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We present simulations of: (1) the electric field distribution, as calculated with MAXWELL® 12.0, within the CZT detector with the delay-line electrode, (2) the charge carrier drift motion within the semiconductor, and (3) the propagation of the induced charge signal along the meandering electrode pattern.
It reaches its maximum at ~150 km (not shown here) and then gradually decreases to the reduction in collision between particles, leading to a purely drift motion.
Ion trajectory simulations have shown that close to the rung electrodes the RF fields actually act as barriers to drift motion (vide supra).
In DMA charged particles, especially aerosols or nanoparticles, travel in a gas flow perpendicular to the ion drift motion between two plates with a potential applied between the two plates.
This drift motion can perturb the spectral emission in the plasma shell.
The phenomenon of negative drift motion for only the sharp-corner BBDB for a certain wave-length range was also reproduced by the fully nonlinear BBDB simulations.
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Methods were identical to Expt. 2, except that all stimuli were presented without drifting motion.
Aberrant cilia are also unable to beat properly: embryos did not show usual drifting motion, which is characteristic of cooperative epidermal cilia beating (not shown).
In the future, the code will be applied to various drifting motions and it will be improved such that it can be used to simultaneously predict the behavior of several drifting objects.
The usefulness of monitoring the vertical F-region drift motions with Digisonde drift measurements is discussed.
The main targets are the drift motions and the additional damping caused by the operating rotor, so-called aerodynamic damping.
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