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RECENT PROGRESS IN JT-60 EXPERIMENTS JT-60 TEAM (Presented by H. Kishimoto) <strong>IAEA</strong>-CN-50/A-I-4 H. AIKAWA, N. AKAOKA, H. AKASAKA, M. AKIBA, N. AKINO, T. ANDO, K. ANNOH, I. AOKI, T. AOYAGI, T. ARAI, K. ARAKAWA, M. ARAKI, M. AZUMI, S. CHIBA, M. DA1RAKU, N. EBISAWA, T. FUJII, T. FUKUDA, A. FUNAHASHI, H. FURUKAWA, H. GUNJI 1 , K. HAMAMATSU, M. HANADA, M. HARA, K. HARAGUCHI, H. HIRATSUKA, T. HIRAYAMA, S. HIROKI, K. HIRUTA, M. HONDA, M. HONDA, H. HOREKE, R. HOSODA, N. HOSOGANE, K. IIDA, T. miMA, Y. IKEDA, Y. IKEDA, T. IMAI, T. INOUE, N. ISAJI, M. ISAKA, S. ISHIDA, K. ITAMI, N. ITIGE, T. ITO, T. KAKIZAKI, Y. KAMADA, A. KAMINAGA, T. KANEKO 1 , T. KATO, M. KAWAI, M. KAWABE, Y. KAWAMATA, Y. KAWANO, K. KAWASAKI, K. KIKUCHI, M. KIKUCHI, H. KIMURA, T. KIMURA, H. KISHIMOTO, S. KITAMURA, A. KITSUNEZAKI, K. KIYONO, N. KOBAYASHI, K. KODAMA, Y. KOIDE, T. KOIKE, M. KOMATA, I. KONDO, K. KONISHI 1 , S. KONOSHIMA, H. KUBO, S. KUNIEDA, K. KURIHARA, M. KURIYAMA, T. KUSHIMA, M. KUSAKA, Y. KUSAMA, Y. MABUTI, S. MAEHARA, K. MAENO, T. MATOBA, S. MATSUDA, M. MATSUKAWA, T. MATSUKAWA, M. MATSUOKA, Y. MATSUZAKI, Y. MIURA, N. MIYA, K. MIYACHI, Y. MIYO, M. MIZUNO, K. MOGAKI, M. MORI, S. MORIYAMA, M. MUTO, M. NAGAMI, K. NAGASE, A. NAGASHIMA, K. NAGASHIMA, T. NAGASHIMA, S. NAGAYA, O. NAITO, H. NAKAMURA, Y. NAKAMURA, M. NEMOTO, Y. NEYATANI, H. NINOMIYA, N. NISHINO, T. NISHITANI, H. NOBUSAKA, H. NOMOTO, K. OBARA, H. OBINATA 2 , K. ODAZIMA, Y. OGAWA, N. OGIWARA, T. OHGA, Y. OHARA, K. OHASA, H. OOHARA, T. OHSHIMA, M. OHKUBO, K. OHTA, M. OHTA, S. OHUCHI, Y. OHUCHI, A. OIKAWA, Y. OKUMURA, K. OMORI, S. OMORI, Y. OMORI, T. OZEKI, M. SAEGUSA, N. SAITOH, K. SAKAMOTO, A. SAKASAI, S. SAKATA, T. SASAJIMA, K. SATOU, M. SATOU, M. SATOU, M. SAWAHATA, T. SEBATA 1 , M. SEIMIYA, M. SEKI, S. SEKI, K. SHIBANUMA, R. SHIMADA, T. SHIMADA 1 , K. SHIMIZU, M. SHIMIZU, Y. SHIMOMURA, S. SHINOZAKI, H. SHIRAI, H. SHIRAKATA, M. SHITOMI, K. SUGANUMA, T. SUGAWARA, T. SUGIE, H. SUNAOSHI, K. SUZUKI, M. SUZUKI, N. SUZUKI, S. SUZUKI, Y. SUZUKI, H. TACHIBANA, M. TAKAHASHI, S. TAKAHASHI, T. TAKAHASHI, M. TAKASAKI, H. TAKATSU, H. TAKEUCHI, A. TAKESHITA, T. TAKIZUKA, S. TAMURA, S. TANAKA, 67
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The cover picture shows the inside
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AFGHANISTAN ALBANIA ALGERIA ARGENTI
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PLASMA PHYSICS AND CONTROLLED NUCLE
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EDITORIAL NOTE The Proceedings have
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A. Kaminaga, T. Kaneko, T. Kato, M.
