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Percolation models for gate oxide breakdown
522
Citations
27
References
1999
Year
Device ModelingDefect ToleranceElectrical EngineeringEngineeringPhysicsCrystalline DefectsHomogeneous PercolationBias Temperature InstabilityIntrinsic ImpurityApplied PhysicsCondensed Matter PhysicsPercolation PathTime-dependent Dielectric BreakdownDefect FormationPercolation ModelsMicroelectronicsDielectric BreakdownPhysic Of Failure
Percolation scaling relations are only valid for large finite systems near the critical probability. The study investigates percolation behavior in very small samples comparable to lattice spacing. Computer simulations of percolation paths on finite lattices, including homogeneous and nonuniform site densities, model dielectric breakdown in these small samples. The simulations show that oxide breakdown statistics and thickness dependence are quantitatively captured, with critical defect density dropping below ~5 nm and plateauing below 3 nm, an effective defect size of ~3 nm, singular behavior when thickness falls below this size, and a ~10⁻³ probability that a percolation path initiates destructive breakdown.
Computer calculations of the formation of a percolation path across a finite lattice are used to model dielectric breakdown. The classical scaling relations for percolation are expected to be valid only for large (finite) systems near pc. We investigate the opposite limit of very small samples, comparable to the lattice spacing. It is shown that relatively simple numerical calculations can quantitatively describe the statistics and thickness dependence of oxide breakdown in thin samples. The critical defect density for breakdown shows a strong decrease with thickness below about 5 nm, then becomes constant below 3 nm. Both of these features can be quantitatively explained by percolation on a finite lattice. The effective defect “size” of about 3 nm is obtained from the thickness dependence of the breakdown distributions. The model predicts a singular behavior when the oxide thickness becomes less than the defect size, because in this limit a single defect near the center of the oxide is sufficient to create a continuous path across the sample. It is found that a given percolation path has a probability of about 10−3 for initiating destructive breakdown. We investigate both homogeneous percolation and percolation in a nonuniform density of sites.
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