Secondary-electron-emission processes under electron bombardment play
an important role in the performance of a variety of electron devices.
While in some devices, the anode and the grid require materials that
suppress the secondary-electron-generation process, the crossed-field
amplifier (CFA) is an example where the cathode requires an efficient
secondary-electron-emission material. Secondary-electron-emission proc
esses will be discussed by a three-step process. penetration of the pr
imary electrons, transmission of the secondary electrons through the m
aterial, and final escape of the secondary electrons over the vacuum b
arrier. The transmission of the secondary electrons is one of the crit
ical factors in determining the magnitude of the secondary-electron yi
eld. The wide band-gap in an insulator prevents low-energy secondary e
lectrons from losing energy through electron-electron collisions, ther
eby resulting in a large escape depth for the secondary electrons and
a large secondary-electron yield. In general, insulating materials hav
e high secondary-electron yields, but a provision to supply some level
of electrical conductivity is necessary in order to replenish the ele
ctrons lost in the secondary-electron-emission process. Our secondary-
emission study of diamond demonstrates that the vacuum barrier height
can have a strong effect on the total yield. The combined effect of a
large escape depth of the secondary electrons and a low vacuum-barrier
height is responsible for the extraordinarily high secondary-electron
yields observed on hydrogen-terminated diamond samples.