Stages of hot electron dynamics in multiexcitation processes at surfaces: General properties and benchmark examples
Tài liệu tham khảo
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Contrary to the popular belief these tails are generally not Lorentzian-like. The spectral wing shapes far away from the QE peak are determined by the short time behaviour of exp[C(k,t)] which due to (22) does not give rise to Lorentzian tails in the quasiparticle spectrum N(k,ω′).
A similar procedure of remeding the threshold properties of multiple boson excitation probabilities was introduced in Section IV of Ref. [56].
The mapping N(ω′)→ρ(ω) in which N(ω′) exhibits a sharp upper band edge cutoff may give rise to negative values of the cumulant spectrum ρ(ω) in certain intervals of ω, likewise in Section 3.2.2.
The root giving the position of GWA plasmaron maximum exceeds Ek by more than the surface plasmon excitation energy [28].
An analogous identification of the corresponding quantities was carried out in Ref. [30].
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The inclusion of the effects of nondispersive surface plasmons amounts to taking a convolution of the spectrum from Eq. (49) with the spectrum from Eq. (26).
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For example of another type interactions and time scales of transients see Refs. [20,21].
For the time scales of formation of image potential and corresponding bands see Figs. 5 and 6 in Ref. [71].
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