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Improved confinement regimes with O
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Tokamak with strong magnetic field
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Resonant island divertor experiment
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Particle removal capabilities of th
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Inside launch electron cyclotron he
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T. Hjima, S. Ishida, K. Itami, T. I
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T. Yamauchi, I. Nakazawa, K. Hasega
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ARTSIMOVICH MEMORIAL LECTURE C. MAI
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IAEA-CN-50/A-0 5 ceptible to fast r
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IAEA-CN-50/A-0 7 fusion power plant
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FIRST EXPERIMENTS IN TORE SUPRA EQU
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IAEA-CN-50/A-I-1 11 Supra is the fi
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IAEA-CN-50/A-I-1 13 poloidal field
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Page 53 and 54: IAEA-CN-50/A-I-2 AN OVERVIEW OF TFT
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Page 67 and 68: LATEST JET RESULTS AND FUTURE PROSP
Page 69 and 70: Parameter Plasma major radius (Ro)
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Page 73 and 74: IAEA-CN-50/A-I-3 47 3.0 3.5 Major r
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Page 77 and 78: IAEA-CN-50/A-I-3 51 Magnetic measur
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Page 87 and 88: IAEA-CN-50/A-I-3 61 where V is the
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Page 95 and 96: 1. INTRODUCTION IAEA-CN-50/A-I-4 69
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Page 107: IAEA-CN-50/A-I-4 81 REFERENCES [1]
Page 110 and 111: 84 STRAIT et al. sequence having mo
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Page 127 and 128: IAEA-CN-50/A-II-2 101 FIG. 2. Soft
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116 NINOMIYA et al. Limiter Diverto
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118 NINOMIYA et al. 2.4 2.2 2.0 1.8
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DISRUPTION MODES AND SAWTOOTH ANALY
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IAEA-CN-50/A-II-4 123 FIG. 1. Hugil
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IAEA-CN-50/A-II-4 125 decreases sig
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0.25 0.15 IAEA-CN-50/A-H-4 127 0.2
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IAEA-CN-50/A-II-4 129 [5] QIN, Yunw
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132 (V) 4.0 1.0 (a) HT-6M GROUP rat
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134 HT-6M GROUP 3. DISCUSSION (keV)
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136 HT-6M GROUP (4) Zeff was consta
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138 HUO et al - In the first case,
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140 HUO et al. 2.20 1.48 1.98 0.78
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142 HUO et al. O.O7 0.04 0.19 0.06
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IMPROVED CONFINEMENT REGIMES WITH O
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2 I o Q- ic 3 O x Q. CO. 0.4- 0.2-
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IAEA-CN-50/A-UI-l 149 — #25717 H
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8- 4- 8- 4- IAEA-CN-50/A-III-l 151
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2 /s) I.OH O.I- 10- Im 2 /sl 10- 0.
