoh; R. Kumazawa; T. Seki; K. Saito; H. Kasahara; Y. Nakamura; S. Masuzaki; S. Kubo; Y. Takeiri; T. Shimozuma; Y. Yoshimura; H. Igami; T. Watanabe; H. Ogawa; J. Miyazawa; M. Shoji; N. Ashikawa; K. Nishimura; M. Osakabe; K. Tsumori; K. Ikeda; K. Nagaoka; Y. Oka; H. Chikaraishi; H. Funaba; S. Morita; M. Goto; S. Inagaki; K. Narihara; T. Tokuzawa

Achieving steady-state plasma operation at high plasma temperatures is one of the important goals of worldwide magnetic fusion research. High temperatures of approximately 1?2?keV, and steady-state plasma sustainment operations have been reported. Recently the steady-state operation regime was greatly extended in the Large Helical Device (LHD). A high-temperature plasma was created and maintained for 54?min with 1.6?GJ in the 2005FY experimental programme. The three-dimensional heat-deposition profile of the LHD helical divertor was modified, and during long-pulse discharges it effectively dispersed the heat load using a magnetic axis swing technique developed at the LHD. A sweep of only 3?cm in the major radius of the magnetic axis position (less than 1% of the major radius of the LHD) was enough to disperse the divertor heat load. The steady-state plasma was heated and sustained mainly by hydrogen minority ion heating using ion cyclotron range of frequencies and partially by electron cyclotron of fundamental resonance frequency. By accumulating the small flux of charge-exchanged neutral particles during the long-pulse operation, a high energy ion tail which extended up to 1.6?MeV was observed. This is the first experimental evidence of high energetic ion confinement of MeV range in helical devices. The long-pulse operations lasted until a sudden increase in radiation loss occurred, presumably because of metal wall flakes dropping into the plasma. The sustained line-averaged electron density and temperature were approximately 0.8 ? 1019?m?3 and 2?keV, respectively, at a 1.3?GJ discharge (#53776) and 0.4 ? 1019?m?3 and 1?keV at a 1.6?GJ discharge (#66053). The average input power was 680?kW and 490?kW, and the plasma duration was 32?min and 54?min, respectively. These successful long operations show that the heliotron configuration has a high potential as a steady-state fusion reactor.


Nuclear Fusion | 1995

High beta discharges with neutral beam injection in CHS

S. Okamura; K. Matsuoka; K. Nishimura; K. Tsumori; R. Akiyama; S. Sakakibara; H. Yamada; S. Morita; T. Morisaki; Noriyoshi Nakajima; Kenji Tanaka; J. Xu; K. Ida; H. Iguchi; A. Lazaros; T. Ozaki; Hideki Arimoto; A. Ejiri; M. Fujiwara; H. Idei; O. Kaneko; K. Kawahata; T. Kawamoto; A. Komori; S. Kubo; O. Motojima; V.D. Pustovitov; C. Takahashi; K. Toi; I. Yamada

High beta plasmas with a volume averaged equilibrium beta value of 2.1% were produced in CHS using tangential neutral beam injection. This beta value was achieved with the confinement improvement (reheat mode) observed after turning off strong gas puffing. Wall conditioning with titanium gettering was used to make high density operation (ne ? 8 ? 1019 m-3) possible for low magnetic fields (Bt = 0.6 T). The discharges start with the magnetic hill configuration (in vacuum) and finally achieve Mercier stable equilibrium owing to the self-stabilization effect given by the magnetic well which is produced by the plasma pressure. The Shafranov shift was about 40% of a plasma minor radius. Magnetic fluctuations did not increase with increasing plasma pressure when the beta value exceeded 1%. Dynamic poloidal field control was applied to suppress the outward plasma shift with increasing plasma pressure. Such operation gave an additional increase of beta value compared with the constant poloidal field operation


Nuclear Fusion | 1992

Shafranov shift in the low aspect ratio heliotron/torsatron Compact Helical System

H. Yamada; K. Ida; H. Iguchi; S. Morita; O. Kaneko; Hideki Arimoto; M. Hosokawa; H. Idei; S. Kubo; K. Matsuoka; K. Nishimura; S. Okamura; Yasuhiko Takeiri; Y. Takita; C. Takahashi; K. Hanatani; H.C. Howe; S.P. Hirshman; D.K. Lee

The MHD equilibrium properties of neutral beam heated plasmas have been experimentally investigated in the Compact Helical System (CHS)-a low aspect ratio (Ap ~ 5) heliotron/torsatron. This configuration is characterized by a strong breaking of helical symmetry. The radial profiles measured by various diagnostics have shown a significant Shafranov shift due to the plasma pressure. The deviation of the magnetic axis from is vacuum position has become as large as 50% of the minor radius. When the three-dimensional equilibrium code VMEC is used to reconstruct the equilibrium from the experimental data, the result is in good agreement with the experimentally observed Shafranov shift as well as with the diamagnetic pressure in plasmas with β ≤ 1.2% and β0 ≤ 3.3%. This beta values corresponds to half of the conventional equilibrium β limit defined by the Shafranov shift reaching a value of half of the minor radius. Although tangential neutral beam injection causes pressure anisotropies, p||/p⊥ ≤ 3, the description of the equilibrium assuming isotropic pressure is consistent with the experiment


Journal of the Physical Society of Japan | 2007

Causal Relationship between Zonal Flow and Turbulence in a Toroidal Plasma

A. Fujisawa; Akihiro Shimizu; Haruhisa Nakano; S. Ohshima; K. Itoh; Y. Nagashima; S.-I. Itoh; Harukazu Iguchi; Yasuo Yoshimura; Takashi Minami; Keiichi Nagaoka; C. Takahashi; M. Kojima; Shin Nishimura; M. Isobe; C. Suzuki; T. Akiyama; Takeshi Ido; K. Matsuoka; S. Okamura; P. H. Diamond

