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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

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

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Strong Inversion Current and Output Resistance (S<strong>at</strong>ur<strong>at</strong>ion Regime)equal to P diblc1 and D vt1 is not equal to D rout is because the g<strong>at</strong>e voltagemodul<strong>at</strong>es the DIBL effect. When the threshold voltage is determined, theg<strong>at</strong>e voltage is equal to the threshold voltage. But in the s<strong>at</strong>ur<strong>at</strong>ion regionwhere the output resistance is modeled, the g<strong>at</strong>e voltage is much larger thanthe threshold voltage. Drain induced barrier lowering may not be the same<strong>at</strong> different g<strong>at</strong>e bias. P diblc2 is usually very small (may be as small as8.0E-3). If P diblc2 is placed into the threshold voltage model, it will notcause any significant change. However it is an important parameter inV ADIBL for long channel devices, because P diblc2 will be dominant in Eq.(2.6.8) if the channel is long.2.6.3 Current Expression without Substr<strong>at</strong>e Current InducedBody EffectIn order to have a continuous drain current and output resistanceexpression <strong>at</strong> the transition point between linear and s<strong>at</strong>ur<strong>at</strong>ion region, theV As<strong>at</strong> parameter is introduced into the Early voltage expression. V As<strong>at</strong> isthe Early Voltage <strong>at</strong> V ds = V ds<strong>at</strong> and is as follows:VAs<strong>at</strong>=(2.6.9)Es<strong>at</strong> L+ Vds<strong>at</strong> + 2Rdsvs<strong>at</strong>CoxW( Vgst − AbulkVds/ 2)1 + Abulk Rdsvs<strong>at</strong>CoxWTotal Early voltage, V A , can be written as(2.6.10)VA1 1 −1= VAs<strong>at</strong>+ ( + )V VACLMADIBL<strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley 2-27

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