- Page 2:
The cover picture shows the inside
- Page 6 and 7:
AFGHANISTAN ALBANIA ALGERIA ARGENTI
- Page 8 and 9:
PLASMA PHYSICS AND CONTROLLED NUCLE
- Page 10 and 11:
EDITORIAL NOTE The Proceedings have
- Page 12 and 13:
A. Kaminaga, T. Kaneko, T. Kato, M.
- Page 14 and 15:
Improved confinement regimes with O
- Page 16 and 17:
Tokamak with strong magnetic field
- Page 18 and 19:
Resonant island divertor experiment
- Page 20 and 21:
Particle removal capabilities of th
- Page 22 and 23:
Inside launch electron cyclotron he
- Page 24 and 25:
T. Hjima, S. Ishida, K. Itami, T. I
- Page 26 and 27:
T. Yamauchi, I. Nakazawa, K. Hasega
- Page 29 and 30:
ARTSIMOVICH MEMORIAL LECTURE C. MAI
- Page 31 and 32:
IAEA-CN-50/A-0 5 ceptible to fast r
- Page 33 and 34:
IAEA-CN-50/A-0 7 fusion power plant
- Page 35 and 36:
FIRST EXPERIMENTS IN TORE SUPRA EQU
- Page 37 and 38:
IAEA-CN-50/A-I-1 11 Supra is the fi
- Page 39 and 40:
IAEA-CN-50/A-I-1 13 poloidal field
- Page 41 and 42:
nee id interfere >res an j-> 1 O E
- Page 43 and 44:
i I •O OJ) — '5 c IS 2 HI 1ZI _
- Page 45 and 46:
5.' ' *[Wbl t. 3. 2. 1. _ _ X IAEA-
- Page 47 and 48:
nl 30 .29 .28 .27 26 .25 .24 .23 22
- Page 49 and 50:
IAEA-CN-50/A-I-1 However, reasonabl
- Page 51 and 52:
IAEA-CN-50/A-I-1 25 will make it po
- Page 53 and 54:
IAEA-CN-50/A-I-2 AN OVERVIEW OF TFT
- Page 55 and 56:
IAEA-CN-50/A-I-2 29 inner belt limi
- Page 57 and 58:
IAEA-CN-50/A-I-2 31 0 10 20 TOTAL P
- Page 59 and 60:
5 DC LU LU 3 - 1 - Q Q A 1 A IAEA-C
- Page 61 and 62:
IAEA-CN-50/A-I-2 35 The question ar
- Page 63 and 64:
0.20 0.15 0.10 Rp= 2.45 m a = 0.79
- Page 65 and 66:
: . • • 1 IAEA-CN-50/A-I-2 39 1
- Page 67 and 68:
LATEST JET RESULTS AND FUTURE PROSP
- Page 69 and 70:
Parameter Plasma major radius (Ro)
- Page 71 and 72:
1500 IAEA-CN-50/A-I-3 45 2 4 I, (MA
- Page 73 and 74:
IAEA-CN-50/A-I-3 47 3.0 3.5 Major r
- Page 75 and 76:
I 15 10 5 0 IAEA-CN-50/A-I-3 49 V \
- Page 77 and 78:
IAEA-CN-50/A-I-3 51 Magnetic measur
- Page 79 and 80:
0.8 0.6 IAEA-CN-50/A-I-3 53 -0.2 12
- Page 81 and 82:
10 0.5 Pulse No: 15376 n(He')/ne=1.
