K. Arakawa M.-C. Marinica S. Fitzgerald L. Proville D. Nguyen-Manh S. L. Dudarev P.-W. Ma T. D. Swinburne A. M. Goryaeva T. Yamada T. Amino S. Arai Y. Yamamoto K. Higuchi N. Tanaka H. Yasuda T. Yasuda H. Mori
The diffusion of defects in crystalline materials governs macroscopic behaviour in a wide range of processes, including alloying, precipitation, phase transformation, and creep. In real materials, intrinsic defects are unavoidably bound to static trapping centres such as impurity atoms, meaning that their diffusion is controlled by the de-trapping …
PublishedK. Arakawa M. Marinica S. Fitzgerald L. Proville D. Nguyen-Manh S.L Dudarev P. Wai Ma T.D Swinburne T. Yamada T. Amino S. Arai Y. Yamamoto K. Higuchi N. Tanaka H. Yasuda T. Yasuda H. Mori
Quantum dynamics within solids is usually restricted to low mass particles such as electrons and muons, or single atoms of light elements such as hydrogen. In this letter we report observation of the quantum-assisted motion of self-interstitial atom clusters in tungsten (each of mass 184 Da), travelling distances of several nanometres between trapp…
PreprintV.F. Shevchenko Y.F. Baranov T. Bigelow J.B. Caughman S. Diem C. Dukes P. Finburg J. Hawes C. Gurl J.Griffiths J. Mailloux M. Peng A.N. Saveliev Y. TakaHe H. Tanaka G. Taylor
Start-up technique reported here relies on a double mode conversion (MC) for electron Bernstein wave (EBW) excitation. It consists of MC of the ordinary (0) mode, entering the plasma from the low field side of the tokamak, into the extraordinary (X) mode at a mirror-polarizer located at the high field side. The X mode propagates back to the plasma,…
Preprint PublishedT. Akiyama K. Kawahata K. Tanaka T. Tokuzawa Y. Ito S. Okajima K. Nakayama C. A. Michael L. N. Vyacheslavov A. Sanin S. Tsuji-Iio LHD Experiment Group
This paper describes the interferometer systems on the Large Helical Device (LHD). LHD is equipped with five interferometer systems, each of which has a different operational purpose and measurable electron density range. A single-channel millimeter-wave interferometer is mainly used for low-density plasmas along a horizontal line of sight on the e…
PublishedT. Tokuzawa K. Kawahata Y. Nagayama S. Inagaki P. C. De Vries A. Mase Y. Kogi Y. Yokota H. Hojo K. Tanaka A. Ejiri R. O. Pavlichenko S. Yamaguchi T. Yoshinaga D. Kuwahara Z. Shi H. Tsuchiya Y. Ito S. Hirokura S. Sudo A. Komori Lhd
Several types of microwave diagnostics, in the category of electron cyclotron emission (ECE) spectroscopy and reflectometry, have been developed on the Large Helical Device (LHD). Since LHD has a complicated magnetic configuration, the polarization effects have been studied for optimization of the microwave passive and active diagnostics. It was fo…
PublishedK. Tanaka K. Kawahata T. Tokuzawa T. Akiyama M. Yokoyama M. Shoji C. A. Michael L. N. Vyacheslavov S. Murakami A. Wakasa A. Mishchenko K. Muraoka S. Okajima H. Takenaga Lhd Experiment Group
Particle confinement processes are studied in detail on the Large Helical Device (LHD). Diffusion coefficients (D) and convection velocities (V) are estimated from density modulation experiments. The magnetic configuration and collisionality are widely scanned in order to investigate parameter dependences of D and V. To study the effect of the magn…
PublishedS. Shiraiwa S. Ide S. Itoh O. Mitarai O. Naito T. Ozeki Y. Sakamoto T. Suzuki Y. Takase S. Tanaka T. Taniguchi M. Aramasu T. Fujita T. Fukuda X. Gao M. Gryaznevich K. Hanada E. Jotaki Y. Kamada T. Maekawa Y. Miura K. Nakamura T. Nish
A new operational scenario of advanced tokamak formation was demonstrated in the JT-60U tokamak. This was accomplished by electron cyclotron and lower hybrid waves, neutral beam injection, and the loop voltage supplied by the vertical field and shaping coils. The Ohmic heating (OH) solenoid was not used but a small inboard coil (part of the shaping…
Published