2005
DOI: 10.1103/physrevlett.94.067601
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Femtosecond Transfer Dynamics of Photogenerated Electrons at a Surface Resonance of Reconstructed InP(100)

Abstract: Time-dependent two-photon photoemission spectra are used to resolve the femtosecond dynamics of hot electrons at the energetically lowest surface resonance of reconstructed InP(100). Two different cases are studied, where electrons either are lifted into the surface resonance via a direct optical transition or are captured from bulk states. These data are the first of this kind recorded with a time resolution below 70 fs. The microscopic analysis shows that electron-phonon scattering is a major mechanism for e… Show more

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Cited by 31 publications
(27 citation statements)
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“…60 Both the time dependence and the continuous energy distribution in the spectra shown in Fig. 4 do not show any sign of a single dominant surface resonance for the catechol:rutile ͑110͒ interface prepared as described above.…”
Section: Resultsmentioning
confidence: 73%
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“…60 Both the time dependence and the continuous energy distribution in the spectra shown in Fig. 4 do not show any sign of a single dominant surface resonance for the catechol:rutile ͑110͒ interface prepared as described above.…”
Section: Resultsmentioning
confidence: 73%
“…Figure 4 shows an additional rather surprising result, i.e., the energy distribution is hardly changing with increasing delay time, a behavior that is strikingly different from, for example, the hot electron relaxation in the case of InP͑100͒ that has been measured also with 2PPE. 60,62 The surprising conclusion here is that the energy relaxation of the electrons injected into the unoccupied states at the catechol:rutile ͑110͒ interface is negligible on the time scale of the measured decay, i.e., 200 fs. The same observation has been made for electron injection into rutile ͑110͒ from the excited state of various perylene dyes.…”
Section: Resultsmentioning
confidence: 80%
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“…Although the second quantization formalism is not necessary for the examination of the optical interaction, thus leading to the same equations as a single particle approach, 26 it is of central importance in the treatment of the phonon-electron interaction, which is necessary to understand recent experiments. 27 Before being specified to a certain material system, the derived equations represent a general description of the electron dynamics at semiconductor surfaces. For the numerical evaluation, typically the restriction to a few-band system is necessary.…”
Section: Introductionmentioning
confidence: 99%