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180 JET TEAM References [ 1 ] Wagner, F., et al., 'Regime of improved confinement and high beta in neutral-beamheated divertor discharges of the ASDEXtokamak', Phys. Rev. Lett. 49(1982) 1408. [2] Kaye, S.M., et al., 'Attainment of high confinement in neutral beam heated divertor discharges in the PDX tokamak', J. Nucl. Mat. 121 (1984) 115. [3] Luxon, J., et al., 'Initial results from the DIII-D tokamak', Plasma Phys. and Contr. Nucl. Fus. Res. 1(1987) 159. [ 4 ] Odaj ima, K., et al., 'Confinement studies of additionally heated plasma in the JFT-2M tokamak', Plasma Phys. and Contr. Nucl. Fus. Res. (Proc. 1 lth Int. Conf., Kyoto, 1986) 1(1987) 151. [ 5 ] Tanga, A., et al., 'Experimental studies in JET with magnetic separatrix', Plasma Phys. and Contr. Nucl. Fus. Res. (Proc. 1 lth Int. Conf., Kyoto, 1986) 1 (1987) 65. [6] Salzmann, H.M., et al., (Invited paper at the APS Topical Conference on Plasma Diagnostics, Napa Valley, Calif, USA), (1988). [7] Smeulders, P., etal., 'Hollow profiles and high-{i effects during H-mode in JET', JET Internal Report JET-IR(88)11, JET Joint Undertaking, (1988). [8] Boileau, A., etal., 'The deduction oflow-Zion temperature and densities in the JET tokamak using charge exchange recombination spectroscopy', JET Preprint JET- P(87)44, JET Joint Undertaking, (1987). To be published in Plasma Phys. [9] Morgan,P.D., 'TheevolutionofZef/r)profilesinJETplasmas',(Pro.c. 15thEurop. Conf. on Contr. Fus. and Plasma Heating, Dubrovnik) 12B (I) (1988) 139. [10] Behringer, K., etal., 'Impurity transport in JET during H-mode, monster sawteeth, and after pellet injection', (Proc. 15th Europ. Conf. on Contr. Fus. and Plasma Heating, Dubrovnik) 12B (I) (1988) 338. [11] O'Rourke, J., et al., 'Polarimetric measurements of the q-profile', (Proc. 15thEurop. Conf. on Contr..Fus. and Plasma Heating, Dubrovnik) 12B (I) (1988) 155. [12] Bickerton, R.J., Connor, J.W., Taylor, J.B., 'Diffusion driven plasma currents and bootstrap tokamak', Nat. Phys. Sc. 229 (1971) 110. [13] Goldston, R.J., etal., 'New techniques for calculating heat and particle source rates due to neutral beam injection in axisymmetric tokamaks', J. Comput. Phys. 43 (1981) 61. [14] Zarnstorff, M.C.etal., 'Non-ohmic currents in TFTR\ Phys. Rev. Lett. 60(1988) 1306. [ 15] Challis, C, etal., 'Non inductively driven currents in JET, JET Preprint JET-P(88)38, JET Joint Undertaking, (1988). To be published in Nucl. Fus.
IAEA-CN-50/A-IH-2 181 [16] Bishop, CM., 'Stability oflocalised MHD modes in divertor tokamaks:a picture of theH-mode', Nucl. Fus. 26 (1986) 1063. [ 17] Bishop, CM., 'Bifurcated temperature profiles and theH-mode', Nucl. Fus. 27(1986) 1765. [18] Harbour, P. J., Workshop on Plasma Edge Theory in Fusion Devices, Augustusburg, GDR, 26-30 April 1988. To be published in 'Contributions to Plasma Physics', (Akademie-Verlag, Berlin, GDR). [ 19] Itoh, S.I. and Itoh, K., 'Modelof H/L transition in tokamak', Phys. Rev. Lett. 60 (1988) 2276. [20] Harbour, P.J., et al., (8th Int. Conf. on Plasma Surface Interactions in Contr. Fus. Devices, 2-6 May 1988, Jiilich, FRG). To be published in J. Nucl. Mat. [21] deKock,L.,etal., 'The plasma boundary in JET', Paper IAEA-CN-50/A-VII-12/2. This conference. [ 22 ] Goldston, R. J., 'Energy confinement scaling in tokamaks: some implications of recent experiments with ohmicandstrong auxiliary heating', Plasma Phys. and Contr. Fus. 26 (1984) 87. [23 ] Keilhacker, M., et al., 'Studies of energy transport in JETH-modes', (Proc. 15th Europ. Conf. Fus. and Plasma Heating, Dubrovnik) 12B (I) (1988) 231.
