/. La-structure-de-bande-de-l-'´-etat-de-shockley-de-la-surface-nue-d-'ag and . Cu, Nous proposons ici d'en rappeler les principaux résultats ComméCommé enoncé précédemment, le Cu(111) possède unétatunétat de Shockley caractérisé par une dispersion parabolique dont le bas de bande est mesurémesuréà -440 meV sous le niveau de Fermi (` a 80K), avec une largeur spectralè a ? d'environ 40 meV et une masse effective de m * = 0.41 m e . Après le dépôt d'Ag, pour des taux de couverture inférieursinférieursà la monocouche, on observe l'atténuation de l'intensité de l

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. Cartes-de-conductance-un, en fonction de la position(x,y) en maintenant la boucle de contre réaction active pour garder la composante continue de I constante Cette technique a pourénormepourénorme avantage d'? etre beaucoup plus rapide, en permettant d'obtenir sur notre dispositif expérimentale une cartographie bidimensionnelle de la conductance en une vingtaine de minute (pour une seulé energie) Elle permet de repérer facilement et rapidement les effets spectroscopiques liés liésà la localisationélectroniquelocalisationélectronique, par exemple dans le cas du confinement desétatsdesétats de Shockley 162 2 STM/STS dans des puits quantiques. Néanmoins, les données sontàsontà interpréter avec précaution car nous n'enregistrons plus dans ce cas la densité d'´ etatàetatà hauteur constante. L'expression donnée en A.17 n'est plus valable, Cet effet a ´ eté notamment discuté dans les travaux de Kliewer et coll. présentés en figure C.8 ou l'on observe sur des résonateurs formés par des atomes de Mn déposés sur Ag(111) un excellent accord entre les cartes de conductances mesurées et calculées, et un fort désaccord avec la densité d'´ etat théorique

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