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Ces deux raies sont caractéristiques de l'´ emission de PL d'une couche de mouillage. La différence d'´ energie entre les deux raies est de l'ordre de 58 meV, ce qui correspond au phonon optique Si-Si [19]. La photoluminescence des bo??tesbo??tes quantiques de Ge, dans lesquelles les porteurs (trous) sont confinés, apparaitàapparaità 0,86 eV. La largeur du pic attribué aux bo??tesbo??tes, de l'ordre de 100 meV, est principalement liéè a l'inhomogéneité en taille des bo??tesbo??tes de Ge. La photoluminescence d'unéchantillonunéchantillon contenant une bo??tebo??te de Ge par??lotpar?par??lot après une croissance du Gè a 600?C et une encapsulation dans le Sì a 650?C a ´ eté mesuréè a basse température (11 K) et le spectre de PL est représentée en figure 4.16. La photoluminescence des bo??tesbo??tes quantiques de Ge, située vers 800 meV (1,55 microns), est attribuéè a une recombinaison non phonon, 988 eV, montre une contribution de la transition non phonon (NP) et sa réplique La position du pic de PL de nos bo??tesbo??tes est similairè a celle observée par Boucaud et al. pour une assemblée de dômes de Ge encapsuléè a 700?C dans le Si. La largeuràlargeurà mi hauteur du pic de luminescence de nos bo??tesbo??tes est de 42 meV. [1] R. J. Asaro et W. A. Tiller, Interface morphology development during stress corrosion cracking. 1. via surface diffusion, p.1789, 1972. ,
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Nos observations par MEB (voir figure 5.19(b) montrent clairement l'existence d'un facettage périodique, La période de ces facettes est plus importante sur les petites faces du nanofil que sur les grandes ,
20, nous montrons une image GISAXS lorsque le faisceau X est dirigé selon l'azimut <-1-12>. Cette image met enévidenceenévidence deux tiges de diffusion formant un angle de 10 ,
alliage SiGè a cette concentration en Ge est donné par la loi de Vegard : Le paramètre de maille d'un alliage Ge x Si 1?x peutêtrepeutêtre approché par la loi de Vegard et donné expérimentalement par [6] : a(Ge x Si 1?x ) = x.a Ge + (1 ? x) ,
6575 ? A) Pour une concentration de 2 %, la loi de Vegard donne un paramètre de maille de 5.4360 ? A Cette valeur est très proche du paramètre de maille moyen que nous venons d'attribuer au Si dans les fils (5.4352 ? A) On peut donc conclure que la faible relaxation observée du Si dans les fils est induite par la présence du Ge. Discutons maintenant du pic labellé 2 sur la figure 5.28. Uné etude par diffraction anomale au seuil du Ge nous a permis de déterminer l'origine de ce pic keV (le seuil d'absorption K du Gé etant situésituéà 11.103 keV) Le traitement de ces différents scans, en utilisant le code dévellopé par Vincent Favre Nicolin, extraire les facteurs de structures des atomes anomaux (atomes de Ge) et non anomaux Les contributions des atomes anomaux (courbe rouge) et non anomaux (courbe verte) sont représentées figure 5.30. Ces scans indiquent une forte contribution du Ge dans le pic ,
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