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ENERGY CONFINEMENT WITH AUXILIARY HEATING IN JT-60 <strong>IAEA</strong>-CN-50/A-V-1 S. TSUJI, M. AKIBA, T. ANDO, K. ANNOH, T. AOYAGI, K. ARAKAWA, M. AZUMI, T. FUJH, T. FUKUDA, A. FUNAHASHI, K. HAMAMATSU, T. HIRAYAMA, M. HONDA, H. HORIIKE, N. HOSOGANE, T. IIJIMA, Y. IKEDA, T. IMAI, S. ISHIDA, K. ITAMI, T. ITO, Y. KAMADA, Y. KAWANO, M. KIKUCHI, H. KIMURA, T. KIMURA, H. KISfflMOTO, Y. KOIDE, T. KOIKE, I. KONDO, S. KONOSfflMA, H. KUBO, S. KUNIEDA, K. KURIHARA, M. KURIYAMA, Y. KUSAMA, S. MAEHARA, K. MAENO, T. MATOBA, S. MATSUDA, M. MATSUKAWA, T. MATSUKAWA, M. MATSUOKA, Y. MATSUZAKI, N. MIYA, K. MIYACHI, M. MIZUNO, M. NAGAMI, A. NAGASHIMA, K. NAGASHIMA, T. NAGASfflMA, O. NAITO, H. NAKAMURA, M. NEMOTO, Y. NEYATANI, H. NINOMIYA, N. NISHINO, T. NISHITANI, K. ODAJIMA, N. OGIWARA, T. OHGA, M. OHTA, K. OMORI, S. OMORI, T. OZEKI, M. SAIGUSA, K. SAKAMOTO, A. SAKASAI, M. SATO, M. SEIMIYA, M. SEKI, S. SEKI, K. SHIMIZU, M. SHIMIZU, Y. SHIMOMURA, H. SHIRAI, H. SHIRAKATA, T. SUGIE, M. TAKAHASHI, S. TAKAHASHI, H. TAKATSU, H. TAKEUCHI, S. TAMURA, Y. TANAKA, K. TANI, K. TOBITA, N. TOYOSHIMA, M. TSUNEOKA, K. UEHARA, K. USHIGUSA, I. YONEKAWA, H. YOSHIDA, R. YOSHINO Naka Fusion Research Establishment, Japan Atomic Energy Research Institute, Naka-machi, Naka-gun, Ibaraki-ken, Japan Abstract ENERGY CONFINEMENT WITH AUXILIARY HEATING IN JT-60. An improved divertor confinement regime has been found in beam heated lower X-point discharges in JT-60. The improvement is associated with an increase in electron density <strong>and</strong> high particle recycling in the divertor region, the latter of which is in contrast to the H-mode. The energy confinement time becomes longer than that of limiter discharges with the same plasma volume by up to 50%. The radiation power in the divertor region is increased up to half of the input power. Frequent edge localized modes observed in low-q discharges degrade the improved energy confinement. 265
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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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nee id interfere >res an j-> 1 O E
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i I •O OJ) — '5 c IS 2 HI 1ZI _
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5.' ' *[Wbl t. 3. 2. 1. _ _ X IAEA-
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nl 30 .29 .28 .27 26 .25 .24 .23 22
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IAEA-CN-50/A-I-1 However, reasonabl
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IAEA-CN-50/A-I-1 25 will make it po
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IAEA-CN-50/A-I-2 AN OVERVIEW OF TFT
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IAEA-CN-50/A-I-2 29 inner belt limi
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IAEA-CN-50/A-I-2 31 0 10 20 TOTAL P
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5 DC LU LU 3 - 1 - Q Q A 1 A IAEA-C
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IAEA-CN-50/A-I-2 35 The question ar
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0.20 0.15 0.10 Rp= 2.45 m a = 0.79
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: . • • 1 IAEA-CN-50/A-I-2 39 1
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LATEST JET RESULTS AND FUTURE PROSP
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Parameter Plasma major radius (Ro)
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1500 IAEA-CN-50/A-I-3 45 2 4 I, (MA
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IAEA-CN-50/A-I-3 47 3.0 3.5 Major r
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I 15 10 5 0 IAEA-CN-50/A-I-3 49 V \
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IAEA-CN-50/A-I-3 51 Magnetic measur
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0.8 0.6 IAEA-CN-50/A-I-3 53 -0.2 12
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10 0.5 Pulse No: 15376 n(He')/ne=1.