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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
Page 157 and 158: SUPERLOW DENSITY EXPERIMENT ON HT-6
Page 159 and 160: IAEA-CN-50/A-n-S-l 133 (b) Hard X-r
Page 161 and 162: IAEA-CN-SO/A-n-5-l 135 0 0.2 0.4 0:
Page 163 and 164: IAEA-CN-50/A-D-5-2 INVESTIGATION OF
Page 165 and 166: 0.14 0.10 0.09 0.08 0.05 0.04 0.03
Page 167 and 168: TABLE I. REDUCTION OF Xe (m 2 -s')
Page 169: IAEA-CN-50/A-II-5-2 143 (3) The lin
Page 172 and 173: 146 FUSSMANN et al. Abstract IMPROV
Page 174 and 175: 148 FUSSMANN et al. 150- 100- 50- 0
Page 176 and 177: 150 FUSSMANN et al. UJ 100- 50- + 2
Page 178 and 179: 152 FUSSMANN et al. In both regimes
Page 180 and 181: 154 FUSSMANN et al. reduced. With c
Page 182 and 183: 156 FUSSMANN et al. and consequentl
Page 185 and 186: THE JET H-MODE AT HIGH CURRENT AND
Page 187 and 188: IAEA-CN-50/A-IH-2 achieve an H-mode
Page 189 and 190: 6.0 40 2.0 (a) 0l=. 5.0 (c) 0 Pulse
Page 191 and 192: IAEA-CN-50/A-III-2 165 reduced in t
Page 193 and 194: IAEA-CN-50/A-HI-2 167 near the firs
Page 195 and 196: IAEA-CN-50/A-III-2 169 plasmas with
Page 197 and 198: I 3s H-mode 8
Page 199 and 200: IAEA-CN-50/A-HI-2 173 The steep tem
Page 201 and 202: IAEA-CN-50/A-III-2 175 available),
Page 203 and 204: IAEA-CN-50/A-III-2 177 (xi0 19 m 3
Page 205: IAEA-CN-50/A-III-2 179 APPENDIX I T
Page 210 and 211: 184 ZARNSTORFT et al. Abstract TRAN
Page 212 and 213: 186 ZARNSTORFF et al. X-ray spectro
Page 214 and 215: 188 ZARNSTORFF et al. 8 CM e CM E 2
Page 216 and 217: 190 ZARNSTORFF et al. 1.5 2.0 2.5 n
Page 219 and 220: IAEA-CN-50/A-III-4 ENERGY CONFINEME
Page 221 and 222: o O •
Page 223 and 224: 0.3 0.2- 0.1- 0.0 0.8 0.6 0.4 0.2 0
Page 225 and 226: 00 d f CM I- CQ i o o o IAEA-CN-50/
Page 227 and 228: E m F LU LJU Z o N_ CE UU o / UJ q
Page 229 and 230: IAEA-CN-50/A-m-4 203 The TB values
Page 231: IAEA-CN-50/A-HM 205 [7] OHYABU, N.,
Page 234 and 235: 208 SUZUKI et al. favourable in a c
Page 236 and 237: 210 SUZUKI etal. As the neutral bea
Page 238 and 239: 212 SUZUKI et al. 3. FOUR-PELLET IN
Page 241 and 242: HEATING OF PEAKED DENSITY PROFILES
Page 243 and 244: Yd o g a> - c 4 _n ...— 0) n 12 t
Page 245 and 246: 1.3 I" 1 |03 C 0.5 i: 12 8 4 n - Te
Page 247 and 248: IAEA-CN-50/A-IV-l 221 1 2 3 Q,_-2ff
Page 249 and 250: 2 q(o) 1- 10 1 U • O • IAEA-CN-
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Page 253 and 254: IAEA-CN-50/A-IV-l 227 APPENDIX I TH
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3 - 2 - 1 - IAEA-CN-50/A-IV-2 231 1
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0 FIG. 4. ONI O £ at o ID c IC 15
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IAEA-CN-50/A-IV-2 0.35 MW 2.6 MW Ga
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IAEA-CN-50/A-IV-2 237 finement. The
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240 AZIZOV et al. TABLE I. TSP PARA
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242 AZIZOV et al. 65 75 85 95 105 1
Page 270 and 271:
244 AZIZOV et al. 30 40 50 60 Ip =
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HIGH TEMPERATURE EXPERIMENTS AND FU
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IAEA-CN-50/A-IV-4 249 FIG. 1. Data
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P ICRHV 2 IAEA-CN-50/A-IV-4 251 FIG
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IAEA-CN-SO/AIV-4 253 FIG. 4. (a) Di
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IAEA-CN-50/A-IV-4 255 The fusion pe
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258 STRACHAN et al. - Z - 1, Steady
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260 STRACHAN et al. 10' 10' Classic