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10 .1 8 I 6 o ^ 4 (0 c: O - )0 IAEA
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IAEA-CN-50/A-in-l 157 assumed that
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160 JET TEAM in the main equilibriu
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162 JET TEAM 3. H-mode Characterist
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164 JET TEAM This occurs, however,
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166 JET TEAM 1.5 1.0 0.5 X(D5eV) «
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168 JET TEAM — 100 50-£ 20 10 5
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170 10 1.0 H-mode JET TEAM 5 10 [Pt
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172 JET TEAM time scales with curre
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174 JET TEAM 4.2. Local transport a
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176 JET TEAM v> 0> J£ rt' 1 E 8 o
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178 JET TEAM So far, the plasma den
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180 JET TEAM References [ 1 ] Wagne
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TRANSPORT IN TFTR SUPERSHOTS IAEA-C
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e at O
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i 30 20 10 10' IAEA-CN-50/A-III-3 1
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IAEA-CN-50/A-III-3 189 0.2 0.4 0.6
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IAEA-CN-50/A-III-3 191 supershot re
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194 BURRELL et al. Abstract ENERGY
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196 BURRELL et al. used in the init
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198 BURRELL et al. at the H-mode tr
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200 BURRELL et al. mode is more sta
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202 BURRELL et al. However, althoug
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204 BURRELL et al. > CO t Q < DC X
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CONFINEMENT STUDIES OF THE H-MODE O
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40 30 ft 20 a 10 50 40 30 20 10 (b)
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30 10 o : Ohmic Fei9 "1.0-4 • : L
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IAEA-CN-50/A-m-S 213 REFERENCES [1]
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216 JET TEAM temperatures. In those
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218 JET TEAM 0.1 5 10 Input Power (
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220 JET TEAM 1.00 0.75 0.50 0.25 0.
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222 JET TEAM FIG. 6. i)e as a junct
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224 JET TEAM TABLE I. PULSE NUMBERS
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226 JET TEAM The occurence of the e
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228 JET TEAM Acknowledgement The ex
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230 KAUFMANN et al. over the respec
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232 KAUFMANN et a\. 16 12 o 8 . At
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234 KAUFMANN et al. E 1.2 Z 0.8- ?
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236 KAUFMANN et al. -1 -2-- -3- + w
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TOKAMAK WITH STRONG MAGNETIC FIELD
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60 H £ 40 - IAEA-CN-50/A-IV-3 180
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,oV 10 10' 10 IAEA-CN-50/A-IV-3 243
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IAEA-CN-50/A-IV-3 245 REFERENCES [1
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248 JET TEAM NBI has been used to o
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250 JET TEAM pulses previously. Tun
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252 JET TEAM 1 5- 0- • 2.5 MeV ne
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254 JET TEAM Major Radius (m) Major
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FUSION PRODUCT MEASUREMENTS ON TFTR
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IAEA-CN-50/A-IV-5 259 to deuterium
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4.5 -.4.. ?3. POLOIDAL PLANE IAEA-C
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IAEA-CN-50/A-IV-5 263 achieved DD T
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266 TSUJ1 et a). 1. INTRODUCTION JT
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268 «+ 3 - 2 1 0 3 2 1 n - - IP IP
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270 TSUJIetal. 2.0 - 1.5 - 1.0 - 0.
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272 TSUJI et al. by the parameter d
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THERMAL WAVE INVESTIGATION OF ANOMA
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IAEA-CN-50/A-V-2-1 277 from the top
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40 30 01 £20 X 1-0 a " \ IAEA-CN-5
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IAEA-CN-50/A-V-2-2 COUPLING OF PART
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IAEA-CN-50/A-V-2-2 283 ASBD(V) FIG.
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'Z 1 IAEA-CN-50/A-V-2-2 285 o o° o
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DENSITY FLUCTUATIONS AND PARTICLE/
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1.0 5 10 15 20 Minor Radius ( cm )
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0.2 0.4 0.6 (a) r/a IAEA-CN-50/A-V-
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TURBULENCE, TRANSPORT AND q MEASURE
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0.01 IAEA-CN-50/A-V-3-2 295 • D H
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2.0 1.8 1.6 1.4 1.2 CT 1.0 0.8 0.6
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IAEA-CN-50/A-V-3-3 COMPARATIVE STUD
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IAEA-CN-50/A-V-3-3 301 TABLE I. COM
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IAEA-CN-50/A-V-3-3 303 85 13S 185 2
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IAEA-CN-50/A-V-3-3 305 the outer ed
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308 EFTHIMION et al. Perturbation t
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310 EFTHIMION et al. 4.0 2.0 - > 1.