- Page 83 and 84:
IAEA-CN-50/A-I-3 57 5 10 15 [Pt-dW/
- 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
- Page 98 and 99:
72 JT-60TEAM E5695 0 1 2 3 4 5 6 7
- Page 100 and 101:
74 JT-60TEAM 3 : LIH *3.1HA 2.8HA A
- 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
- Page 113 and 114:
0.5- 0- 0.8- 0.4- 0.0- IAEA-CN-50/A
- Page 115 and 116:
IAEA-CN-50/A-IM 89 absence of the l
- Page 117 and 118:
s.o • .5 (a) IAEA-CN-50/A-II-l 91
- 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
- Page 130 and 131:
104 OKABAYASHI et al. 40 30 I I I I
- 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
- 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 and 206:
IAEA-CN-50/A-III-2 179 APPENDIX I T
- Page 207:
IAEA-CN-50/A-IH-2 181 [16] Bishop,
- 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-
- 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
- Page 255 and 256:
IAEA-CN-50/A-IV-2 PELLET INJECTION
- Page 257 and 258:
3 - 2 - 1 - IAEA-CN-50/A-IV-2 231 1
- 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
- Page 279 and 280:
IAEA-CN-SO/AIV-4 253 FIG. 4. (a) Di
- Page 281:
IAEA-CN-50/A-IV-4 255 The fusion pe
- 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 291 and 292:
ENERGY CONFINEMENT WITH AUXILIARY H
- Page 293 and 294:
E6950(Bi=4.0T) E6956(Bt = 2.7T) °4
- Page 295 and 296:
E7558 • IMPROVED 5 6 TIME (S) IAE
- Page 297 and 298:
7.0 E - 1 0.0 7.0 0.0 =— \ n; - T
- Page 299:
IAEA-CN-50/A-V-1 273 [9] SHIMOMURA,
- Page 302 and 303:
276 ASHRAF et al. However, the conv
- Page 304 and 305:
278
- Page 306 and 307:
280 ASHRAF et al. Modulation amplit
- Page 308 and 309:
282 KIMet al. (a) (b) 410 420 TIME
- Page 310 and 311:
284 KIM et al. (b) o 3
- Page 312 and 313:
286 KIM et ah In summary, we observ
- Page 314 and 315:
288 KAWAHATA et al. TEXT tokamak, t
- Page 316 and 317:
290 KAWAHATA et al. ^ 30 °- S-200.
- Page 318 and 319:
292 KAWAHATA et al. 0 6 12 18 24 ra
- Page 320 and 321:
294 WOOTTON et al. 1. Particle tran
- Page 322 and 323:
296 10' N 10° E gio- 1 O (a) 10" 0
- Page 324 and 325:
298 WOOTTON et al. ne=3xl0 19 m- 3
- Page 326 and 327:
300 ZURRO et al. FIG. 1. Variation
- Page 328 and 329:
302 ZURRO et al. Mo) 6 (10"cm- 3 )
- Page 330 and 331:
304 ZURRO et al. -140 50 100 f(kHz)
- Page 333 and 334:
TRANSPORT STUDIES ON TFTR UTILIZING
- Page 335 and 336:
IAEA-CN-50/A-V-4 309 uses the TRANS
- Page 337 and 338:
5 g 30 20 < 2.0 Q § 1.0 i 0.5 10 1
- Page 339 and 340:
IAEA-CN-50/A-V-4 313 the laser-blow
- Page 341 and 342:
IAEA-CN-S0/A-V-4 315 on working gas
- Page 343 and 344:
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
- Page 347:
IAEA-CN-50/A-V-4 321 [12] RADEZTSKY
- Page 350 and 351:
324 DONNE et al. E CO o FIG. 1. Sho
- Page 352 and 353:
326 DONNE et al. 350 300 250 200 15
- Page 354 and 355:
328 DONNE et al. 1.0 0.8 - 0.6 - t
- Page 357 and 358:
RECENT TEXTOR RESULTS TEXTOR TEAM (
- Page 359 and 360:
IAEA-CN-50/A-VI-l 333 line-radiatio
- Page 361 and 362:
IAEA-CN-50/A-VI-l 335 These measure
- Page 363 and 364:
q(r] 3- 2- 1- - IAEA-CN-50/A-VI-l 3
- Page 365 and 366:
IAEA-CN-50/A-VI-l 339 FIG. 4. Sawto
- Page 367 and 368:
IAEA-CN-S0/A-VI-2-1 RESONANT ISLAND
- Page 369 and 370:
IAEA-CN-50/A-VI-2-1 343 • «• >
- Page 371:
IAEA-CN-50/A-VI-2-1 345 tons. This
- Page 374 and 375:
348 EVANS et al. JIPP T-IIU ( minor
