Results 271 to 280 of about 3,275,320 (297)
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Electric field dynamics at a charged point
Physical Review E, 1996The autocorrelation function for the electric field at an impurity ion in a plasma is considered. A simple model is constructed that preserves the exact short time dynamics and the long time global constraint of a given self-diffusion coefficient. The input required is the initial value of the autocorrelation function and its derivatives, and the self ...
Berkovsky, Ma +4 more
openaire +3 more sources
2014
This chapter introduces the essential concepts of carrier recombination and transport in silicon. The differential equations of interest are derived and solutions are given—particularly focusing on harmonically modulated excess carrier generation.
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This chapter introduces the essential concepts of carrier recombination and transport in silicon. The differential equations of interest are derived and solutions are given—particularly focusing on harmonically modulated excess carrier generation.
openaire +1 more source
Dynamics of charge transport in planar devices
Physical Review E, 2008The Poisson-Nernst-Planck equations describe the dynamics of charge transport in an electric field. Although they are relevant in many applications, a general solution is not known and several aspects are not well understood. In many situations nonlinear effects arise for which no analytical description is available. In this work, we investigate charge
Beunis, F. +5 more
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1987
The dynamics of colloidal solutions is classically studied in terms of the short-time diffusion coefficient D(q) which is extracted from the first cumulant of the auto-correlation function of the scattered amplitude I(q,t): $$D(q) = - \frac{1}{{{q^2}}}\frac{\partial }{{\partial t}}\log I(q,t = 0).$$ (1)
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The dynamics of colloidal solutions is classically studied in terms of the short-time diffusion coefficient D(q) which is extracted from the first cumulant of the auto-correlation function of the scattered amplitude I(q,t): $$D(q) = - \frac{1}{{{q^2}}}\frac{\partial }{{\partial t}}\log I(q,t = 0).$$ (1)
openaire +1 more source
Charge storage and charge transfer in dynamic memories
1984Among the many problems parallel processing is faced with — bigger nets, long range connections, communications with the outside world, organization, imperfections, etc. — the need for local memories enjoys a central role. To process information means first of all to get and keep the information where it is needed.
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Charge Localization and Dynamics in Rhodopsin
Physical Review Letters, 1996Buda F, deGroot HJM, Bifone A
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Dynamic Pricing for EV Charging Stations: A Deep Reinforcement Learning Approach
IEEE Transactions on Transportation Electrification, 2022Carman K. Lee, Zhonghao Zhao
exaly

