Standard IC processes, as well as those involving the use of ionizing
radiation, such as x-ray lithography etc., result in the generation of
bulk defects, and interface states in the gate insulator, or underlyi
ng substrate, respectively, of insulated gate field effect transistors
. Bulk defects are believed to be present as positively and negatively
charged electron and hole traps, respectively, as well as neutral hol
e and ''large'' and ''small'' neutral electron traps. This paper provi
des a perspective of the current state of knowledge about the spatial
distributions of large bulk defects, their areal densities, sizes, pos
sible interrelationships among them, and the special cases of defects
created by ion implanted silicon and oxygen, where knock-on effects ha
ve been simulated. It appears that bulk defects may all have their ori
gin in neutral hole traps, (so-called E' centers) and that when the in
sulator thickness is decreased to about 6-7 nm, defects are either no
longer present, or, more likely, are incapable of trapping charge at r
oom temperature because trapped carriers can either tunnel to one of t
he interfaces, or be annihilated by a reverse process. It appears poss
ible also that the precursor of the several types of defects only form
s at a ''grown'' silicon-silicon oxide interface. In theory, this woul
d make it possible to grow defect free insulators by a combination of
deposition and oxidation processes.