• Aucun résultat trouvé

A CO2 LASER -PLASMA INTERACTION EXPERIMENT- THE SCATTERED SPECTRUM OF LANGMUIR WAVES DRIVEN VIA THE ELECTRON-ION DECAY INSTABILITY

N/A
N/A
Protected

Academic year: 2021

Partager "A CO2 LASER -PLASMA INTERACTION EXPERIMENT- THE SCATTERED SPECTRUM OF LANGMUIR WAVES DRIVEN VIA THE ELECTRON-ION DECAY INSTABILITY"

Copied!
3
0
0

Texte intégral

(1)

HAL Id: jpa-00219356

https://hal.archives-ouvertes.fr/jpa-00219356

Submitted on 1 Jan 1979

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

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�

(2)

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 n

L 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 e

i 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 by

T 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

(3)

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 .

Références

Documents relatifs

To test whether the vesicular pool of Atat1 promotes the acetyl- ation of -tubulin in MTs, we isolated subcellular fractions from newborn mouse cortices and then assessed

Néanmoins, la dualité des acides (Lewis et Bronsted) est un système dispendieux, dont le recyclage est une opération complexe et par conséquent difficilement applicable à

Cette mutation familiale du gène MME est une substitution d’une base guanine par une base adenine sur le chromosome 3q25.2, ce qui induit un remplacement d’un acide aminé cystéine

En ouvrant cette page avec Netscape composer, vous verrez que le cadre prévu pour accueillir le panoramique a une taille déterminée, choisie par les concepteurs des hyperpaysages

Chaque séance durera deux heures, mais dans la seconde, seule la première heure sera consacrée à l'expérimentation décrite ici ; durant la seconde, les élèves travailleront sur

A time-varying respiratory elastance model is developed with a negative elastic component (E demand ), to describe the driving pressure generated during a patient initiated

The aim of this study was to assess, in three experimental fields representative of the various topoclimatological zones of Luxembourg, the impact of timing of fungicide

Attention to a relation ontology [...] refocuses security discourses to better reflect and appreciate three forms of interconnection that are not sufficiently attended to