- Page 376 and 377:
350 EVANS et al. FIG. 3. High speed
- Page 378 and 379:
352 EVANS et al. REFERENCES [1] KAR
- Page 380 and 381:
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
- Page 386 and 387:
360 STfiCKEL et al. A quantitative
- Page 388 and 389:
362 STOCKEL et al. This and other f
- Page 390 and 391:
364 STOCKEL et al. 15 I 10 "" 5 0 (
- Page 393 and 394:
GLOBAL POWER BALANCE AND LOCAL HEAT
- Page 395 and 396:
0.5 1 r. (s> Goldston IAEA-CN-50/A-
- Page 397 and 398:
IAEA-CN-50/A-VH-l 371 Separate Elec
- Page 399 and 400:
IAEA-CN-50/A-VII-l 373 4. SIMULATIO
- Page 401 and 402:
6. CONCLUSIONS IAEA-CN-50/A-VII-l 3
- Page 403 and 404:
SAWTOOTH ACTIVITY AND CURRENT DENSI
- Page 405 and 406:
-0.6 (keV) 6.6 6.4 6.2 6.0 5.8 IAEA
- Page 407 and 408:
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
- Page 414 and 415:
388 NAGAYAMA et al. of the magnetic
- Page 416 and 417:
390 NAGAYAMA et al. RECONNECTION RE
- Page 418 and 419:
392 NAGAYAMA et al. m/n=2/1 island
- Page 421 and 422:
STABILITY OF TFTR PLASMAS IAEA-CN-5
- Page 423 and 424:
IAEA-CN-50/A-VII-4 397 the electron
- Page 425 and 426:
9 8 — 7 6 5 4 - 3 2 X • * • i
- Page 427 and 428:
0.5 ' 0.4 0.3 - 3 0.2 0.1 - 0 —r"
- Page 429 and 430:
0.4 0.3 0.2 0.1 n IAEA-CN-50/A-VH-4
- Page 431 and 432:
Ip(MA) 0.85 0.89 0.9 0.9 1.4 IAEA-C
- Page 433:
IAEA-CN-50/A-VH-4 407 ACKNOWLEDGMEN
- Page 436 and 437:
410 AGIM et al. , , , , I , , , .,
- Page 438 and 439:
412 AGIM et al. to diminish and the
- Page 440 and 441:
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
- Page 446 and 447:
420 100- 350 MAUEL et al. RAOIUS (c
- Page 449 and 450:
STUDY OF PLASMA MHD STABILITY IN T-
- Page 451 and 452:
1.5 _ 1.0 >
- Page 453 and 454:
20 £ 15 - " 10 II 5 5 — ECH IAEA
- Page 455 and 456:
200 - IAEA-CN-S0/A-Vn-7 429 I I I I
- Page 457 and 458:
60 40 20 n / l IAEA-CN-S0/A-VII-7 4
- Page 459 and 460:
LU 30 - 20 - 10 - IAEA-CN-50/A-V1I-
- Page 461 and 462:
as if 200 - 100 -- 20 - I 10 - 15
- Page 463 and 464:
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
- Page 469:
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
- Page 487 and 488:
THE ROLE OF LIMITERS AND WALLS IN I
- Page 489 and 490:
Shine through IAEA-CN-50/A-VH-ll 46
- Page 491 and 492:
3 01 £ "c t=! o E c 12 10 8 6 4 2
- Page 493 and 494:
THE PLASMA BOUNDARY IN JET IAEA-CN-
- Page 495 and 496:
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
- Page 512 and 513:
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
- Page 521 and 522: IAEA-CN-S0/A-Vn-15 EXPERIMENTAL RES
- Page 523 and 524: IAEA-CN-50/A-VII-15 497 800 (a) _ -
- Page 525 and 526: IAEA-CN-50/A-VII-15 499 formation.
- Page 527 and 528: 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
- Page 541 and 542: IAEA-CN-50/E-I-l-l 515 1 2 3 4 5 ne
- Page 543 and 544: / / IAEA-CN-50/E-I-l-l 517 / / / /
- Page 545 and 546: (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
- Page 556 and 557: 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 568 and 569: 542 ASHRAF et al. experiments on FT
- Page 570 and 571: 544 1.1 ASHRAF et al. Absorption zo
- Page 572 and 573: 546 ASHRAF et al. cm from the magne
- Page 574 and 575: 548 ASHRAF et al. 20 4 I ,5 £ 10 .
- Page 577 and 578: HIGH POWER ECRH AND ICRF HEATING EX
- Page 579 and 580: IAEA-CN-50/E-I-4 553 0-1 Jr FIG. 2.
