2014
DOI: 10.1088/0953-8984/27/2/025801
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Relaxation of highly excited carriers in wide-gap semiconductors

Abstract: The electron energy relaxation in semiconductors and insulators after high-level external excitation is analysed by a semi-classical approach based on a kinetic equation of the Boltzmann type. We show that the non-equilibrium distributions of electrons and holes have a customary Fermi-like shape with some effective temperature but also possess a high-energy non-Fermian 'tail'. The latter may extend deep into the conduction and valence bands while the Fermi-like component is localized within a small energy rang… Show more

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Cited by 4 publications
(4 citation statements)
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References 25 publications
(67 reference statements)
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“…The knowledge of the probabilities of electron scattering by short-wavelength phonons is necessary in the study of energy relaxation at high excitation levels by external high-energy radiation [18], as well as in connection with the search of thermoelectric materials with high efficiency [16], sf also recent review article Sjakste et al [47] and references therein.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The knowledge of the probabilities of electron scattering by short-wavelength phonons is necessary in the study of energy relaxation at high excitation levels by external high-energy radiation [18], as well as in connection with the search of thermoelectric materials with high efficiency [16], sf also recent review article Sjakste et al [47] and references therein.…”
Section: Discussionmentioning
confidence: 99%
“…Scattering of electrons by long-wave phonons in chalcopyrites earlier was studied in our paper [17]. In the presence of closely spaced energy minima in the conduction band the intervalley scattering (scattering by short-wavelength phonons) is also important, especially for the study of energy relaxation at high excitation levels [18].…”
Section: Introductionmentioning
confidence: 99%
“…However, one should expect that the recombination time is going to be several orders of magnitude smaller if there is no gap between the vacancy states and the conduction band, as is the cases for TiO 2 + vacancy and TiO 2 + N + vacancy. It was shown in [34] that, because of the emission of phonons, the excited electrons in the conduction band states of TiO 2 lose their excitation energy and sink onto the bottom of the band over the time that does not exceed several tens of fs; after this time the electrons recombine with the holes in the vacancy states. These data are also in agreement with the experimental results which reveal that the trapping of conduction band electron onto the states of dopants near the top of the band gap occurs over 100 -250 fs, while the hole trapping on the states near the bottom of the gap takes 50 -150 fs [33].…”
Section: Oxygen Vacancy Formation Energy and The Effect Of Doping Witmentioning
confidence: 99%
“…Therefore, one can expect that for these cases, only a small number of electrons are involved in the photocatalytic process. These are the excited electrons which form a high-energy "tail" of the electron distribution in the conduction band [34]; in analogy, a similar distribution of holes inside the valence band can exist [35]. In both cases, as in TiO 2 + vacancy as in TiO 2 + N + vacancy, the electron-hole pairs can be formed not only because of the excitations inside the conduction band but also because of the excitations into the conduction band from the valence band or from the band of nitrogen states.…”
Section: Oxygen Vacancy Formation Energy and The Effect Of Doping Witmentioning
confidence: 99%