Page 288 and 289:
262 STRACHAN et al. _ 1 s 10* I : 1
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ENERGY CONFINEMENT WITH AUXILIARY H
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E6950(Bi=4.0T) E6956(Bt = 2.7T) °4
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E7558 • IMPROVED 5 6 TIME (S) IAE
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7.0 E - 1 0.0 7.0 0.0 =— \ n; - T
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IAEA-CN-50/A-V-1 273 [9] SHIMOMURA,
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276 ASHRAF et al. However, the conv
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278
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280 ASHRAF et al. Modulation amplit
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282 KIMet al. (a) (b) 410 420 TIME
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284 KIM et al. (b) o 3
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286 KIM et ah In summary, we observ
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288 KAWAHATA et al. TEXT tokamak, t
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290 KAWAHATA et al. ^ 30 °- S-200.
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292 KAWAHATA et al. 0 6 12 18 24 ra
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294 WOOTTON et al. 1. Particle tran
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296 10' N 10° E gio- 1 O (a) 10" 0
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298 WOOTTON et al. ne=3xl0 19 m- 3
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300 ZURRO et al. FIG. 1. Variation
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302 ZURRO et al. Mo) 6 (10"cm- 3 )
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304 ZURRO et al. -140 50 100 f(kHz)
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TRANSPORT STUDIES ON TFTR UTILIZING
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IAEA-CN-50/A-V-4 309 uses the TRANS
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5 g 30 20 < 2.0 Q § 1.0 i 0.5 10 1
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IAEA-CN-50/A-V-4 313 the laser-blow
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IAEA-CN-S0/A-V-4 315 on working gas
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I0 7 ! 10' 1.8 IAEA-CN-50/A-V-4 317
Page 345 and 346:
IAEA-CN-50/A-V-4 319 The difference
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IAEA-CN-50/A-V-4 321 [12] RADEZTSKY
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324 DONNE et al. E CO o FIG. 1. Sho
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326 DONNE et al. 350 300 250 200 15
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328 DONNE et al. 1.0 0.8 - 0.6 - t
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RECENT TEXTOR RESULTS TEXTOR TEAM (
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IAEA-CN-50/A-VI-l 333 line-radiatio
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IAEA-CN-50/A-VI-l 335 These measure
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q(r] 3- 2- 1- - IAEA-CN-50/A-VI-l 3
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IAEA-CN-50/A-VI-l 339 FIG. 4. Sawto
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IAEA-CN-S0/A-VI-2-1 RESONANT ISLAND
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IAEA-CN-50/A-VI-2-1 343 • «• >
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IAEA-CN-50/A-VI-2-1 345 tons. This
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348 EVANS et al. JIPP T-IIU ( minor
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350 EVANS et al. FIG. 3. High speed
Page 378 and 379:
352 EVANS et al. REFERENCES [1] KAR
