Sentence examples for mobile and trapped from inspiring English sources

In pure Fe, dislocation loops were mobile and trapped in the strain field of a dislocation, leading to the formation of loop decoration of dislocations.

The source terms of recombination and trapping learn about the variation (disappearance or appearance) in densities of each type of mobile and trapped carriers.

Open image in new window Figure 3 Mobile and trapped electron densities in a thickness of 150 × 10 −6 m under 10 kV.

In order to study the effect of the sample thickness on the charge dynamic, we represent in Figures 7a,b and 8a,b the densities of mobile and trapped electrons under 60-kV dc applied voltage at 600 and 200 μm, respectively.

Finally, these mobile charge densities are used as initial data for the Runge-Kutta method, of the precision degree 5, applied to the continuity equation with source terms for the purpose of determining the densities of mobile and trapped electrons and holes.

The SSV can be associated with the ratio between mobile and trapped charge-carriers at the semiconductor dielectric interface as carriers first enter the channel when the OFET is switched from off- to on-state.[ 25] The presence of PαMS therefore reduces the density of interfacial traps responsible for the SSV in TIPS-pentacene.

where s1 is the recombination coefficient for mobile electron and trapped hole.

Indeed, we show that under low dc applied voltage, the total recombination rate density is dominated by the recombination between trapped electrons and trapped holes, while under high dc voltage, the recombination is governed by mobile electron-trapped hole and trapped electron-mobile hole recombinations.

In the following sections, we investigate the recombination phenomenon by examining the dominant type of recombination under low and high dc applied voltage: trapped electron-trapped hole (S0), mobile electron-trapped hole (S1), and trapped electron-mobile hole (S2).

The net charge density ρ x,t) is locally composed of the mobile and the trapped carriers.

To understand how the charges behave at low and high voltages, we plot the mobile and the trapped electron densities under 10 and 60 kV. Figure 3a,b shows the electron densities at 10 kV.