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1 TOKAMAK

2

3 1.TOKAMAK ITER----- TOKAMAK 016 D-T

4 1. MHD ne,te). (ne

5 .

6 1958 ( 1916 ) ( 19619)

7 back

8

9 ack

10 ( ,

11 Light Amplification by Stimulated Emission of Radiation Laser 0,,,

12 1... Λ

13

14

15

16

17

18

19

20

21 ,,..

22 .,,,

23

24 e c ( t) = Ac cos( ω ct + ϕc )

25 Q Q

26 Q 10 9 ~ 10 1 W

27

28

29

30 A r A = A e 0 r / ω

31 x d = [ d d 1/ 0 + (4λ / π )( x / 0 )]

32 f d1d 1 1 ) ( 1 ) (1 1 1 λ πd f f l d d + = Z1Z ]} )) /( ( ) /[( ){ ( 1 ' λ πd f l f f l f l + =

33

34 m c c m c ν ν ν ν ν ν + = ) ( qc nl / = ν CO YAG ν ν α = = L L T

35 D-H T-H Mev (4 1 : 1 10

36 50 TammSakharov TOKAMAK 1968Artsimovich T-3 1keV 1969 Pease T-3, T-3

37

38 ITER Thomson Scattering (Core)* Te,ne Thomson Scattering (Edge) Te,ne Thomson Scattering (X- Point) Te,ne Thomson Scattering (Divertor) Te,ne Toroidal Interferometric/ Polarimetric System* ne Polarimetric System (Pol. Magnetic Field Meas.) B Collective Scattering System ne( ) Laser Induced Fluorescence He

39 v E S dr V 3 v v n( r, t)exp[ i( K i v K S ) r] K=K S -K i K i dump K S K De P s v E s = v E sj j + j l v E sj v E sl Laser beam

40 ω ω θ d k S L n P r P e e s = ), ( sin = + = ) ) ( ) ( ) ( 4 i e i e T T Z Z k S k S k S α α α α ω θ πλ λ θ λ λ α 1 0 1/ 0 4 sin 4 / ) ( ) / sin( D e e D T n k = = ) 1/ 4 / ( e n kt e e D π λ =

41 α ( kλ D ) 1 << 1 α 1 λ θ kt e 1 = 4λ0 sin [ ln ] mec ω = 1 / θ kt i 4ω 0 sin m c i 1 ln

42 ,,,.

43

44

45 t=.56sec 10 Thomson Signal Intensity (A.U.) n e (x10 19 m - 3 ) ρ t=1.06sec Thomson Signal Intensity (A.U.) n e (x10 19 m - 3 ) ρ

46

47

48 ,,, :

49

50

51 N X( 1 X) = X Y sin θ ± [( Y sin θ) + ( 1 X) Y cos θ] / 1 1/ = p ce ω p = ( nee / ε 0me ) X ω / ω, Y = ω / ω ωce = eb / m e N = 1 x = 1 ω p / ω O N X (1 X ) ω p = 1 = 1 ( ω ω ) /( ) p ω ω p ω E ce 1 X Y ω

52 O 1/ )] / ( 1 [ c n e n N = = 1 ) ( )] /(4 [ 0 Z Z e e dz Z n m c e ε π λ φ = = 1 ) ( 8 ) /( 0 Z Z e e dz Z n m c e F ε π λ π φ

53 x = acos( ωt φ) x b cosω t R = ( x+ x ) = a cos ( ωt φ) + b cos ωt+ ab[cos( ωt φ) + cos φ] R ab cosφ

54 ω = ( ω / c)(πρm sin β ) S R = a b cosϕ S = abcos( φ + ϕ) ϕ = ωt

55 N X = 1 1 Y ± XY 1 Y X = 1 1± Y = 1 ( ω / ω )[ ω /( ω ± ω p ce )]

56 Faraday Ψ Linearly Polarized EM wave E k E n e B z Ψ= λ n e B z dz n R n L Φ= λ n e dz n R + n L

57 Faraday R-wave ω 1 E R = E R cos(ω 1 t k R z) Plasmas L-wave ω E L = E L cos(ω t k L z) mixer j ~(E R + E L ) ~ E R E L cos[(ω 1 ω )t (k R k L )z]+.. ω 1 ~ ω >> ω pe,ω ce >> ω 1 ω k L k R = ω c (N L N R ) = ω peω ce cω ~ n e B z

58

59 nedl Time (ms) ne1 ne ne3 ne4 ne5 ne6 70 Faraday Rotation (deg.) Time (ms) s cm nedl Time (ms) ne7 ne8 ne9 ne10 ne11 70 Faraday Rotation (deg.) Time (ms) 60-4 cm

60

61 ------

62 HCN HCN J= J=10 = m J= J=0 = m -HV 10kV/A P LaB6 F-P KF KF 5 Gas inlet 16 8/ HCN dengzc CH4+N+He KF 6 He KF 16 ( (,,, )

63

64

65 1.0 M5 M4 M5X1 M4 M4 M5 M475 M5 M6 M5 M3 M5 M5 M6 M3 M5M3 M4 M5M6 M4 6 M5X16 M4 M5X16 M5X16 M5 M3 M6 M5 M3 75 M4 M6 M4 M5X16 M5 M5X1M 3 M3 M6 75 M3M3 6 M3M3 M6 M5 M4 M4 M4 M4M4 M4M4 M4 M4 M4 M8 M8 M6 M6 M6 M6 SPE CTRUM A NALYZ ER Asy-15 Asy-15 Asy-15 M5 M5 M5 M5 M5 M5 M4 M4 M4 M6 M4 M4 Asy-139 M6 M4 M6 M 4 M4 M6 M Beam3 Beam Beam1 Detection optics area CO /YAG two color laser interferometer on LHD Port3 Port Port1 Local beam PM PM f=1300 f=100 SM f=400 PM; Off axis parabolic mirror SM; Spherical mirror SL; Spherical lens BS; Beam splitter BC; Beam combiner f; Focal length in mm Probe beam BS PM f=15 YAG APD Detector Plane SL f=550 BC Vertical s lab beams Probe beam CO MCT Detector Plane Detection Layout Local beam CO 0 ) YAG laser M3 CO laser Spectrometer Local FIR I nterferometer housing YAG AOM SM f=50 YAG BS SM f=750 SL f=-1000 SL f=-150 BS Tranmission Layout BC BC BS CO AOM HeNe

66 Laser,detector and every optics are place on vibration protected stand. 8W CO (10.6µm) and 0.5W YAG (1.06µm) are used. Two 3 ch LN coled HgCdTe detector array for CO and APD for YAG are used. n e (x10 19 m -3 ) t(sec) Shot# R(m)

67

68 λ/ Plate 3-Wave Polarimeter Reference Mixer Lens ω Probe Beams ω 1 ω Polarizer Signal Mixer ω 1 ω 3 FIR LASER λ/4 Plate L.O. Beam Beam Splitter Plasma Lens Ψ=c F n e B z dz Φ=c n n e dz

69 Refraction problem due to plasma density gradient sets the long wavelength limit α m = sin 1 n ( n o c ) n n o c = n oλ

70 Cotton-Mouton

71

72

73

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