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354 BAKOS et al. The radiation of t
Page 382 and 383:
356 BAKOS et al. < + s 5 2 1 5 2 10
Page 384 and 385:
358 BAKOS et al. REFERENCES [1] BAK
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360 STfiCKEL et al. A quantitative
Page 388 and 389:
362 STOCKEL et al. This and other f
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364 STOCKEL et al. 15 I 10 "" 5 0 (
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GLOBAL POWER BALANCE AND LOCAL HEAT
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0.5 1 r. (s> Goldston IAEA-CN-50/A-
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IAEA-CN-50/A-VH-l 371 Separate Elec
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IAEA-CN-50/A-VII-l 373 4. SIMULATIO
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6. CONCLUSIONS IAEA-CN-50/A-VII-l 3
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SAWTOOTH ACTIVITY AND CURRENT DENSI
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-0.6 (keV) 6.6 6.4 6.2 6.0 5.8 IAEA
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IAEA-CN-50/A-VII-2 381 #15697 . 0 1
Page 409 and 410:
IAEA-CN-50/A-VII-2 383 radius. In a
Page 411:
IAEA-CN-50/A-VH-2 385 [11] Goldston
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388 NAGAYAMA et al. of the magnetic
Page 416 and 417:
390 NAGAYAMA et al. RECONNECTION RE
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392 NAGAYAMA et al. m/n=2/1 island
Page 421 and 422:
STABILITY OF TFTR PLASMAS IAEA-CN-5
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IAEA-CN-50/A-VII-4 397 the electron
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9 8 — 7 6 5 4 - 3 2 X • * • i
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0.5 ' 0.4 0.3 - 3 0.2 0.1 - 0 —r"
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0.4 0.3 0.2 0.1 n IAEA-CN-50/A-VH-4
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Ip(MA) 0.85 0.89 0.9 0.9 1.4 IAEA-C
Page 433:
IAEA-CN-50/A-VH-4 407 ACKNOWLEDGMEN
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410 AGIM et al. , , , , I , , , .,
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412 AGIM et al. to diminish and the
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414 AGIM et al. Hence, the preventi
Page 442 and 443:
416 MAUELetal. Small tokamak plasma
Page 444 and 445:
418 MAUELetal. 3. Mode structure of
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420 100- 350 MAUEL et al. RAOIUS (c
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STUDY OF PLASMA MHD STABILITY IN T-
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1.5 _ 1.0 >
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20 £ 15 - " 10 II 5 5 — ECH IAEA
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200 - IAEA-CN-S0/A-Vn-7 429 I I I I
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60 40 20 n / l IAEA-CN-S0/A-VII-7 4
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LU 30 - 20 - 10 - IAEA-CN-50/A-V1I-
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as if 200 - 100 -- 20 - I 10 - 15
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RELAXATION OF q PROFILE IN A HIGH B
Page 465 and 466:
0 0.5 1.0 IAEA-CN-50/A-VII-8 439 .
Page 467 and 468:
0 6 12 (Wall) r(cm) IAEA-CN-50/A-VH
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5. CONCLUSIONS IAEA-CN-50/A-VH-8 44
Page 472 and 473:
446 HENDERetal. An alternative meth
Page 474 and 475:
448 HENDER et al. and Jdriven(max)
Page 476 and 477:
450 HENDER et al. TJ :? Island V 6
Page 479 and 480:
IAEA-CN-50/A-VII-10 PARTICLE REMOVA
Page 481 and 482:
IAEA-CN-50/A-VH-10 455 3. POLOIDAL
Page 483 and 484:
X > o S 6 U- 2- 0 160 • 80 0 1 0.