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IAEA-CN-50/A-I-3 57 5 10 15 [Pt-dW/
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10 E X 4 H-mode y 0.2 0.4 0.6 0.8 1
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IAEA-CN-50/A-I-3 61 where V is the
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IAEA-CN-50/A-I-3 63 confinement deg
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IAEA-CN-50/A-I-3 65 References [1 ]
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68 JT-60 TEAM T. TANAKA, Y. TANAKA,
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Ip = 3.2 MA lp = 2.7 MA JT-60TEAM R
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72 JT-60TEAM E5695 0 1 2 3 4 5 6 7
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74 JT-60TEAM 3 : LIH *3.1HA 2.8HA A
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76 JT-60TEAM 4.5 5.0 5.5 6.0 6.5 7.
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78 JT-60TEAM 250 "(a) 200 150 50 n
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80 JT-60 TEAM The further developme
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STABILITY OF HIGH BETA DISCHARGES I
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IAEA-CN-50/A-II-l 85 a typical plas
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0.5- 0- 0.8- 0.4- 0.0- IAEA-CN-50/A
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IAEA-CN-50/A-IM 89 absence of the l
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s.o • .5 (a) IAEA-CN-50/A-II-l 91
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IAEA-CN-50/A-II-l 93 stability limi
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IAEA-CN-50/A-II-l 95 [6] STAMBAUGH,
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98 OKABAYASHI et al. PBX-M maximall
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100 1 .0 .6 .0 -.2 -.4 -.6 1.11 CO
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102 0.5 OKABAYASHI et al. Indentati
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104 OKABAYASHI et al. 40 30 I I I I
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106 OKABAYASHI et al. §1 •a J i
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108 OKABAYASHI et al. -2 1 • •
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MHD ACTIVITIES AND RELATED IMPURITY
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0.5 IAEA-CN-50/A-H-3 113 FIG. 1. St
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0) a. II E IAEA-CN-50/A-H-3 115 1 1
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IAEA-CN-50/A-II-3 117 These observa
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6. CONCLUSIONS IAEA-CN-50/A-II-3 11
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122 GAO et al. With hydrogen plasma
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124 GAO et al. P—3.0 r—8.5 SHOT
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126 GAO et al. a) M >
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128 GAO et al. 0.6 0.3 0.0 50 100 r
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SUPERLOW DENSITY EXPERIMENT ON HT-6
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IAEA-CN-50/A-n-S-l 133 (b) Hard X-r
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IAEA-CN-SO/A-n-5-l 135 0 0.2 0.4 0:
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IAEA-CN-50/A-D-5-2 INVESTIGATION OF
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0.14 0.10 0.09 0.08 0.05 0.04 0.03
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TABLE I. REDUCTION OF Xe (m 2 -s')
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IAEA-CN-50/A-II-5-2 143 (3) The lin
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146 FUSSMANN et al. Abstract IMPROV
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148 FUSSMANN et al. 150- 100- 50- 0
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150 FUSSMANN et al. UJ 100- 50- + 2
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152 FUSSMANN et al. In both regimes
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154 FUSSMANN et al. reduced. With c
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156 FUSSMANN et al. and consequentl
