aux pre-mì eres expériences de gravure sur différents matériaux carbonés. L'objectif principal de cesdernì eresétaiteresétait de vérifier si notre source d'hydrogène atomique, avec une puissance RF maximale de 1 kW, permettait d'atteindre des vitesses d'´ erosion non négligeablesnégligeablesà si basse pression, et s'est limitéè a l'observation de la surfacé erodée pour voir si nous obtenions des structures se rapprochant de celles que l'on retrouve sur les tuiles des tokamaks ,
ladernì ere section présente l'effet de la source d'hydrogène atomique sur des tuiles de composite carbone-carbone, ´ egalement appelé compositè a fibre de carbone (CFC) de type N 11 ,
CEA Cadarache), p.11 ,
obtenue dans le réacteur NAGDIS-II après exposition d'une cible de graphitè a un plasma de deutérium. (a)poussì ere initiale, (b) après dépôt d'une couche de tungstène pour la fixer, (c) structure interne de lapoussì eres après découpe par FIB ; (d), p.28 ,
C2 (rouge) = signal TD-LIF, C3 (bleu) = signal de la diode de contrôle, et C4 (vert) = courant injecté dans la diode laser, p.53 ,
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ion argon ; (b) pour l'argon neutre, p.59 ,
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centre de la chambre de diffusion en fonction de P RF pour différentes valeurs de B source : 75 G, 115 G et 150 G, p.86 ,
rel mesuré au centre de la chambre de diffusion en fonction de B source pour trois P RF fixées : 500, 700 et 900 W, p.91 ,
de diffusion) en fonction de la pression pour deux valeurs de B source : 0 et 75 G, p.94 ,
en fonction de B dif f pour trois puissances fixées : (a) 500 W, (b) 700 W, et (c) 900 W. B source = 0 G, p.117 ,
Ar m ] th calculés en fonction de B dif f pour trois puissances fixées : (a) 500 W, p.123 ,
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= 100 G, t exp = 4h, chauffage du porte-´ echantillonàechantillonà 650?C, p.148 ,
unéchantillonunéchantillon de GrFl 125 ayant subi le traitement suivantAr 100/0, p = 100 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 4h, p.149 ,
= 100 G, t exp = 4h, chauffage du porte-´ echantillonàechantillonà 650?C, p.150 ,
unéchantillonunéchantillon de GrFl 125 ayant subi le traitement suivantAr 0/100, p = 10 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 4h, p.152 ,
= 100 G, t exp = 4h, chauffage du porte-´ echantillonàechantillonà 650?C, p.153 ,
unéchantillonunéchantillon de GrFl 125 ayant subi le traitement suivantAr 0/100, p = 100 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 4h, p.154 ,
= 100 G, t exp = 4h, chauffage du porte-´ echantillonàechantillonà 650?C, p.155 ,
Ar 100/0, p = 10 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 6h, p.163 ,
Ar 100/0, p = 10 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 6h, chauffage du porte-´ echantillonàechantillonà 650?C, p.165 ,
Ar 0/100, p = 10 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 6h, p.166 ,
Ar 0/100, p = 10 mTorr, P RF = 900 W, B source = 0 G, B dif f = 100 G, t exp = 6h, chauffage du porte-´ echantillonàechantillonà 650?C, p.167 ,
apparition de plaques de dépôts issu de la coalescence de croissances isolées (a) sur le graphite GrFl 125 et (b) sur le composite N11 ; (c) ouverture de pores entre les faisceaux de fibres de carbone sur leséchantillonsleséchantillons de composite N11, p.173 ,
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