Page 485 and 486:
IAEA-CN-S0/A-VH-10 459 between scoo
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THE ROLE OF LIMITERS AND WALLS IN I
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Shine through IAEA-CN-50/A-VH-ll 46
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3 01 £ "c t=! o E c 12 10 8 6 4 2
Page 493 and 494:
THE PLASMA BOUNDARY IN JET IAEA-CN-
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o x CO o 3.0 2.0 .2-0.5 'in c 0.3 1
Page 497 and 498:
1 10" IAEA-CN-50/A-VI1-12 LCFS LCFS
Page 499 and 500:
o •£ 0.15 'o = 0.05 C O J3 o 0.0
Page 501:
IAEA-CN-50/A-VIM2 475 densities, bu
Page 504 and 505:
478 LEONOV et al. 2. INSTALLATION A
Page 506 and 507:
480 LEONOV et al. &r (cm) 0.2 -0.2
Page 508 and 509:
482 LEONOV et al. Uo, at constant p
Page 510 and 511:
484 CHEETHAM et al. We present simu
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486 CHEETHAM et al. 0 20 40 60 30 1
Page 514 and 515:
488 CHEETHAM et al. o LU 3.0 2.8
Page 516 and 517:
490 CHEETHAM et al. sior CO 111 c o
Page 518 and 519:
492 CHEETHAM et al. reported from o
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IAEA-CN-S0/A-Vn-15 EXPERIMENTAL RES
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IAEA-CN-50/A-VII-15 497 800 (a) _ -
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IAEA-CN-50/A-VII-15 499 formation.
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300 4X10' 3 - IAEA-CN-50/A-VII-15 5
Page 529:
CONCLUSION IAEA-CN-50/A-VU-1S 503 W
Page 532 and 533:
506 KIKUCH1 et al. 1. INTRODUCTION
Page 534 and 535:
508 KIKUCHI et al. 1.0 o.s 1 — -
Page 536 and 537:
510 KIKUCHIetal. REFERENCES [1] ZAR
Page 539 and 540:
STUDY OF DENSITY LIMIT AND LOW q(aL
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IAEA-CN-50/E-I-l-l 515 1 2 3 4 5 ne
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/ / IAEA-CN-50/E-I-l-l 517 / / / /
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(J n 3 o ? 2 i o ' 1 IAEA-CN-50/E-M
Page 547 and 548:
0.03 - 0.02 - 0.01 - IAEA-CN-50/E-I
Page 549 and 550:
CO u CO "o IC 7 - 6 — 5 - 4 - 3 1
Page 551:
IAEA-CN-50/E-I-l-l REFERENCES 52 5
Page 554 and 555:
528 PRATER et al. 1. INTRODUCTION E
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530 PRATER et al. 0.8 0.6 0.4 0.2 n
Page 558 and 559:
532 PRATER et al. 1.5 x 10 19 m~ 3
Page 560 and 561:
534 PRATER et al. 10 1 0.75 0.25 0.
Page 562 and 563:
536 PRATER et al. added to 1.25 MW
Page 564 and 565:
538 PRATER et al. 2.0 1.5 1.0 0.5 /
Page 567 and 568:
INSIDE LAUNCH ELECTRON CYCLOTRON HE
Page 569 and 570:
0-20 0-15 a CO. 0-10 0-05 0-0 5S g.
