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Submitted on 1 Jan 1979
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A CO2 LASER -PLASMA INTERACTION
EXPERIMENT- THE SCATTERED SPECTRUM OF LANGMUIR WAVES DRIVEN VIA THE
ELECTRON-ION DECAY INSTABILITY
M. Forrest, R. Kirk, N. Peacock
To cite this version:
M. Forrest, R. Kirk, N. Peacock. A CO2 LASER -PLASMA INTERACTION EXPERIMENT- THE SCATTERED SPECTRUM OF LANGMUIR WAVES DRIVEN VIA THE ELECTRON- ION DECAY INSTABILITY. Journal de Physique Colloques, 1979, 40 (C7), pp.C7-745-C7-746.
�10.1051/jphyscol:19797360�. �jpa-00219356�
JOURNAL DE PHYSIQUE CoZZoque C7, suppZdment au n07, Tome 40, JuiZilet 1979, page C7-
,745
A C02 LASER -PLASMA INTERACTI(UU EXPERIMENT- THE SCATTERED SPECTRUM OF LANGMUIR WAVES DRIVEN VIA THE ELECTRON-ION DECAY INSTABIUW
M.J. Forrest, R.E.
irk'
and N.J. peacock.CuZham
m o r a t o r y , Abingdon, Oxon, OX14 3DB, UK fEuratom/UKAEA Fusion AssoOiation).
S t u d i e s o f t h e i n t e r a c t i o n o f a p u l s e d C02 l a s e r w i t h a p r e f o r m e d h i g h d e n s i t y p l a s m a a r e r e p o r t e d . T h e p l a s m a i s p r o d u c e d i n a P l a s m a F o c u s d e v i c e w h i c h h a s b e e n e x t e n s i v e l y d i a g n o s e d . B e c a u s e o f
- 3 t h e h i g h k i n e t i c e n e r g y o f t h e p l a s m a ( 5 k j cm I c o m p a r e d t o t h e l a s e r pump e n e r g y ( 1 5 j o u l e s l , n o n - l i n e a r p l a s m a p r o c e s s e s c a n b e e x c i t e d w i t h o u t a l t e r i n g t h e b a s i c p l a s m a p a r a m e t e r s .
P r e v i o u s e x p e r i m e n t s " ) h a v e i n d i c a t e d t h a t d u r i n g t h e c o m p r e s s i o n p h a s e o f t h e p l a s m a when ne>ncrit
- 3
C02 = 9 . 9 4 , 1 0 e l e c t r o n s , cm t h e f o c u s e d l a s e r beam i s t o t a l l y a b s o r b e d . T h e f o c u s e d s p o t s i z e i s 5 0 0 m i c r o n s a n d t h e p u l s e w i d t h 4 0 n a n o s e c o n d s FWHM.
V a r i o u s p r o c e s s e s h a v e b e e n p r o p o s e d t o a c c o u n t f o r t h i g b e h a v i o u r . E a r l i e r e x p e r i m e n t s ( 2 1 h a v e i n d i c - a t e d t h a t t h e e l e c t r o n - i o n d e c a y i n s t a b i l i t y , w +
C02 w + w
+
6w c a n c o n t r i b u t e t o t h e a b s o r p t i o nL i a
p r o c e s s . W h e r e wL a n d w. a r e t h e L a n g m u i r a n d i o n - l a
a c o u s t i c w a v e f r e q u e n c i e s r e s p e c t i v e l y a n d 6w i s t h e p e r m i s s i b l e f r e q u e n c y m i s m a t c h g i v e n by
P b e i n g t h e r a t i o o f t h e pump i n t e n s i t y t o t h e t h r e s h o l d i n t e n s i t y o f t h e i n s t a b i l i t y , a n d v e i s t h e e l e c t r o n t h e r m a l y e l o c i t y . U s i n g t h e a n a l y s i s o f P e r k i n s a n d F l i c k ( 1 9 7 1 1 ( 3 1 f o r a n i n h o m o g e n e o u s p l a s m a w h e r e Te >> T . , t h e t h r e s h o l d pump i n t e n s i t y , when t h e s w e l l i n g o f t h e pump w a v e i s t a k e n i n t o
- 2 a c c o u n t , i s o f t h e o r d e r o f 3.10' w a t t s cm
.
