Simulated expansion of an ultra-cold, neutral plasma
... Coulomb coupling parameter is especially important because if it is roughly 1 or larger then the potential energy dominates and highly correlated motion between charged particles is expected. The experiments can tune the plasma so that ⌫ e Ⰷ1. It is precisely when the Coulomb coupling parameter was ...
... Coulomb coupling parameter is especially important because if it is roughly 1 or larger then the potential energy dominates and highly correlated motion between charged particles is expected. The experiments can tune the plasma so that ⌫ e Ⰷ1. It is precisely when the Coulomb coupling parameter was ...
The evolution of the magnetic structures in electron phase‐ space
... conditions is employed in our simulations. The background magnetic field B0 is along the x direction. In the simulations, ions are assumed infinitely massive and their dynamics are excluded. The electric and magnetic fields are obtained by integrating the time‐dependent Maxwell equations, and a rigo ...
... conditions is employed in our simulations. The background magnetic field B0 is along the x direction. In the simulations, ions are assumed infinitely massive and their dynamics are excluded. The electric and magnetic fields are obtained by integrating the time‐dependent Maxwell equations, and a rigo ...
PHOTONS IN SEMICONDUCTORS
... behind an empty state called a hole). The inverse process can also occur. An electron can decay from the conduction band into the valence band to fill an empty state (provided that one is accessible) by means of a process called electron-hole recombination. We therefore have two types of particles t ...
... behind an empty state called a hole). The inverse process can also occur. An electron can decay from the conduction band into the valence band to fill an empty state (provided that one is accessible) by means of a process called electron-hole recombination. We therefore have two types of particles t ...
Electrostatics PowerPoint
... Coulomb [N/C]. This describes the amount of force present for every coulomb of charge used as a test charge. The field strength equation (on the next slide) has no way of specifying the direction of the field, therefore you should ignore any negative signs that get created in your answer. ...
... Coulomb [N/C]. This describes the amount of force present for every coulomb of charge used as a test charge. The field strength equation (on the next slide) has no way of specifying the direction of the field, therefore you should ignore any negative signs that get created in your answer. ...
electric field
... Coulomb [N/C]. This describes the amount of force present for every coulomb of charge used as a test charge. The field strength equation (on the next slide) has no way of specifying the direction of the field, therefore you should ignore any negative signs that get created in your answer. ...
... Coulomb [N/C]. This describes the amount of force present for every coulomb of charge used as a test charge. The field strength equation (on the next slide) has no way of specifying the direction of the field, therefore you should ignore any negative signs that get created in your answer. ...
