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90 STRAIT et al. central soft x-ray emission (a.u.) 1400 1800 2200 2600 TIME (ms) Be AMPLITUDE SPECTRUM (SHOT 55771) n-3 BURST PRECEDES GROWTH OF n-2 MODE 10 20 30 40 FREQUENCY {kHz) FIG. 4. (a) Time traces for a typical beta collapse associated with low-n MHD activity (discharge 55771). B = 0.9 T, I = 1.0 MA, q9S = 3.1, 0 < 5.3%; (b) time-dependent amplitude spectra of % from a Mirnov loop at the outer wall midplane. 3000
s.o • .5 (a) IAEA-CN-50/A-II-l 91 360 0 60 120 180 2*0 300 360 POLOIDAL ANGLE (DEGREES) FIG. 5. Resistive mode calculation for n = 1 beta collapse (55791): (a) calculated perturbation of poloidal magnetic flux; (b) phase and amplitude of Mirnov oscillations versus poloidal angle, comparing measured (•) and calculated (o) values. The low-n modes which cause beta saturation and collapse cannot be attributed to ideal modes. Their growth rates are slow (typically r ~ 10 4 TAifven) and they can persist unchanged for times approaching the resistive time of the plasma. Ideal stability calculations using GATO [13] (discussed further below) show that the point where the n = 4, 3, and 2 modes are first observed is usually far from the kink mode stability limit. These low-n modes are most consistent with pressure driven resistive instabilities. The three-dimensional resistive code CART—II [14] was used to analyze a discharge similar to that of Fig. 4, at a time during the large n = 1 oscillation. The nonlinear calculation predicts a predominantly ?n = 2/n = 1 instability, as shown in Fig. 5. The predicted mode structure agrees well with soft X-ray and magnetic fluctuation measurements, including the coupling to higher poloidal mode numbers which dominates the structure along the inboard wall. The nonlinear calculation was halted when the calculated value of Bg/Be at the outer wall was 1%, equal to the measured value at the time when the n = 1 mode in the discharge of Fig. 4 stopped rotating and the rate of energy loss accelerated. At this point, the width of the 2/1 island was calculated to be 11 cm and flux surfaces outside of the q = 2 surface had started to become stochastic.
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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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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 81 and 82: 10 0.5 Pulse No: 15376 n(He')/ne=1.
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Page 85 and 86: 10 E X 4 H-mode y 0.2 0.4 0.6 0.8 1
Page 87 and 88: IAEA-CN-50/A-I-3 61 where V is the
Page 89 and 90: IAEA-CN-50/A-I-3 63 confinement deg
Page 91: IAEA-CN-50/A-I-3 65 References [1 ]
Page 94 and 95: 68 JT-60 TEAM T. TANAKA, Y. TANAKA,
Page 96 and 97: Ip = 3.2 MA lp = 2.7 MA JT-60TEAM R
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Page 102 and 103: 76 JT-60TEAM 4.5 5.0 5.5 6.0 6.5 7.
Page 104 and 105: 78 JT-60TEAM 250 "(a) 200 150 50 n
Page 106 and 107: 80 JT-60 TEAM The further developme
Page 109 and 110: STABILITY OF HIGH BETA DISCHARGES I
Page 111 and 112: IAEA-CN-50/A-II-l 85 a typical plas
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Page 115: IAEA-CN-50/A-IM 89 absence of the l
Page 119 and 120: IAEA-CN-50/A-II-l 93 stability limi
Page 121: IAEA-CN-50/A-II-l 95 [6] STAMBAUGH,
Page 124 and 125: 98 OKABAYASHI et al. PBX-M maximall
Page 126 and 127: 100 1 .0 .6 .0 -.2 -.4 -.6 1.11 CO
Page 128 and 129: 102 0.5 OKABAYASHI et al. Indentati
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Page 132 and 133: 106 OKABAYASHI et al. §1 •a J i
Page 134 and 135: 108 OKABAYASHI et al. -2 1 • •
Page 137 and 138: MHD ACTIVITIES AND RELATED IMPURITY
Page 139 and 140: 0.5 IAEA-CN-50/A-H-3 113 FIG. 1. St
Page 141 and 142: 0) a. II E IAEA-CN-50/A-H-3 115 1 1
Page 143 and 144: IAEA-CN-50/A-II-3 117 These observa
Page 145: 6. CONCLUSIONS IAEA-CN-50/A-II-3 11
Page 148 and 149: 122 GAO et al. With hydrogen plasma
Page 150 and 151: 124 GAO et al. P—3.0 r—8.5 SHOT
Page 152 and 153: 126 GAO et al. a) M >
Page 154 and 155: 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
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Page 163 and 164: IAEA-CN-50/A-D-5-2 INVESTIGATION OF
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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
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HEATING OF PEAKED DENSITY PROFILES
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Yd o g a> - c 4 _n ...— 0) n 12 t
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1.3 I" 1 |03 C 0.5 i: 12 8 4 n - Te
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IAEA-CN-50/A-IV-l 221 1 2 3 Q,_-2ff
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2 q(o) 1- 10 1 U • O • IAEA-CN-
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0.3 f0.2 1 5" 0.1 IAEA-CN-50/A-IV-l
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IAEA-CN-50/A-IV-l 227 APPENDIX I TH
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IAEA-CN-50/A-IV-2 PELLET INJECTION
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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
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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
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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
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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
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352 EVANS et al. REFERENCES [1] KAR
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354 BAKOS et al. The radiation of t
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356 BAKOS et al. < + s 5 2 1 5 2 10
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358 BAKOS et al. REFERENCES [1] BAK
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360 STfiCKEL et al. A quantitative
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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
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IAEA-CN-50/A-VII-2 383 radius. In a
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IAEA-CN-50/A-VH-2 385 [11] Goldston
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388 NAGAYAMA et al. of the magnetic
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390 NAGAYAMA et al. RECONNECTION RE
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392 NAGAYAMA et al. m/n=2/1 island
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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
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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
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416 MAUELetal. Small tokamak plasma
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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
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0 0.5 1.0 IAEA-CN-50/A-VII-8 439 .