H e r ei t i s p o s s i b l e f o r L a n g m u i r w a v e s t o b e d r i v e n w e l l a b o v e t h e i r t h e r m a l l e v e l , w h i l e t h e i o n a c o u s t i c w a v e s a r e h e a v i l y L a n d a u d a m ~ e d .
P O - s w i t c h e d r u b y p r o b e l a s e r ( 5 0 0 NWI h a s b e e n u s e d t o p r o d u c e a c o - o p e r a t i v e l y s c a t t e r e d s p e c t r u m . T h e p r o b e beam i s c o - a x i a l t o t h e CO 'pump beam a n d
2
b o t h h a v e h o r i z o n t a l l y p o l a r i s e d o u t p u t s . T h e s c a t t e r i n g c o l l e c t i o n o p t i c s a r e a r r a n g e d t o g i v e a f o r w a r d sc:ttering a n g l e o f 8 f 2.4', F i g . 1. T h i s r e s u l t s i n t h e s c a t t e r i n g p a r a m e t e r
a = k ( D e b y e l . / k ( L a n g m u i r 1 > 6
If a < 4 t h e n s i g n i f i c a n t L a n d a u d a m p i n g o f t h e
L a n g m u i r w a v e s o c c u r s .
nR5K fl SELECT
GrERMWH LENS
Fig.1 Schematic showing coaxiai! C02 pump beam and ruby probe beam and coZZection optics. The perspect- 2vs veetdr diagram-iSLiustrates in00 t h e scattering vectoiq k i s arranged t o be paraZZe2 t o the excited k Langmuir ' s
.
T h e s c a t t e r i n g o f t h e s e e n h a n c e d L a n g m u i r w a v e s r e s u l t s i n d i s c r e t e s h i f t e d e l e c t r o n f e a t u r e s , e a c h s i d e o f t h e r u b y l a s e r w a v e l e n g t h 6 9 4 3
8.
T h i s s c a t - t e r e d s p e c t r u m i s g i v e n byT h e r e f o r e t h e p e a k i s d i s p l a c e d by (w - wia1 = c o 2
w
gram
wruby, w i t h a w i d t h o f 2 6w. T h e r e i s , i n cO?addition, a s p r e a d i n f r e q u e n c y d u e t o t h e f i n i t e r a n g e o f w a v e v e c t o r s a c c e p t e d by t h e s c a t t e r i n g o p t i c s .
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19797360
A g a t e d i n t e n s i f i e d o p t i c a l m u l t i c h a n n e l a n a l y s e r REFERENCES
( O N A ) , i n c o n j u n c t i o n w i t h a o n e m e t r e f o c a l l e n g t h 1. FORREST M J e t a l , P h y s . R e v . L e t t s . 3 7 ( 1 9 7 9 ) 1681-1684
g r a t i n g s p e c t r o m e t e r , h a s been used t o r e s o l v e t h e
2. PEACOCK N J e t a l , J o u r n a l d e P h y s i q u e (19771 d o w n - s h i f t e d w a v e l e n g t h e l e c t r o n f e a t u r e . The e x - Tome 38 C6 43-54
p e r i m e n t a l l y d e r i v e d p r o f i l e was compared w i t h t h e o - 3 m a n d FLICK J , Phys. of Fluids, r e t i c a l p r e d i c t i o n s o f a m p l i t u d e and s h a p e . 14(1971 I 2012-2018
* A t t a c h e d from Royal Holloway C o l l e g e , U n i v e r s i t y o f London, E n g l e f i e l d Green, S u r r e y , U K .