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Photoionization cross section confinement resonances

The dependence of confinement resonances on quantum numbers of the ionized subshell nl can be illustrated by the 5-potential model calculated data [34] for the Ne Is and 2s photoionization cross sections from Ne C60, see Figure 5. [Pg.34]

Mb. Note, also, that, away from the threshold, the confinement resonances in er1 <5 and a s emerge at different energies and have different resonance amplitudes. Caution since the data displayed in Figure 5 were obtained in the 5-potential model, the predicted amplitudes of confinement resonances in these photoionization cross sections are, most likely, overestimated, as in the case of Xe C60-... [Pg.35]

In this case, the photoionization cross section possesses no Coulomb confinement resonances. This is because the fullerene cation s potential Vcti(r) seen by an outgoing photoelectron does not exhibit a Coulomb potential barrier (see Figure 10 for z = +5 for illustration purposes). [Pg.41]


See other pages where Photoionization cross section confinement resonances is mentioned: [Pg.13]    [Pg.26]    [Pg.32]    [Pg.32]    [Pg.32]    [Pg.32]    [Pg.33]    [Pg.34]    [Pg.37]    [Pg.41]    [Pg.41]    [Pg.43]    [Pg.43]    [Pg.44]    [Pg.44]    [Pg.48]    [Pg.49]    [Pg.49]    [Pg.49]    [Pg.51]    [Pg.52]    [Pg.52]    [Pg.53]    [Pg.54]    [Pg.59]   
See also in sourсe #XX -- [ Pg.32 , Pg.33 , Pg.34 ]




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