The secondary electron blur was reported to be not observed in this range.

The range of secondary electrons depends on the energy.

Secondary electrons are generated by the decay of the core hole.

One type had a funnel of sorts to capture the secondary electrons.

The reaction centers in this complex are secondary electron acceptors.

In both techniques, it is not the primary beam, but secondary electrons which cause the deposition.

This can for example be a light source creating secondary electrons via the photoelectric effect.

Using the signal of secondary electrons image resolution less than 0.5 nm is possible.

This is necessary since the energy distribution of secondary electrons peaks well below 10 eV.

This affects the number of secondary electrons that escape the device surface and reach the detector.

These electrons create secondary electrons when they strike the face of the detector.

These secondary electrons also are accelerated, creating larger numbers of free electrons.

In this case the localized image rapidly fades as energy is removed by the secondary electrons.

Some crashing positive ions may generate a secondary electron.

The secondary electrons will ionize far more atoms than the primary photon.

These secondary electrons are detected by a sensor, and the image of the specimen is generated over a certain time period.

Flare effects may be difficult to separate from the secondary electron effects discussed earlier.

Multiple secondary electrons are emitted, which accelerate towards the second dynode.

For example, a dye chromophore has been modified by the addition of secondary electron donors.

This is possible because the ions hitting the cathode release secondary electrons at the impact.

The coefficient gives the number of secondary electrons produced by primary electron per unit path length.

As the primary photon beam passes through the plate, secondary electrons are generated.

The impact of an electron to a surface can, depending on its energy and angle, release one or more secondary electrons into the vacuum.

This adds another significant source of photoelectrons and secondary electrons which effectively reduce the image contrast.

Secondary electron collision cross sections for use in radiotherapy and radioprotection.