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Indirect processes, double photoionization

Its chief characteristic is that the excess energy of the photon above the double ionization threshold is shared as a continuous monotonic distribution between the two outgoing electrons. This direct double photoionization is contrasted with several indirect processes, of which by far the most important can be written... [Pg.104]

The prototypical indirect double photoionization process is the classical Auger effect, where the single-hole state created by ejection of an inner-shell electron exists for a significant time before ejection of a second electron. Alternatively, an intermediate singly charged state may exist as a multiply excited valence state or a Rydberg state, but whatever its nature, a lifetime of at least a few femtoseconds will normally allow the whole process to be considered as a sequence of two distinct steps. A sharp peak in the photoelectron spectrum and also, therefore, in... [Pg.109]


See other pages where Indirect processes, double photoionization is mentioned: [Pg.268]    [Pg.269]    [Pg.268]    [Pg.269]    [Pg.105]    [Pg.105]    [Pg.116]    [Pg.121]    [Pg.122]    [Pg.124]    [Pg.124]    [Pg.124]    [Pg.128]    [Pg.133]    [Pg.138]    [Pg.144]   


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