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Iron oxide hole mobility

Electrical conductivity is due to the motion of free charge carriers in the solid. These may be either electrons (in the empty conduction band) or holes (vacancies) in the normally full valence band. In a p type semiconductor, conductivity is mainly via holes, whereas in an n type semiconductor it involves electrons. Mobile electrons are the result of either intrinsic non-stoichiometry or the presence of a dopant in the structure. To promote electrons across the band gap into the conduction band, an energy greater than that of the band gap is needed. Where the band gap is small, thermal excitation is sufficient to achieve this. In the case of most iron oxides with semiconductor properties, electron excitation is achieved by irradiation with visible light of the appropriate wavelength (photoconductivity). [Pg.115]


See other pages where Iron oxide hole mobility is mentioned: [Pg.339]    [Pg.305]    [Pg.318]    [Pg.237]    [Pg.75]    [Pg.306]    [Pg.353]    [Pg.118]    [Pg.332]    [Pg.350]    [Pg.333]    [Pg.195]   
See also in sourсe #XX -- [ Pg.306 ]




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