Page 571 and 572:
IAEA-CN-50/E-I-3 545 0.25 • (a) 1
Page 573 and 574:
IAEA-CN-50/E-I-3 547 A/3 deduced fr
Page 575:
IAEA-CN-50/E-I-3 549 ECRH phases as
Page 578 and 579:
552 MOTOJIMA et al. ICRF and plasma
Page 580 and 581:
554 MOTOJIMA et al. (a) 0.6SneS0.9x
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556 MOTOJIMA et al. 0 20 W 60 80 10
Page 584 and 585:
558 5 4 3 2 1 0 60 40 20 0 la) cuto
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560 MOTOJIMA et al. 3 0.005 0 0.2 0
Page 589 and 590:
RF CURRENT DRIVE AND MHD INSTABILIT
Page 591 and 592:
IAEA-CN-50/E-I-5 565 80 PEC
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of x o o i L_ t IAEA-CN-50/E-I-5 56
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IAEA-CN-50/E-I-5 569 FIG. 5. Contou
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HEATING AND CONFINEMENT STUDIES WIT
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R 6 IAEA-CN-50/E-IM 0.5 10 1.5 Ne(r
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IAEA-CN-50/E-II-l FIG. 3. Total rad
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IAEA-CN-50/E-II-l 577 1.0 2.0 Time
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IAEA-CN-50/E-II-l 579 TABLE I. SUMM
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6. SAWTOOTH BEHAVIOUR IAEA-CN-50/E-
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IAEA-CN-50/E-II-2 LONG PULSE HIGH P
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IAEA-CN-50/E-II-2 585 23996 2 3 0 U
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IAEA-CN-50/E-II-2 587 TABLE I. a) C
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t a ce> 03 E cs o. otal 100 90 80 7
Page 617 and 618:
IAEA-CN-50/E-H-2 591 and confinemen
Page 619 and 620:
IAEA-CN-50/E-n-3 EXPERIMENTAL AND T
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§ 1PUTUDE ( $ #•14613 200 (a) 18
Page 623 and 624:
IAEA-CN-50/E-II-3 597 The results o
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to V. (a)' • \ \ \ \ \ \ w \'\ \\
Page 627 and 628:
IAEA-CN-50/E-II-3 601 cccurs progre
Page 629:
IAEA-CN-50/E-II-3 603 [5] CAMPBELL,
Page 632 and 633:
606 FUJII et al. 1. INTRODUCTION Se
Page 634 and 635:
608 140 " (0,0) PIC= l~ 3 MW 120 '
Page 636 and 637:
610 FUJII et al. ACKNOWLEDGEMENTS T
Page 638 and 639:
612 BATCHELOR et al. resolves this
Page 640 and 641:
614 BATCHELOR et al. •J5 1
Page 642 and 643:
616 BATCHELOR et al. to match asymp
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618 BATCHELOR et al. of T, R, and C
Page 646 and 647:
620 BATCHELOR et al. [3] SMITHE, D.
Page 648 and 649:
622 USHIGUSA et al. 1. INTRODUCTION
Page 650 and 651:
624 USHIGUSA et al. at f = 1.74 GHz
Page 652 and 653:
626 USHIGUSA et al. BT (T) (ms) ao
Page 654 and 655:
628 USHIGUSA et al. [2] JT-60 TEAM,
Page 656 and 657:
630 ITOH et al. , Breakdown 20 40 6
Page 658 and 659:
632 ITOH et al. 1.0 20 30 40 50 60
Page 660 and 661:
634 ITOH et al. 30 |20 a "" 10 n H=
Page 662 and 663:
636 ITOH et al. REFERENCES [1] ITOH
Page 664 and 665:
638 ALLADIO et al. generation of hi
Page 666 and 667:
640 ALLADIO et al. 4 T (keV) 3 2 -
Page 668 and 669:
642 ALLADIO et al. 3 ID 10 2 10' 10
Page 671 and 672:
IAEA-CN-50/E-ID-4 LOWER HYBRID WAVE
Page 673 and 674:
1000 - 500 1001— o — 2 35 IAEA-
Page 675 and 676:
10 10* 10 10 IAEA-CN-50/E-HI-4 649
Page 677 and 678:
IAEA-CN-50/E-III-4 651 density of t
Page 679 and 680:
IAEA-CN-50/E-IU-4 653 I I I I I I F
Page 681 and 682:
CURRENT DRIVE AND CONFINEMENT OF AN
Page 683 and 684:
1.0 -0.5 o - - 4.0 IAEA-CN-50/E-III
Page 685 and 686:
IAEA-CN-50/E-III-5 659 TABLE I. SUM
Page 687 and 688:
IAEA-CN-SO/E-in-S 661 0.4 RADIUS (m
Page 689 and 690:
10' Convection Dominates IAEA-CN-50
Page 691 and 692:
IAEA-CN-50/E-III-5 665 versus unbal
Page 693:
IAEA-CN-50/E-III-5 667 [11] ZARNSTO
Page 696 and 697:
670 SIMONEN et al. Neutral beam cur
Page 698 and 699:
