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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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Subthreshold Drain CurrentV1 PSCBE2 PSCBE1ASCBEl= exp( − )L V − Vdsds<strong>at</strong>(2.6.17)<strong>The</strong> variables P scbe1 and P scbe2 are determined experimentally.2.7 Subthreshold Drain Current<strong>The</strong> drain current equ<strong>at</strong>ion in the subthreshold region can be expressed as [2, 3]IdsV V V Vdsgs−th−<strong>of</strong>f= Is0 ( 1−exp( − )) exp( )vnv tttm(2.7.1)I= µs0 0WLqεsiNchv2φs2t(2.7.2)Here the parameter v t is the thermal voltage and is given by K B T/q. V <strong>of</strong>f is the<strong>of</strong>fset voltage, as discussed in Jeng's dissert<strong>at</strong>ion [18]. V <strong>of</strong>f is an importantparameter which determines the drain current <strong>at</strong> V gs = 0. In Eq. (2.7.1), theparameter n is the subthreshold swing parameter. Experimental d<strong>at</strong>a shows th<strong>at</strong> thesubthreshold swing is a function <strong>of</strong> channel length and the interface st<strong>at</strong>e density.<strong>The</strong>se two mechanisms are modeled by the following(2.7.3)C C V C V D L effDL eff( dsc + dscd ds + dscb bseff )⎛⎜exp( − VT + −⎞1 ) 2exp( VT1) ⎟Cd⎝ 2ltlt⎠ Cn= 1+ Nfactor++CoxCoxCitoxwhere the term2-30 <strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley

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