- Page 581 and 582: 1.2. ICRF experiments IAEA-CN-50/E-
- Page 583 and 584: IAEA-CN-50/E-I-4 557 This effect mi
- Page 585 and 586: 100 50 4th 2.0 3,0 IAEA-CN-50/E-I-4
- Page 587: IAEA-CN-50/E-I-4 561 [3] SATO, M.,
- Page 590 and 591: 564 * 0 2 ' 0 20 ? I 0 § 0 50 100
- Page 592 and 593: 566 TANAKA et al. and one order sma
- Page 594 and 595: 568 TANAKA et al. Figures 3(a)-(i)
- Page 596 and 597: 570 TANAKA et al. [2] TANAKA, S., e
- Page 598 and 599: 572 WEYNANTS et al. Important aniso
- Page 600 and 601: 574 WEYNANTS et al. 05- (c) V. V DI
- Page 602 and 603: 576 WEYNANTS et al. 3 eff.o 2 1 •
- Page 604 and 605: 578 WEYNANTS et al. 2.06 2.10 2.14
- Page 606 and 607: 580 20 EH.rh [kJl WEYNANTS et al. 3
- Page 608 and 609: 582 WEYNANTS et al. [II] JACQUINOT,
- Page 610 and 611: 584 NOTERDAEME et al. in the start-
- Page 612 and 613: 586 NOTERDAEME et al.
- Page 614 and 615: 588 NOTERDAEME et al. with the time
- Page 616 and 617:
590 NOTERDAEME et al. the small imp
- Page 618 and 619:
592 NOTERDAEME et al. 13] NOTERDAEM
- Page 620 and 621:
594 START et al. sustained for 1.2
- Page 622 and 623:
596 START et al. 300 200 Te (eV) 10
- Page 624 and 625:
598 START et al. GAMMA YIELD COUNTS
- Page 626 and 627:
600 START et al. 45 t(S) Onset of s
- Page 628 and 629:
602 START et al. and the energy con
- Page 631 and 632:
SECOND HARMONIC ICRF HEATING EXPERI
- Page 633 and 634:
,01) |c= 0.4 0.2 0 2 I 0 3 2 • 1
- Page 635 and 636:
IAEA-CN-50/E-II-4 609 1 1 I 1 I 1 1
- Page 637 and 638:
IAEA-CN-50/E-II-5 FULL-WAVE MODELIN
- Page 639 and 640:
IAEA-CN-50/E-II-5 613 When Eq. (4)
- Page 641 and 642:
IAEA-CN-50/E-II-5 615 the equations
- Page 643 and 644:
IAEA-CN-50/E-H-5 617 I i i i I I I
- Page 645 and 646:
1.0 0.9 0.8 0.7 1 0.6 10.5 1 0.4 0.
- Page 647 and 648:
LOWER HYBRID EXPERIMENTS IN JT-60 K
- Page 649 and 650:
- 2t ji IplMA) OIV LIM 0.7 - A 1.0
- Page 651 and 652:
'E - 3 "2 2 - 2 le? Ip(MA) 0.7 1.0
- Page 653 and 654:
IAEA-CN-SO/E-m-l 627 circles are da
- Page 655 and 656:
STEADY STATE CURRENT DRIVE BY LOWER
- Page 657 and 658:
45 2 30 a. " 15 0 7 e s 9 2.5 : ic
- Page 659 and 660:
1/1 z 3 163- IAEA-CN-50/E-III-2 633
- Page 661 and 662:
50* 70" 90' 110" 130' 150' 170* A*
- Page 663 and 664:
IAEA-CN-50/E-III-3 LOWER HYBRID HEA
- Page 665 and 666:
1.0 0.8 - _ OOnrr IAEA-CN-50/E-HI-3
- Page 667 and 668:
-4 IAEA-CN-50/E-HI-3 641 FIG. 3. Sa
- Page 669:
IAEA-CN-50/E-III-3 643 stronger emi
- Page 672 and 673:
646 BUDNIKOV et al. 100 50 34 36 38
- Page 674 and 675:
