Abstract
An analysis of nondiffusing and diffusing space‐charge effects in growing oxide films using simple models provides justification for the equation L(t)2=L2[1−exp(−t/τ)] as a first approximation for describing film growth, where L(t) is the film thickness and t is the time of oxidation. The limiting film thickness squared L2 and the pseudo rise‐time τ are functions of the space‐charge concentration and are temperature‐dependent, increasing linearly with temperature for most cases. Space‐charge effects for a given defect concentration are predicted to be more important at low temperatures; growth tends to become parabolic at higher temperatures.
Keywords