672 SIMONEN et al. 1.6 2.0 FIG. 3.
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674 SIMONEN et al. MHD modes, obser
Page 702 and 703:
676 SIMONEN et al. toroidal drift o
Page 704 and 705:
678 SIMONEN et al. occurs near the
Page 707 and 708:
NEW CURRENT DRIVE AND CONFINEMENT T
Page 709 and 710:
IAEA-CN-50/E-III-7 683 is typically
Page 711 and 712:
IAEA-CN-S0/E-III-7 685 plasma beta
Page 713 and 714:
IAEA-CN-50/E-III-7 687 The equilibr
Page 715:
IAEA-CN-50/E-III-7 689 [8] McGUIRE,
Page 718 and 719:
692 100 a 10- 0.1 WILSON et al. •
Page 720 and 721:
694 WILSON et al. 3. Plasma Heating
Page 722 and 723:
696 WILSON et al. I 3 i - • / Tim
Page 725 and 726:
INVESTIGATION OF ICRH ON THE TUMAN-
Page 727 and 728:
~x o X •9to 12 1 11 10 180 s - 12
Page 729 and 730:
400 - 300 - 200 - I 100 - 35 / 1 ,
Page 731 and 732:
5 - IAEA-CN-50/E-IV-2 r (cm) FIG. 7
Page 733 and 734:
IAEA-CN-50/E-IV-3 CONVERSION AND CY
Page 735 and 736:
IAEA-CN-50/E-IV-3 709 bution, e(j,
Page 737 and 738:
IAEA-CN-S0/E-IV-3 711 FIG. 3. kxPd
Page 739 and 740:
IAEA-CN-50/E-IV-3 713 3. NON-LOCAL
Page 741 and 742:
x exp | ds" ' u ' x -oosgn u d fiV2
Page 743 and 744:
IAEA-CN-50/E-IV-3 717 x If {sin i [
Page 745:
IAEA-CN-5O/E-IV-3 719 2. A non-loca
Page 748 and 749:
722 MOREAU et al. =t _» Here, K is
Page 750 and 751:
724 MOREAU et al. FIG. 1. Modulus o
Page 752 and 753:
726 MOREAU et al. REFERENCES [1] MA
Page 754 and 755:
728 YASAKA et al. 2. EFFICIENT PLAS
Page 756 and 757:
730 YASAKA et al. '£ 1 0.5 0 4 Pne
Page 758 and 759:
732 YASAKA et al. WT-3 1 2 Q,f C 10
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734 invi p o p p •^ CJ -^ o IO o
Page 762 and 763:
736 YAMAMOTO et al. (A) OJ — o (A
Page 764 and 765:
738 YAMAMOTO et al. of Tsx =1.5 keV
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740 PEREVERZEV current drive produc
Page 768 and 769:
742 PEREVERZEV 300 - - 150 ne (10 1
Page 770 and 771:
744 PEREVERZEV 0.2- -0.2- 0.1X10 19
Page 772 and 773:
746 PEREVERZEV The dependences of l
Page 774 and 775:
748 PORKOLAB et al. ASPECT RATIO FI
Page 776 and 777:
750 PORKOLAB et al. 1.0 _, 0.8 1 0.
Page 778 and 779:
752 PORKOLAB et al. X D E o Q_ 1.8
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754 LUO et al. - o £ 3 §. II Ml "
Page 782 and 783:
756 LUO et al. 20 10 ATe ( 1 m11 1
Page 785 and 786:
IAEA-CN-50/E-IV-10 MICROWAVE HEATIN
Page 787 and 788:
n MCPAT _ Analysis IAEA-CN-50/E-IV-
Page 789 and 790:
IAEA-CN-50/E-IV-10 763 3. QUASI-LIN
Page 791 and 792:
IAEA-CN-50/E-IV-10 765 In the limit
Page 793 and 794:
IAEA-CN-50/E-IV-ll SECOND ELECTRON
Page 795 and 796:
IAEA-CN-50/E-IV-ll 769 FIG. ]. Real
Page 797 and 798:
-0.2 IAEA-CN-50/E-IV-ll 771 FIG. 3.
Page 799:
IAEA-CN-50/E-IV-ll 773 gests that i
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