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We deemed this to be a reasonable simplification, as the impact ionization model was kept enabled and likewise the essential lattice heating routine.
Its surface roughness (SR) evolution is investigated using a dynamic dissolution algorithm based on critical ionization model.
Recently, Ala et al. (2008) [7] have proposed a soil ionization model, on the basis of the dynamic soil-resistivity model of Liew and Darveniza (1974) [16], for finite-difference time-domain (FDTD) computations, and tested the validity of the model against experiments on a single vertical grounding conductor.
Avalanche multiplication was described by the Selberherr impact ionization model.
The impact ionization model used here has been calibrated from 25 500°C°C.
The effect of carrier avalanche is accounted by the impact ionization model.
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In this paper we investigate the origin of the deviation and consider time dependent ionization models assuming material flow in solar flares or multiple loops occurring with a short time period.
There are many impact ionization models.
These ion-ization levels show that full ionization models are required to reconstruct the depletion pattern for low density gas.
SRH and the impact ionization models have been used successfully in explaining the experimental data of Si nanowire based SONOS memory cells with nanowire diameter of 5 nm [8], and thus their applicability to nanowire modeling is verified.
We extracted spectra from 3′-spaced annular regions across the Loop and fitted them either with a one-kTe-component non-equilibrium ionization (NEI) model or with two-kTe-component NEI model.
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