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Crossover from localized to itinerant electron

On the basis of the known electronic properties of actinides (which have been discussed elsewhere in this book), theoreticians had distinguished the 5f itinerant behaviour of light actinide metals from the 5 f localized behaviour of heavy actinide metals from Am on. The crossover, presented often as a Mott transition, had been predicted to occur between Pu and Am metal, due to the localized character of the 5f state in the latter. Photoemission spectroscopy demonstrates this phenomenon directly with the observation of a 5 f multiplet away from the Fermi level. The detailed description of this peak is certainly complicated, as often happens for response of localized states in photoemission on the other hand (Fig. 17) the contrast to the emission of Pu metal is convincing. [Pg.258]


See other pages where Crossover from localized to itinerant electron is mentioned: [Pg.250]    [Pg.285]    [Pg.293]    [Pg.304]    [Pg.311]    [Pg.332]    [Pg.343]    [Pg.260]    [Pg.278]    [Pg.250]    [Pg.285]    [Pg.293]    [Pg.304]    [Pg.311]    [Pg.332]    [Pg.343]    [Pg.250]    [Pg.285]    [Pg.293]    [Pg.304]    [Pg.311]    [Pg.332]    [Pg.343]    [Pg.260]    [Pg.278]    [Pg.250]    [Pg.285]    [Pg.293]    [Pg.304]    [Pg.311]    [Pg.332]    [Pg.343]    [Pg.290]    [Pg.299]    [Pg.330]    [Pg.604]    [Pg.278]    [Pg.37]    [Pg.248]    [Pg.290]    [Pg.299]    [Pg.330]    [Pg.282]    [Pg.282]    [Pg.75]    [Pg.71]    [Pg.144]    [Pg.58]   


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Crossover

Crossover from localized to itinerant electron behavior

Crossover from localized to itinerant electronic

Crossover from localized to itinerant electronic

Crossover from localized to itinerant electronic behavior

Crossover localization

Electron localization

Itinerant

Itinerant electrons

Localizing electrons

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