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312 EFTHIMION et al. diffusivity ob
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314 EFTHIMION et al. 1.5 - 0 I.O- 0
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316 EFTHIMION et al. CX Sightlines
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318 EFTHEVHON et al. In the core re
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320 EFTHIMION et al. This explanati
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CURRENT DRIVEN TURBULENCE AND MICRO
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GO 40 20ri HI i i ii 1 \ IAEA-CN-S0
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E 4 tc) IAEA-CN-50/A-V-5 327 500 0
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IAEA-CN-50/A-V-5 329 REFERENCES [1]
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332 TEXTOR TEAM TEXTOR measurements
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334 TEXTOR TEAM The hydrogen recycl
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336 TEXTOR TEAM FIG. I. Sawtooth mo
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338 tv(r) 10 l9 m 3 J -0.2 TEXTOR T
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340 TEXTOR TEAM 11 12 13 !«] 18 19
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342 (a) MOVABLE UMITER DRIVE DeGRAS
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344 DeGRASSIE et al. CJ CO a 23 21
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IAEA-CN-50/A-VI-2-2 RESONANT HELICA
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( b ) 900 1 - 1200- 1100- S iooo- S
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IAEA-CN-50/A-VI-2-2 351 flow by pla
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INVESTIGATIONS ON THE MT-1 TOKAMAK
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IAEA-CN-50/A-VI-3-1 >v MPL J{_ FIG.
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IAEA-CN-50/A-VI-3-1 357 10 12 No. c
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IAEA-CN-50/A-VI-3-2 EDGE TURBULENCE
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3 Q. I I I I IAEA-CN-50/A-V1-3-2 36
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6 m / IAEA-CN-50/A-V1-3-2 363 I N 1
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a. 15 10 IAEA-CN-50/A-VI-3-2 365 s
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368 TARONI et al. report in Section
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370 TARONI et al. 100- q 80- 60- 40
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372 TARONI et al. 3.2 3.4 3.6 Radiu
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374 TARONI et al. t 1st FIG. 4. Res
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376 TARONI et al. [13] ROSS, D.W.,
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378 CAMPBELL et al. 'slow' partial
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380 -1 hot core Z(m) V) 4.4 4.2 4.0
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382 CAMPBELL et al. #13430 1 *1 ^.
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384 CAMPBELL et al. above 1, underl
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RESEARCH ON SAWTOOTH OSCILLATIONS A
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2=0.2 cm l ^ ^ f ^ ^ ^ ^ IAEA-CN-50
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-1.8 cm__^jJ/\M^ 0.2 2.2 IAEA-CN-50
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IAEA-CN-50/A-VII-3 393 [6] NAGAYAMA
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396 MANICKAM et al. Abstract STABIL
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398 MANICKAM et al. 1.6 1.0 30 20 1
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400 MANICKAM et al. 5. TURBULENCE,
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402 MANICKAM et al. sr 3 £.2 1 Bal
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404 MANICKAM et al. FIG. 6. Radial
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406 MANICKAM et al. FIG. 7. Punctur
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IAEA-CN-SO/A-VII-S MAGNETIC TURBULE
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IAEA-CN-50/A-VII-5 411 We compare t
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y
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MEASUREMENT OF MHD INSTABILITIES IN
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10 5 2 1 4 2 +5 0 2.0 1.0 Plasma Cu
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8.0 % 6.0
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IAEA-CN-50/A-VII-6 421 REFERENCES [
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424 BAGDASAROV et al. 0.1 0.2 0.3 t
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426 BAGDASAROV et al. _ 1.0 - 15 r~
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428 BAGDASAROV el al. 3. RATE OF CU
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430 BAGDASAROV et al. 1.5 1.0 0.5 0
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432 BAGDASAROV et al. 100 80 60 40
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434 BAGDASAROV et al. 1.5 - 1.0 CD
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436 BAGDASAROV et a!. suppression f
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438 KIYAMA et al. H profile is in t
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440 transition S 2 0.5 0 KIYAMA et
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442 KIYAMA et al. 1.0 ne/ne 0.5 ne/
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DISRUPTION CONTROL IN THE TOKAMAK T
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CD • CD IAEA-CN-50/A-VII-9 447 Ti