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THE JET H-MODE AT HIGH CURRENT AND
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IAEA-CN-50/A-IH-2 achieve an H-mode
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6.0 40 2.0 (a) 0l=. 5.0 (c) 0 Pulse
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IAEA-CN-50/A-III-2 165 reduced in t
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IAEA-CN-50/A-HI-2 167 near the firs
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IAEA-CN-50/A-III-2 169 plasmas with
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I 3s H-mode 8
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IAEA-CN-50/A-HI-2 173 The steep tem
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IAEA-CN-50/A-III-2 175 available),
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IAEA-CN-50/A-III-2 177 (xi0 19 m 3
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IAEA-CN-50/A-III-2 179 APPENDIX I T
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IAEA-CN-50/A-IH-2 181 [16] Bishop,
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184 ZARNSTORFT et al. Abstract TRAN
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186 ZARNSTORFF et al. X-ray spectro
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188 ZARNSTORFF et al. 8 CM e CM E 2
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190 ZARNSTORFF et al. 1.5 2.0 2.5 n
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IAEA-CN-50/A-III-4 ENERGY CONFINEME
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o O •
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0.3 0.2- 0.1- 0.0 0.8 0.6 0.4 0.2 0
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00 d f CM I- CQ i o o o IAEA-CN-50/
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E m F LU LJU Z o N_ CE UU o / UJ q
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IAEA-CN-50/A-m-4 203 The TB values
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IAEA-CN-50/A-HM 205 [7] OHYABU, N.,
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208 SUZUKI et al. favourable in a c
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210 SUZUKI etal. As the neutral bea
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212 SUZUKI et al. 3. FOUR-PELLET IN
Page 241 and 242: HEATING OF PEAKED DENSITY PROFILES
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Page 245 and 246: 1.3 I" 1 |03 C 0.5 i: 12 8 4 n - Te
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Page 251 and 252: 0.3 f0.2 1 5" 0.1 IAEA-CN-50/A-IV-l
Page 253 and 254: IAEA-CN-50/A-IV-l 227 APPENDIX I TH
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Page 259 and 260: 0 FIG. 4. ONI O £ at o ID c IC 15
Page 261 and 262: IAEA-CN-50/A-IV-2 0.35 MW 2.6 MW Ga
Page 263: IAEA-CN-50/A-IV-2 237 finement. The
Page 266 and 267: 240 AZIZOV et al. TABLE I. TSP PARA
Page 268 and 269: 242 AZIZOV et al. 65 75 85 95 105 1
Page 270 and 271: 244 AZIZOV et al. 30 40 50 60 Ip =
Page 273 and 274: HIGH TEMPERATURE EXPERIMENTS AND FU
Page 275 and 276: IAEA-CN-50/A-IV-4 249 FIG. 1. Data
Page 277 and 278: P ICRHV 2 IAEA-CN-50/A-IV-4 251 FIG
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Page 284 and 285: 258 STRACHAN et al. - Z - 1, Steady
Page 286 and 287: 260 STRACHAN et al. 10' 10' Classic
Page 288 and 289: 262 STRACHAN et al. _ 1 s 10* I : 1
Page 292 and 293: 266 TSUJ1 et a). 1. INTRODUCTION JT
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Page 296 and 297: 270 TSUJIetal. 2.0 - 1.5 - 1.0 - 0.
Page 298 and 299: 272 TSUJI et al. by the parameter d
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Page 303 and 304: IAEA-CN-50/A-V-2-1 277 from the top
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Page 307 and 308: IAEA-CN-50/A-V-2-2 COUPLING OF PART
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Page 313 and 314: DENSITY FLUCTUATIONS AND PARTICLE/
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Page 325 and 326: IAEA-CN-50/A-V-3-3 COMPARATIVE STUD
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Page 331: IAEA-CN-50/A-V-3-3 305 the outer ed
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Page 336 and 337: 310 EFTHIMION et al. 4.0 2.0 - > 1.
