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Nous montrons que cette technique peut détecter des changements de dopage dans la gamme 10 15 à 10 20 atomes.cm -3 , avec une résolution nanométrique et un bon ratio signal/bruit. Puis, nous présentons des mesures de durée de décroissance sur des wafers silicium cristallin passivés. Les mesures sont réalisées sur la tranche non-passivée des échantillons. Nous montrons que, même si la tranche n'est pas passivée, les durées de décroissance obtenue par KPFM ont une bonne corrélation avec les temps de vie des wafers mesurées par décroissance de la photoconductivité détectée par micro-ondes. Par la suite, nous nous concentrons sur les analyses dispositif. A l'aide du KPFM, nous analysons deux types de cellules solaires silicium cristallin : les cellules solaires silicium épitaxié (epi-Si) et les cellules solaires hétérojonctions à contact arrière (IBC) En particulier, nous nous focalisons sur l'analyse de dispositifs en condition d'opération. Nous étudions d'abord l'influence de la tension électrique appliquée et nous montrons que les effets de résistance et de diode peuvent être détectés à l'échelle nanométrique, Les mesures de KPFM sont comparées aux mesures de microscopie électronique à balayage (SEM) dans les mêmes conditions, puisque le SEM est aussi sensible au potentiel de surface. Nous montrons que les mesures KPFM sur la tranche de cellules solaires epi-Si peuvent permettre d'étudier les changements de champ électrique avec la tension électrique appliquée ,
nous montrons que des mesures de temps de vie peuvent être effectuées à l'échelle locale sur la tranche de cellules solaires epi-Si, ce qui peut permettre de détecter les interfaces limitantes. Puis, nous étudions l'influence de l'illumination sur les mesures KPFM et CP-AFM. Nous effectuons des mesures sur la tranche de cellules epi-Si sous différentes valeurs d'intensité et longueurs d'onde d'illumination. Nous montrons une bonne sensibilité des mesures KPFM à l'illumination. Cependant, nous montrons que pour différentes longueurs d'onde, à tension de circuit ouvert fixé, nos mesures ne sont pas corrélées avec les mesures de rendement quantique interne, comme nous le pensions. Enfin, nous résumons notre travail dans un tableau qui représente les forces et faiblesses des techniques pour les différentes mesures d'intérêt exposées précédemment. A partir de ce tableau, nous imaginons un setup de microscopie « idéal ,