Electrons which diffuse from the cathode into the P-doped layer, or anode, become what is termed " minority carriers " and tend to recombine there with the majority carriers, which are holes, on a timescale characteristic of the material which is the p-type minority carrier lifetime.

Electrons excited to the conduction band also leave behind electron holes, i. e. unoccupied states in the valence band.

Electrons and holes are the charge carriers in semiconductors.

Electrons ( negative charges ) and holes ( positive charges ) both contribute to the induced thermoelectric voltage thus canceling each other's contribution to that voltage and making it small.

Electrons and holes diffuse into regions with lower concentrations of electrons and holes, much as ink diffuses into water until it is uniformly distributed.

Electrons have higher diffusion constant than holes leading to fewer excess electrons at the center as compared to holes.

Electrons and holes are injected into the organic layer at the electrodes and form excitons, a bound state of the electron and hole.

Electrons and holes are both fermions with half integer spin.

Mnemonics: LEO Red Cat ( Loss of Electrons is Oxidation, Reduction occurs at the Cathode ), or AnOx Red Cat ( Anode Oxidation, Reduction Cathode ), or OIL RIG ( Oxidation is Loss, Reduction is Gain of electrons ), or Roman Catholic and Orthodox ( Reduction-Cathode, anode-Oxidation ), or LEO the lion says GER ( Losing electrons is Oxidation, Gaining electrons is Reduction )

Electrons are at the heart of cathode ray tubes, which have been used extensively as display devices in laboratory instruments, computer monitors and television sets.

Electrons that belong to different molecules start " fleeing " and avoiding each other at the short intermolecular distances, which is frequently described as formation of " instantaneous dipoles " that attract each other.

Electrons, being fermions, cannot occupy the same quantum state, so electrons have to " stack " within an atom, i. e. have different spins while at the same place.

Electrons at these states can be easily excited to the conduction band, becoming free electrons, at room temperature.

Electrons and ions in the magnetosphere, for example, will bounce back and forth between the stronger fields at the poles.

Electrons will be accelerated in the opposite direction to the electric field by the average electric field at their location.

Electrons exiting the source cavity are velocity modulated by the electric field as they travel through the drift tube and emerge at the destination chamber in bunches, delivering power to the oscillation in the cavity.

* Electrons are fermions, but when they pair up into Cooper pairs they act as bosons, and so can collectively form a coherent state at low temperatures.

Electrons follow the path indicated by the arrow and approach the sample at angle θ.

Electrons can only reach ( and " illuminate ") a given plate element if both the grid and the plate are at a positive potential with respect to the cathode.

Electrons flow through that digit's grid and strike those plates that are at a positive potential.

" Inelastic Scattering Of Electrons By Protons ", Department of Physics at Harvard University, United States Department of Energy ( through predecessor agency the United States Atomic Energy Commission ), ( December 1966 ).

Electrons inside the blob travel at speeds just a tiny fraction below the speed of light and are whipped around by the magnetic field.

In 1936, the two published a paper, " The Passage of Fast Electrons and the Theory of Cosmic Showers " in the Proceedings of the Royal Society, Series A, in which they used their theory to describe how primary cosmic rays from outer space interact with the upper atmosphere to produce particles observed at the ground level.

*“ Electrons move at the same speed whether at Intel or AMD .”

Electrons emitted at any point are accelerated a modest distance down the funnel before impacting the surface, perhaps on the opposite side of the funnel.

Electrons also have a long ballistic length at this temperature ; their mean free path can be several micrometres.

Electrons move according to the cross product of the magnetic field and the electron propagation vector, such that, in an infinite uniform field moving electrons take a circular motion at a constant radius dependent upon electron velocity and field strength according to the following equation, which can be derived from circular motion:

Electrons are reflected from the outside surface of the sheath while all positive ions which reach the sheath are attracted to the electrode.

Electrons do not penetrate as deeply into matter as X-rays, hence electron diffraction reveals structure near the surface ; neutrons do penetrate easily and have an advantage that they possess an intrinsic magnetic moment that causes them to interact differently with atoms having different alignments of their magnetic moments.

Electrons flow through the conductive structure of the tether to the power system interface, where it supplies power to an associated load, not shown.

Perhaps the most famous conference was the October 1927 Fifth Solvay International Conference on Electrons and Photons, where the world's most notable physicists met to discuss the newly formulated quantum theory.

Electrons are the charge carriers in metals and they follow an erratic path, bouncing from atom to atom, but generally drifting in the opposite direction of the electric field.

Electrons are responsible for emission of most EMR because they have low mass, and therefore are easily accelerated by a variety of mechanisms.

Electrons are particulate radiation and, hence, have cross section many times larger than photons, so that they do not penetrate the product beyond a few inches, depending on product density.

Electrons and how they interact with electromagnetic fields are important in our understanding of chemistry and physics.

Electrons can absorb energy from photons when irradiated, but they usually follow an " all or nothing " principle.

Electrons and how they interact with electromagnetic fields are important in our understanding of chemistry and physics.

Electrons will move to the left side ( uncovering positive ions on the right side ) until they cancel the field inside the metal.

Electrons inside these long focus coils take helical paths as they travel along the length of the tube.

Electrons in non-bonding orbitals tend to be in deep orbitals ( nearly atomic orbitals ) associated almost entirely with one nucleus or the other, and thus they spend equal time between and not between nuclei.

Electrons which are trapped in an electromagnetic cavity are in a bound state and thus organise themselves as they do in a regular atom, thus expressing chemical-like behaviour.

Electrons, within an electron shell around an atom, tend to distribute themselves as far apart from each other, within the given shell, as they can ( due to each one being negatively charged ).

Electrons were ideal for the role, as they are abundant and easily accelerated to high energies due to their electric charge.