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0 6 12 (Wall) r(cm) IAEA-CN-50/A-VH
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5. CONCLUSIONS IAEA-CN-50/A-VH-8 44
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446 HENDERetal. An alternative meth
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448 HENDER et al. and Jdriven(max)
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450 HENDER et al. TJ :? Island V 6
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IAEA-CN-50/A-VII-10 PARTICLE REMOVA
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IAEA-CN-50/A-VH-10 455 3. POLOIDAL
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X > o S 6 U- 2- 0 160 • 80 0 1 0.
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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
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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
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1 10" IAEA-CN-50/A-VI1-12 LCFS LCFS
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o •£ 0.15 'o = 0.05 C O J3 o 0.0
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IAEA-CN-50/A-VIM2 475 densities, bu
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478 LEONOV et al. 2. INSTALLATION A
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480 LEONOV et al. &r (cm) 0.2 -0.2
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482 LEONOV et al. Uo, at constant p
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484 CHEETHAM et al. We present simu
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486 CHEETHAM et al. 0 20 40 60 30 1
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488 CHEETHAM et al. o LU 3.0 2.8
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490 CHEETHAM et al. sior CO 111 c o
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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
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CONCLUSION IAEA-CN-50/A-VU-1S 503 W
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506 KIKUCH1 et al. 1. INTRODUCTION
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508 KIKUCHI et al. 1.0 o.s 1 — -
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510 KIKUCHIetal. REFERENCES [1] ZAR
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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
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0.03 - 0.02 - 0.01 - IAEA-CN-50/E-I
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CO u CO "o IC 7 - 6 — 5 - 4 - 3 1
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IAEA-CN-50/E-I-l-l REFERENCES 52 5
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528 PRATER et al. 1. INTRODUCTION E
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530 PRATER et al. 0.8 0.6 0.4 0.2 n
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532 PRATER et al. 1.5 x 10 19 m~ 3
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534 PRATER et al. 10 1 0.75 0.25 0.
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536 PRATER et al. added to 1.25 MW
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538 PRATER et al. 2.0 1.5 1.0 0.5 /
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INSIDE LAUNCH ELECTRON CYCLOTRON HE
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0-20 0-15 a CO. 0-10 0-05 0-0 5S g.
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IAEA-CN-50/E-I-3 545 0.25 • (a) 1
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IAEA-CN-50/E-I-3 547 A/3 deduced fr
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IAEA-CN-50/E-I-3 549 ECRH phases as
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552 MOTOJIMA et al. ICRF and plasma
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554 MOTOJIMA et al. (a) 0.6SneS0.9x
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556 MOTOJIMA et al. 0 20 W 60 80 10
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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
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RF CURRENT DRIVE AND MHD INSTABILIT
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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
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IAEA-CN-50/E-H-2 591 and confinemen
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IAEA-CN-50/E-n-3 EXPERIMENTAL AND T
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§ 1PUTUDE ( $ #•14613 200 (a) 18
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IAEA-CN-50/E-II-3 597 The results o
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to V. (a)' • \ \ \ \ \ \ w \'\ \\
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IAEA-CN-50/E-II-3 601 cccurs progre
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IAEA-CN-50/E-II-3 603 [5] CAMPBELL,
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606 FUJII et al. 1. INTRODUCTION Se
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608 140 " (0,0) PIC= l~ 3 MW 120 '
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610 FUJII et al. ACKNOWLEDGEMENTS T
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612 BATCHELOR et al. resolves this
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614 BATCHELOR et al. •J5 1
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616 BATCHELOR et al. to match asymp
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618 BATCHELOR et al. of T, R, and C
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620 BATCHELOR et al. [3] SMITHE, D.
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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.
Page 700 and 701:
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
Page 760 and 761:
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
Page 766 and 767:
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
Page 780 and 781:
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
Page 802:
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