H-mode and recycling control in JFT-2M

Sengoku, S.; Aikawa, Hiroshi; Funahashi, A.; Hasegawa, Mitsuru; Hoshino, Kazuo; Kasai, S.; Kawakami, T.; Kawashima, H.; Kondoh, T.; Maeda, Hideaki; Matoba, T.; Matsuda, Toshiaki; Matsumoto, Hiroshi; Miura, Y.; Mori, Masahiro; Nakazawa, I.; Odajima, K.; Ogawa, Hideyuki; Ogawa, T.; Ohasa, K.; Ohtsuka, Hokuto; Shoji, T.; Suzuki, Norio; Tamai, Hiroshi; Uesugi, Yoshihiko; Yamamoto, T.; Yamauchi, Toshihiko; Hamano, Tomoyuki; Hasegawa, Kouichi; Honda, A.; Ishibori, I.; Kashiwa, Y.; Kazawa, M.; Kikuchi, Kazuo; Matsuzaki, Y.; Ohuchi, Kinji; Okano, F.; Shibata, Takemasa; Shibuya, Takehisa; Shiina, T.; Suzuki, Kazuya; Suzuki, Shingo; Tani, Tadaaki; Tokutake, T.; Uno, S.; Yokoyama, Kenji

doi:10.1016/0022-3115(90)90029-m

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Cited by 13 publications

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“…The initial experiments have shown that the operational domain at H 98y2 = 1 is significantly reduced with the JET ITER-like wall (JET-ILW) mainly because of the need to inject large amount of gas (above 10 22 D s −1 ) to control core radiation mostly due to W, as also observed in ASDEX Upgrade [2]. It is well known that gas fuelling can impact on confinement as observed in carbon and metallic devices in both L-mode [3] and H-modes [4]. In JET-ILW however, detailed kinetic studies [5] have also pointed out that the pedestal confinement is impacted independently from the gas injection used in the experiments for both baseline H-modes (β N ~ 1.8) and improved H-mode or hybrid scenario (β N ~ 3).…”

Section: Introductionmentioning

confidence: 99%