Electric field fluctuations are directly measured using twin heavy-ion-beam probes in Compact Helical System. The spectrum of the electric field fluctuation reveals the existence of a zonal flow at a frequency of less than 1 kHz, coherent modes with a long correlation length (conjectured as geodesic acoustic modes), and background turbulence. Analyses using a wavelet elucidate nonlinear interactions between these fluctuation components in disparate scales. The highlighted findings are that the turbulent fluctuations should be modulated in response to the direction of zonal flow, and should be suppressed, on average, by the zonal flow. This is the first observation that demonstrates the causal linkage between zonal flow and turbulence in toroidal plasmas at a high temperature.


Nuclear Fusion | 1999

Plasma confinement studies in LHD

M. Fujiwara; H. Yamada; A. Ejiri; M. Emoto; H. Funaba; M. Goto; K. Ida; H. Idei; S. Inagaki; S. Kado; O. Kaneko; K. Kawahata; T. Kobuchi; A. Komori; S. Kubo; R. Kumazawa; S. Masuzaki; T. Minami; J. Miyazawa; T. Morisaki; S. Morita; S. Murakami; S. Muto; T. Mutoh; Y. Nagayama; Y. Nakamura; H. Nakanishi; K. Narihara; K. Nishimura; N. Noda

The initial experiments on the Large Helical Device (LHD) have extended confinement studies on currentless plasmas to a large scale (R = 3.9 m, a = 0.6 m). Heating by NBI of 3 MW produced plasmas with a fusion triple product of 8 × 1018m-3keVs at a magnetic field strength of 1.5 T. An electron temperature of 1.5 keV and an ion temperature of 1.1 keV were achieved simultaneously at a line averaged electron density of 1.5 × 1019 m-3. The maximum stored energy reached 0.22 MJ with neither unexpected confinement deterioration nor visible MHD instabilities, which corresponds to β = 0.7%. Energy confinement times reached a maximum of 0.17 s. A favourable dependence of energy confinement time on density remains in the present power density (~40 kW/m3) and electron density (3 × 1019 m-3) regimes, unlike the L mode in tokamaks. Although power degradation and significant density dependence are similar to the conditions on existing medium sized helical devices, the absolute value is enhanced by up to about 50% from the International Stellarator Scaling 95. Temperatures of both electrons and ions as high as 200 eV were observed at the outermost flux surface, which indicates a qualitative jump in performance compared with that of helical devices to date. Spontaneously generated toroidal currents indicate agreement with the physical picture of neoclassical bootstrap currents. Change of magnetic configuration due to the finite β effect was well described by 3-D MHD equilibrium analysis. A density pump-out phenomenon was observed in hydrogen discharges, which was mitigated in helium discharges with high recycling.


Physics of Plasmas | 2008

Experimental studies of zonal flow and field in compact helical system plasma

A. Fujisawa; K. Itoh; A. Shimizu; H. Nakano; S. Ohshima; H. Iguchi; K. Matsuoka; S. Okamura; T. Minami; Y. Yoshimura; K. Nagaoka; K. Ida; K. Toi; C. Takahashi; M. Kojima; S. Nishimura; M. Isobe; C. Suzuki; T. Akiyama; T. Ido; Y. Nagashima; S.-I. Itoh; P. H. Diamond

The experimental studies on zonal flows and turbulence have been carried out in Compact Helical System [K. Matsuoka, S. Kubo, M. Hosokawa et al., in Plasma Physics and Controlled Nuclear Fusion Research, Proc. 12th Int. Conf., Nice, 1988 (International Atomic Energy Agency, Vienna, 1989, Vol. 2, p. 411] using twin heavy ion beam probes. The paper presents the experimental observations of stationary zonal flow, nonlinear couplings between zonal flow and turbulence, and the role of zonal flow in the improved confinement, together with the recent discovery of zonal magnetic field. The presented experimental results strongly support the new paradigm that the plasma transport should be considered as a system of drift wave and zonal flows, and provides the first direct evidence for turbulence dynamo that the structured magnetic field can be really generated by turbulence.


Nuclear Fusion | 2004

Increased understanding of neoclassical internal transport barriers in CHS

T. Minami; A. Fujisawa; H. Iguchi; Y. Liang; K. Ida; S. Nishimura; M. Yokoyama; S. Murakami; Y. Yoshimura; M. Isobe; C. Suzuki; I. Nomura; K. Toi; M. Yoshinuma; A. Shimizu; C. Takahashi; K. Matsuoka; S. Okamura

We report recent progress in the study of neoclassical internal transport barriers (N-ITBs) in the compact helical system (CHS) experiment. N-ITBs have been observed in electron cyclotron (EC) heated NBI plasmas. The improved confinement region for electrons is expanded compared with that of previous N-ITB plasmas heated by only EC heating. Moreover, the ion temperature is found to be increased simultaneously by two to three times (Ti(0) ~ 400–500 eV), with a steep gradient region at ρ ~ 0.6. From measurement of the averaged peak energy intensity using a soft x-ray CCD camera, it is confirmed that the impurity confinement is also improved with N-ITBs. The radial electric field is observed to bifurcate into ion and electron root (Er ~ 15 kV m−1), and a rather large electric field shear (dEr/dr ~ −300 kV m−2) is produced in the layer between ion and electron root.

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Y. Yoshimura

Graduate University for Advanced Studies

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K. Toi

Instituto de Salud Carlos III

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