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BSIM3v3.2.2 MOSFET Model - The University of Texas at Dallas

BSIM3v3.2.2 MOSFET Model - The University of Texas at Dallas

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Poly G<strong>at</strong>e Depletion Effect2.9 Poly G<strong>at</strong>e Depletion EffectWhen a g<strong>at</strong>e voltage is applied to a heavily doped poly-silicon g<strong>at</strong>e, e.g. NMOSwith n + poly-silicon g<strong>at</strong>e, a thin depletion layer will be formed <strong>at</strong> the interfacebetween the poly-silicon and g<strong>at</strong>e oxide. Although this depletion layer is very thindue to the high doping concentr<strong>at</strong>ion <strong>of</strong> the poly-Si g<strong>at</strong>e, its effect cannot beignored in the 0.1µm regime since the g<strong>at</strong>e oxide thickness will also be very small,possibly 50Å or thinner.Figure 2-7 shows an N<strong>MOSFET</strong> with a depletion region in the n + poly-silicong<strong>at</strong>e. <strong>The</strong> doping concentr<strong>at</strong>ion in the n + poly-silicon g<strong>at</strong>e is N g<strong>at</strong>e and the dopingconcentr<strong>at</strong>ion in the substr<strong>at</strong>e is N sub . <strong>The</strong> g<strong>at</strong>e oxide thickness is T ox . <strong>The</strong> depletionwidth in the poly g<strong>at</strong>e is X p . <strong>The</strong> depletion width in the substr<strong>at</strong>e is X d . If weassume the doping concentr<strong>at</strong>ion in the g<strong>at</strong>e is infinite, then no depletion regionwill exist in the g<strong>at</strong>e, and there would be one sheet <strong>of</strong> positive charge whosethickness is zero <strong>at</strong> the interface between the poly-silicon g<strong>at</strong>e and g<strong>at</strong>e oxide.In reality, the doping concentr<strong>at</strong>ion is, <strong>of</strong> course, finite. <strong>The</strong> positive charge nearthe interface <strong>of</strong> the poly-silicon g<strong>at</strong>e and the g<strong>at</strong>e oxide is distributed over a finitedepletion region with thickness X p . In the presence <strong>of</strong> the depletion region, thevoltage drop across the g<strong>at</strong>e oxide and the substr<strong>at</strong>e will be reduced, because part<strong>of</strong> the g<strong>at</strong>e voltage will be dropped across the depletion region in the g<strong>at</strong>e. Th<strong>at</strong>means the effective g<strong>at</strong>e voltage will be reduced.<strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley 2-33

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