648 BUDN1K0V et al. 2 E (keV) F/G.
- Page 676 and 677:
650 BUDNIKOV et a). » 4 t 660 f (M
- Page 678 and 679:
652 BUDNIKOV et al. •a I -a 10' 1
- Page 680 and 681:
654 BUDNIKOV etal. 0.5 CM* ne(x10 1
- Page 682 and 683:
656 SCOTT et al. 1. Introduction A
- Page 684 and 685:
658 SCOTT et al. FIG. 2. Central ro
- Page 686 and 687:
660 SCOTT et al. 30 25 20 - / 1 10
- Page 688 and 689:
662 SCOTT et al. The TFTR "supersho
- Page 690 and 691:
664 SCOTT et al. Z3 5. 2 ? 1 Ge XXX
- Page 692 and 693:
666 SCOTT et al. to drive most or a
- Page 695 and 696:
DIII-D NEUTRAL BEAM CURRENT DRIVE E
- Page 697 and 698:
IAEA-CN-50/E-III-6 671 2. NEUTRAL B
- Page 699 and 700:
3.0 0.0 0.2 0.0 0.2 0.0 30.0 SXR (r
- Page 701 and 702:
IAEA-CN-50/E-HKS 675 obtained and i
- Page 703 and 704:
0.5- o.o -1 0.2- 0.0- 1.0- 0.6- 4.0
- Page 705:
IAEA-CN-50/E-HI-6 679 [17] STRAIT,
- Page 708 and 709:
682 OHKAWA et al. 2. CURRENT DRIVE
- Page 710 and 711:
684 OHKAWA et al. In terms of the h
- Page 712 and 713:
686 OHKAWA et al. regime. For ut <
- Page 714 and 715:
688 OHKAWA et al. while holding the
- Page 717 and 718:
ICRF HEATING ON THE TFTR TOKAMAK FO
- Page 719 and 720:
IAEA-CN-50/E-IV-l 693 4 He plasma a
- Page 721 and 722:
300 IAEA-CN-50/E-IV-l 695 -10 o 10
- Page 723:
5. Conclusions IAEA-CN-50/E-IV-l 69
- Page 726 and 727:
700 ASKINASI et al. 0 120 , 60 RF 1
- Page 728 and 729:
702 ASKINASI et al. 240 - \ -3 \ J
- Page 730 and 731:
704 ASKINASI et al. TABLE I. LOCATI
- Page 732 and 733:
706 ASKINASI et al. REFERENCES [1]
- Page 734 and 735:
708 KASILOV et al. current drive me
- Page 736 and 737:
710 KASILOV et al. to the two-ion h
- Page 738 and 739:
712 KASILOV et al. with the FW exci
- Page 740 and 741:
714 KASILOV et al. Similarly, takin
- Page 742 and 743:
716 KASILOV et al. If the resonant
- Page 744 and 745:
718 KASILOVetal. If eh < e,, Eq. (1
- Page 747 and 748:
IAEA-CN-50/E-IV-4 FULL WAVE SOLUTIO
- Page 749 and 750:
with IAEA-CN-50/E-IV-4 723 H;(r) =
- Page 751 and 752:
3000 m 2000 1000 0 1AEA-CN-50/E-IV-
- Page 753 and 754:
IAEA-CN-50/E-IV-5 EXPERIMENTS ON EF
- Page 755 and 756:
IAEA-CN-50/E-IV-5 729 0 ""'"10 20 3
- Page 757 and 758:
IAEA-CN-50/E-IV-5 731 A, for a net
- Page 759 and 760:
IMPROVEMENT OF RF CURRENT DRIVE DEN
- Page 761 and 762:
IAEA-CN-S0/E-IV-6 735 A fast wave (
- Page 763 and 764:
IAEA-CN-50/E-IV-6 737 electrons. Th
- Page 765 and 766:
IAEA-CN-50/E-IV-7 NON-INDUCTIVE STA
- Page 767 and 768:
300 200 - 100 - IAEA-CN-50/E-IV-7 7
- Page 769 and 770:
IAEA-CN-50/E-IV-7 743 are related t
- Page 771 and 772:
IAEA-CN-50/E-IV-7 745 TABLE I. CHAR
- Page 773 and 774:
ACCESS TO SECOND STABILITY VIA PROF
- Page 775 and 776:
6 5 4 w 3 2 1 0 IAEA-CN-50/E-IV-8 7
- Page 777 and 778:
IAEA-CN-50/E-IV-8 751 10 15 20 RF C
- Page 779 and 780:
IAEA-CN-50/E-IV-9 ELECTRON CYCLOTRO
- Page 781 and 782:
IAEA-CN-50/EIV-9 755 The second mec
- Page 783:
IAEA-CN-50/E-IV-9 757 In our case,
- Page 786 and 787:
760 COHEN et al. concept of using p
- Page 788 and 789:
762 COHEN et al. TABLE I. REPRESENT
- Page 790 and 791:
764 COHEN et al. 20 ECH power P (MW
- Page 792 and 793:
766 COHEN et al. [3] COHEN, B.I., e
- Page 794 and 795:
768 electron velocity distribution
- Page 796 and 797:
770 PESlC -02 FIG. 2. Real and imag
- Page 798 and 799:
772 PESlC FIG. 5. Real and imaginar
- Page 801 and 802:
CHAIRMEN OF SESSIONS Session A-I J.
- Page 804:
INTERNATIONAL ATOMIC ENERGY AGENCY