Page 338 and 339: 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
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580 20 EH.rh [kJl WEYNANTS et al. 3
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582 WEYNANTS et al. [II] JACQUINOT,
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584 NOTERDAEME et al. in the start-
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586 NOTERDAEME et al.
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588 NOTERDAEME et al. with the time
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590 NOTERDAEME et al. the small imp
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592 NOTERDAEME et al. 13] NOTERDAEM
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594 START et al. sustained for 1.2
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596 START et al. 300 200 Te (eV) 10
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598 START et al. GAMMA YIELD COUNTS
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600 START et al. 45 t(S) Onset of s
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602 START et al. and the energy con
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SECOND HARMONIC ICRF HEATING EXPERI
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,01) |c= 0.4 0.2 0 2 I 0 3 2 • 1
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IAEA-CN-50/E-II-4 609 1 1 I 1 I 1 1
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IAEA-CN-50/E-II-5 FULL-WAVE MODELIN
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IAEA-CN-50/E-II-5 613 When Eq. (4)
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IAEA-CN-50/E-II-5 615 the equations
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IAEA-CN-50/E-H-5 617 I i i i I I I
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1.0 0.9 0.8 0.7 1 0.6 10.5 1 0.4 0.
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LOWER HYBRID EXPERIMENTS IN JT-60 K
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- 2t ji IplMA) OIV LIM 0.7 - A 1.0
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'E - 3 "2 2 - 2 le? Ip(MA) 0.7 1.0
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IAEA-CN-SO/E-m-l 627 circles are da
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STEADY STATE CURRENT DRIVE BY LOWER
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45 2 30 a. " 15 0 7 e s 9 2.5 : ic
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1/1 z 3 163- IAEA-CN-50/E-III-2 633
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50* 70" 90' 110" 130' 150' 170* A*
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IAEA-CN-50/E-III-3 LOWER HYBRID HEA
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1.0 0.8 - _ OOnrr IAEA-CN-50/E-HI-3
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-4 IAEA-CN-50/E-HI-3 641 FIG. 3. Sa
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IAEA-CN-50/E-III-3 643 stronger emi
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646 BUDNIKOV et al. 100 50 34 36 38
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648 BUDN1K0V et al. 2 E (keV) F/G.
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650 BUDNIKOV et a). » 4 t 660 f (M
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652 BUDNIKOV et al. •a I -a 10' 1
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654 BUDNIKOV etal. 0.5 CM* ne(x10 1
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656 SCOTT et al. 1. Introduction A
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658 SCOTT et al. FIG. 2. Central ro
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660 SCOTT et al. 30 25 20 - / 1 10
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662 SCOTT et al. The TFTR "supersho
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664 SCOTT et al. Z3 5. 2 ? 1 Ge XXX
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666 SCOTT et al. to drive most or a
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DIII-D NEUTRAL BEAM CURRENT DRIVE E
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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
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IAEA-CN-50/E-HKS 675 obtained and i
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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,
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682 OHKAWA et al. 2. CURRENT DRIVE
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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
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702 ASKINASI et al. 240 - \ -3 \ J
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704 ASKINASI et al. TABLE I. LOCATI
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706 ASKINASI et al. REFERENCES [1]
Page 734 and 735:
708 KASILOV et al. current drive me
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710 KASILOV et al. to the two-ion h
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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
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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
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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
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300 200 - 100 - IAEA-CN-50/E-IV-7 7
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IAEA-CN-50/E-IV-7 743 are related t
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IAEA-CN-50/E-IV-7 745 TABLE I. CHAR
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ACCESS TO SECOND STABILITY VIA PROF
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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
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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
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764 COHEN et al. 20 ECH power P (MW
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766 COHEN et al. [3] COHEN, B.I., e
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768 electron velocity distribution
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770 PESlC -02 FIG. 2. Real and imag
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772 PESlC FIG. 5. Real and imaginar
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CHAIRMEN OF SESSIONS Session A-I J.
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INTERNATIONAL ATOMIC ENERGY AGENCY
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