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340 350 360 Time(ms) IAEA-CN-50/A-V
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IAEA-CN-50/A-VII-9 451 Experiments
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454 DIPPELetal. 1. INTRODUCTION ALT
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456 DIPPEL et al. 100 80 >< 60 < E
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458 DIPPEL et al. four outside faci
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460 DIPPEL et al. REFERENCES [1] CO
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462 McCRACKEN et al. and the way in
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464 McCRACKEN et al. TABLE I. IMPUR
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466 McCRACKEN et al. 4. CONCLUSIONS
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468 DE KOCK et al. 2. EXPERIMENTAL
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470 DE KOCK et al. Profiles in dive
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472 DE KOCK et al. rrr 3 Ja. eV lio
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474 DE KOCK et al. discrepancy. How
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INVESTIGATION OF LIMITER SCRAPE-OFF
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-o.i 0 0 -0.2 .J-\ I I I 2 4 6 8 ar
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m 2 3 - 4 > o 3 2 - _ 5 -50 -100 |
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IAEA-CN-50/A-VII-14 MEASUREMENTS OF
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IAEA-CN-50/A-VII-14 have arbitrary
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IAEA-CN-50/A-VH-14 487 TABLE I. SOM
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IAEA-CN-50/A-VII-14 489 r =-D Vn +r
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IAEA-CN-50/A-VII-14 491 thermonucle
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IAEA-CN-50/A-VIM4 493 [11] Christia
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496 BOLTON et al. 70 60 50- £ 40
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498 BOLTON et al. * 3 - 5 T 3 - •
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500 BOLTON et al. SMM 1.0 (s) 0.5 t
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502 BOLTON et al. The Tokamak de Va
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CHARACTERISTICS OF BANANA REGIME CO
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o sz. It 11! IAEA-CN-50/A-VII-16 50
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IAEA-CN-50/A-VIM6 509 The estimated
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PLASMA HEATING AND CURRENT DRIVE (S
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514 ALIKAEVetal. 1. INTRODUCTION Th
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516 ALIKAEVetal. The profiles of ne
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518 ALIKAEV et al. 4 ~ S " 3 1 b
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520 ALIKAEV et al. u n < 3 - 2 r ,
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522 ALIKAEV et al. FIG. 10. Diamagn
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524 ALIKAEV et al. 3.2 _ ^ 3.1 CO 3
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IAEA-CN-50/E-I-2 ELECTRON CYCLOTRON
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IAEA-CN-50/E-I-2 529 2. ELECTRON CY
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4.0 3.0 2.0 1.0 0.0 6.0 4.0- 2.0- 0
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IAEA-CN-50/E-I-2 3. CONFINEMENT WIT
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2.0 . P« (MW) \PNBI 800 1000 1200
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S Q o ERH a. HI Q - AMPL 80- 60- 40
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IAEA-CN-50/E-I-2 539 The ELM-free p
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542 ASHRAF et al. experiments on FT
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544 1.1 ASHRAF et al. Absorption zo
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546 ASHRAF et al. cm from the magne
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548 ASHRAF et al. 20 4 I ,5 £ 10 .
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HIGH POWER ECRH AND ICRF HEATING EX
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IAEA-CN-50/E-I-4 553 0-1 Jr FIG. 2.
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1.2. ICRF experiments IAEA-CN-50/E-
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IAEA-CN-50/E-I-4 557 This effect mi
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100 50 4th 2.0 3,0 IAEA-CN-50/E-I-4
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IAEA-CN-50/E-I-4 561 [3] SATO, M.,
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564 * 0 2 ' 0 20 ? I 0 § 0 50 100
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566 TANAKA et al. and one order sma
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568 TANAKA et al. Figures 3(a)-(i)
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570 TANAKA et al. [2] TANAKA, S., e
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572 WEYNANTS et al. Important aniso
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574 WEYNANTS et al. 05- (c) V. V DI
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576 WEYNANTS et al. 3 eff.o 2 1 •
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578 WEYNANTS et al. 2.06 2.10 2.14
Page 606 and 607:
580 20 EH.rh [kJl WEYNANTS et al. 3
Page 608 and 609:
582 WEYNANTS et al. [II] JACQUINOT,
Page 610 and 611:
584 NOTERDAEME et al. in the start-
Page 612 and 613:
