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Electron–Phonon Interaction and Electron Transport
2001Semiconductor device operation depends on the speed of carriers, electrons and holes, which is determined by the mobility. The mobility μ is expressed by e〈Τ〉/m*, where e, 〈Τ〉, and m* are the electronic charge, average of the relaxation time, and the effective mass.
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Polarizationeffects in electron-electron and positron-electron scattering
Zeitschrift f�r Physik, 1966The polarization-asymmetries in the cross-sections for electron-electron and positron-electron scattering are investigated numerically in first order perturbation theory in the range from 1 keV to 10 GeV for all angles with regard to polarization-measurements.
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Electron-electron bremsstrahlung for bound target electrons
The European Physical Journal D, 2008For the process of electron-electron (e-e) bremsstrahlung the momentum and energy distributions of the recoiling electrons are calculated in the laboratory frame. In order to get the differential cross section and the photon spectrum for target electrons which are bound to an atom, these formulae are multiplied by the incoherent scattering function and
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In Situ and Emerging Transmission Electron Microscopy for Catalysis Research
Chemical Reviews, 2023Sheng Dai +2 more
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Electron microscopy: Remarks on 40 years of ultrastructural explorations
Ca-A Cancer Journal for Clinicians, 1977E de Harven
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