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.. De-si, Perte d'énergie cinétique due aux interactions nucléaires et électroniques en fonction de l'énergie de la particule incidente pour un atome Cs dans une cible, p.16

.. Les-distributions-angulaires-dy, Si par des ions Cs + en fonction de l'angle d'incidence avec une énergie d'impact fixée à 2 keV en atomes/ion·sr. La flèche noire représente le faisceau incident. Nous pouvons observer que les distributions en élévation a) b) et c) sont de type sur-cosinus. Les distributions en fonction de l'azimut sont quasi circulaires, p.76

.. Exemple-de-diagramme-polaire, la fonction f (?) = cos 2.5 (? ? 23) avec ? l'angle d'émission. La flèche représente le faisceau incident, p.79

6. De, Ceci signifie qu'une fois le régime d'équilibre atteint, la région modifiée, donc le profil de la concentration, se déplace continûment avec l'érosion du cratère. Le profil mis en exemple est calculé pour un échantillon de GaAs pour une dose de 10 17 ions/cm 2 de Cs + avec une énergie d'impact de 2 keV et un angle, IV.19 La profondeur de départ du graphique correspond à la surface du fond du cratère, p.97

C. La, de la méthode de pulvérisation-collection sur un collecteur plan. x 0 est le point sur le collecteur à la verticale du centre du cratère. b) Photo du dispositif expérimental permettant la collection à plat de la matière émise sous le bombardement de Cs + au sein de, p.117

S. Epaisseur-de and .. Déposé-en-fonction-du-collecteur, L'épaisseur du dépôt sur le Ge est normalisée pour que les valeurs à l'émission normale à l'échantillon correspondent.L'échantillon est pulvérisé par un bombardement d'ions Cs + de 2 keV et un angle d'incidence de 60?par60?par rapport à la normale. Nous observons que le maximum d'épaisseur sur le collecteur plan est à environ 15ålors que le maximum sur le collecteur cylindrique est à environ 35?, p.119

F. Le, Image par électrons secondaires d'une grille de cuivre disposée sur le porte-échantillon Storing Matter et irradiée par, p.128

S. , A. /. Xps, and .. , Un sas de transfert adapté a été installé sur plusieurs instruments . ) du CRP-Gabriel Lippmann mais également dans d'autres laboratoires européens, Valise de transfert sous ultravide, p.130

.. Conditions-de-bombardement-des-cibles, 61 III.4 Conditions d'analyse des profils en profondeur dans l'instrument, p.63