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In the next section we will investigate acceleration of an externally injected electron bunch in the wakefield of these explained cases.
In "Acceleration of an externally injected electron bunch", electron bunch acceleration with frequency chirped laser pulse in the magnetized plasma is considered, and a discussion of the results is given in "Conclusion".
The collector current density Jc and base stored charge Qb are then separately expressed as a function of the injected electron density n(0) in the base in order to find base transit time.
On the basis of obtained wave Hamiltonian, all the dynamic characteristics of the injected electron, considered as a quasiparticle, were found: speed, tensor of effective dynamic mass, and wave Lagrangian.
(The injected electron will also produce a spin excitation, which will travel at a different velocity than the charge excitations). Observing charge fractionalization physics in an experiment is a challenge in those (nonchiral) low-dimensional systems which are adiabatically coupled to Fermi liquid leads.
In principle, a QD active region can couple every injected electron and hole to the lasing mode so that the change in gain per change in injected electron is increased over a planar well [2].
The injected electron bunch is distributed numerically by a random Gaussian distribution in both coordinates and velocities.
The lorentz factor of the break in injected electron distribution.
The amount of charge captured is expected to increase considerably17 as the emittance of the injected electron bunch is reduced and its geometric overlap with the wakefield is improved.
The peak power of 112.5 mW was obtained at 10 K in pulsed mode, indicating ∼36 photons per injected electron for 120 periods of active region.
The transport of the injected electron in the ZnO to the TiO2 conduction band occurred by tunneling when the ZnO thickness is less than 2.2 nm.
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