586 NOTERDAEME et al.
Page 614 and 615:
588 NOTERDAEME et al. with the time
Page 616 and 617:
590 NOTERDAEME et al. the small imp
Page 618 and 619:
592 NOTERDAEME et al. 13] NOTERDAEM
Page 620 and 621:
594 START et al. sustained for 1.2
Page 622 and 623:
596 START et al. 300 200 Te (eV) 10
Page 624 and 625:
598 START et al. GAMMA YIELD COUNTS
Page 626 and 627:
600 START et al. 45 t(S) Onset of s
Page 628 and 629:
602 START et al. and the energy con
Page 631 and 632:
SECOND HARMONIC ICRF HEATING EXPERI
Page 633 and 634:
,01) |c= 0.4 0.2 0 2 I 0 3 2 • 1
Page 635 and 636:
IAEA-CN-50/E-II-4 609 1 1 I 1 I 1 1
Page 637 and 638:
IAEA-CN-50/E-II-5 FULL-WAVE MODELIN
Page 639 and 640:
IAEA-CN-50/E-II-5 613 When Eq. (4)
Page 641 and 642:
IAEA-CN-50/E-II-5 615 the equations
Page 643 and 644:
IAEA-CN-50/E-H-5 617 I i i i I I I
Page 645 and 646:
1.0 0.9 0.8 0.7 1 0.6 10.5 1 0.4 0.
Page 647 and 648:
LOWER HYBRID EXPERIMENTS IN JT-60 K
Page 649 and 650:
- 2t ji IplMA) OIV LIM 0.7 - A 1.0
Page 651 and 652:
'E - 3 "2 2 - 2 le? Ip(MA) 0.7 1.0
Page 653 and 654:
IAEA-CN-SO/E-m-l 627 circles are da
Page 655 and 656:
STEADY STATE CURRENT DRIVE BY LOWER
Page 657 and 658:
45 2 30 a. " 15 0 7 e s 9 2.5 : ic
Page 659 and 660:
1/1 z 3 163- IAEA-CN-50/E-III-2 633
Page 661 and 662:
50* 70" 90' 110" 130' 150' 170* A*
Page 663 and 664:
IAEA-CN-50/E-III-3 LOWER HYBRID HEA
Page 665 and 666:
1.0 0.8 - _ OOnrr IAEA-CN-50/E-HI-3
Page 667 and 668:
-4 IAEA-CN-50/E-HI-3 641 FIG. 3. Sa
Page 669:
IAEA-CN-50/E-III-3 643 stronger emi
Page 672 and 673:
646 BUDNIKOV et al. 100 50 34 36 38
Page 674 and 675:
648 BUDN1K0V et al. 2 E (keV) F/G.
Page 676 and 677:
650 BUDNIKOV et a). » 4 t 660 f (M
Page 678 and 679:
652 BUDNIKOV et al. •a I -a 10' 1
Page 680 and 681:
654 BUDNIKOV etal. 0.5 CM* ne(x10 1
Page 682 and 683:
656 SCOTT et al. 1. Introduction A
Page 684 and 685:
658 SCOTT et al. FIG. 2. Central ro
Page 686 and 687:
660 SCOTT et al. 30 25 20 - / 1 10
Page 688 and 689:
662 SCOTT et al. The TFTR "supersho
Page 690 and 691:
664 SCOTT et al. Z3 5. 2 ? 1 Ge XXX
Page 692 and 693:
666 SCOTT et al. to drive most or a
Page 695 and 696:
DIII-D NEUTRAL BEAM CURRENT DRIVE E
Page 697 and 698:
IAEA-CN-50/E-III-6 671 2. NEUTRAL B
Page 699 and 700:
3.0 0.0 0.2 0.0 0.2 0.0 30.0 SXR (r
Page 701 and 702:
IAEA-CN-50/E-HKS 675 obtained and i
Page 703 and 704:
0.5- o.o -1 0.2- 0.0- 1.0- 0.6- 4.0
Page 705:
IAEA-CN-50/E-HI-6 679 [17] STRAIT,
Page 708 and 709:
682 OHKAWA et al. 2. CURRENT DRIVE
Page 710 and 711:
684 OHKAWA et al. In terms of the h
Page 712 and 713:
686 OHKAWA et al. regime. For ut <
Page 714 and 715:
688 OHKAWA et al. while holding the
Page 717 and 718:
ICRF HEATING ON THE TFTR TOKAMAK FO
Page 719 and 720:
IAEA-CN-50/E-IV-l 693 4 He plasma a
Page 721 and 722:
300 IAEA-CN-50/E-IV-l 695 -10 o 10
Page 723:
5. Conclusions IAEA-CN-50/E-IV-l 69
Page 726 and 727:
700 ASKINASI et al. 0 120 , 60 RF 1
Page 728 and 729:
702 ASKINASI et al. 240 - \ -3 \ J
Page 730 and 731:
704 ASKINASI et al. TABLE I. LOCATI
Page 732 and 733:
706 ASKINASI et al. REFERENCES [1]
Page 734 and 735:
708 KASILOV et al. current drive me
Page 736 and 737:
710 KASILOV et al. to the two-ion h
Page 738 and 739:
712 KASILOV et al. with the FW exci
Page 740 and 741:
714 KASILOV et al. Similarly, takin
Page 742 and 743:
716 KASILOV et al. If the resonant
Page 744 and 745:
718 KASILOVetal. If eh < e,, Eq. (1
Page 747 and 748:
IAEA-CN-50/E-IV-4 FULL WAVE SOLUTIO
Page 749 and 750:
with IAEA-CN-50/E-IV-4 723 H;(r) =
Page 751 and 752:
3000 m 2000 1000 0 1AEA-CN-50/E-IV-
Page 753 and 754:
IAEA-CN-50/E-IV-5 EXPERIMENTS ON EF
Page 755 and 756:
IAEA-CN-50/E-IV-5 729 0 ""'"10 20 3
Page 757 and 758:
IAEA-CN-50/E-IV-5 731 A, for a net
Page 759 and 760:
IMPROVEMENT OF RF CURRENT DRIVE DEN
Page 761 and 762:
IAEA-CN-S0/E-IV-6 735 A fast wave (
Page 763 and 764:
IAEA-CN-50/E-IV-6 737 electrons. Th
Page 765 and 766:
IAEA-CN-50/E-IV-7 NON-INDUCTIVE STA
Page 767 and 768:
300 200 - 100 - IAEA-CN-50/E-IV-7 7
Page 769 and 770:
IAEA-CN-50/E-IV-7 743 are related t
Page 771 and 772:
IAEA-CN-50/E-IV-7 745 TABLE I. CHAR
Page 773 and 774:
ACCESS TO SECOND STABILITY VIA PROF
Page 775 and 776:
6 5 4 w 3 2 1 0 IAEA-CN-50/E-IV-8 7
Page 777 and 778:
IAEA-CN-50/E-IV-8 751 10 15 20 RF C
Page 779 and 780:
IAEA-CN-50/E-IV-9 ELECTRON CYCLOTRO
Page 781 and 782:
IAEA-CN-50/EIV-9 755 The second mec
Page 783:
IAEA-CN-50/E-IV-9 757 In our case,
Page 786 and 787:
760 COHEN et al. concept of using p
Page 788 and 789:
762 COHEN et al. TABLE I. REPRESENT
Page 790 and 791:
764 COHEN et al. 20 ECH power P (MW
Page 792 and 793:
766 COHEN et al. [3] COHEN, B.I., e
Page 794 and 795:
768 electron velocity distribution
Page 796 and 797:
770 PESlC -02 FIG. 2. Real and imag
Page 798 and 799:
772 PESlC FIG. 5. Real and imaginar
Page 801 and 802:
CHAIRMEN OF SESSIONS Session A-I J.
Page 804:
INTERNATIONAL ATOMIC ENERGY AGENCY
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