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CONFINAMIENTO NANOSC´OPICO EN ESTRUCTURAS ... - It works!

CONFINAMIENTO NANOSC´OPICO EN ESTRUCTURAS ... - It works!

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Confinamiento dieléctrico 225Delocalized image surface states in defects free SiO 2 hollow nanospheresJ.L. Movilla, F. Rajadell and J. Planelles ∗Departament de Química Física i Analítica, UJI, Box 224, E-12080 Castelló, Spain∗ E-mail: josep.planelles@qfa.uji.esDelocalized image surface states in free-standing hollow silica nanospheres populated with one or twoelectrons or an exciton are theoretically predicted for a wide range of internal radii and shell thicknesses.The driving force building up these surface states is the image self-polarization potential originated fromthe dielectric mismatch between the nanoshell and the surrounding air. The surface states are localizedin a spherical crown beyond the nanoshell border, i.e. carriers are mostly in air. The transition fromvolume to surface state will then have to overcome the spatial confining potential barrier of the nanoshell.Owing to the different spatial confining barriers of electrons and holes in the silica nanoshell, electron butno hole density can be concentrated in surface distributions. The self-polarization potential looks like adouble-well potential, each well located just beyond the nanoshell border, with the internal well deeperthan the external one, so that an excess carrier is attracted more strongly by the inner interface. Thisleads the electron density of a surface state to be located mainly in the internal surface of the hollownanosphere. The shorter the inner nanoshell radius is, the stronger the binding of the excess electron tothe surface will be. The volume/surface ground state phase diagrams of the one-electron, two-electronand exciton systems have been calculated. All three diagrams are quite similar, thus revealing the monoelectroniccharacter of the driving force for the transition from volume to surface states.Keywords: Semiconductor nanocrystals, image surface states, self-energy, silica.pacs:73.20.-r; 73.20.At; 73.22.-f.1 IntroductionColloidal growth of free-standing nanocrystals makes it possible to fabricate the smallest semiconductornanocrystallites with sizes of just a few nm and a spherical shape.[1, 2, 3, 4, 5] Wet chemistry methodsalso allow multishell structures built of concentric layers to be synthesized with highly controlled shellthicknesses and compositions.[1, 2, 3, 6, 7, 8, 9, 10] Treating these core-shell composites further (by calcining,chemistry or photo-etching methods) one can finally obtain hollow spheres.[11, 12, 13] Hollowspherical materials have aroused a great deal of interest owing to their numerous potential applications in

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