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(a) Mobile electron density under 50-kV dc voltage.
(b) Mobile electron density under 1-kV dc voltage.
(a) Mobile electron density and (b) trapped electron density.
(a) Trapped electron density and (b) mobile electron density.
In fact, the trapped electron density is almost equal to 4 C m−3 and the mobile electron density is nearly equal to 2 C m−3.
Variation of mobile electron density: ∂ ρ eμ x, t ∂ t = − s 1 ρ eμ x, t ρ ht x, t ⏟ Disappearance by recombination with trapped holes − B e ρ eμ x, t 1 − ρ et x, t ρ Te x, t ⏟ Disappearance by trapping Open image in new window (17).
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Open image in new window Figure 11 Trapped electron and mobile electron densities.
Indeed, under this low voltage, the mobile electron and hole densities are not important and cannot reach the opposite electrodes, so the recombination rate density is more significant in the middle of the sample.
A possible explanation for this observation is that the absent guiding bar in mouse TR3, PfTR, and DmTR renders the C-terminal tails of these enzymes too mobile to generate sufficient electron density to observe the C-terminus of these enzymes.
Open image in new window Figure 3 Mobile electron and mobile hole densities.
Open image in new window Figure 3 Mobile and trapped electron densities in a thickness of 150 × 10 −6 m under 10 kV.
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