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Fermi nanostructured materials

In order to take advantage of nanometer-sized semiconductor clusters, one must provide an electron pathway for conduction between the particles. This has been achieved by sintering colloidal solutions deposited on conductive glasses. The resulting material is a porous nanostructured film, like that shown in Fig. 1, which retains many of the characteristics of colloidal solutions, but is in a more manageable form and may be produced in a transparent state. Furthermore, the Fermi level within each semiconductor particle can be controlled potentiostati-cally, a feature which is fundamental for the functioning of the electrochromic devices described in Section III. [Pg.4]

Polarization of the non-bonding electrons is responsible for the size emergence of defect and nanostructures with properties that the bulk material does not demonstrate. This kind properties include dilute magnetism, catalysis, Dirac-Fermi polaron, magnetoresistance, etc. [Pg.429]


See other pages where Fermi nanostructured materials is mentioned: [Pg.664]    [Pg.443]    [Pg.515]    [Pg.180]    [Pg.145]    [Pg.96]    [Pg.386]    [Pg.271]    [Pg.137]    [Pg.413]    [Pg.286]    [Pg.361]    [Pg.4983]    [Pg.327]    [Pg.169]    [Pg.158]    [Pg.159]    [Pg.6]   
See also in sourсe #XX -- [ Pg.1035 , Pg.1049 , Pg.1055 ]

See also in sourсe #XX -- [ Pg.1035 , Pg.1049 , Pg.1055 ]




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