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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>Model</strong> Formul<strong>at</strong>ionFigure 5-1. Quasi-St<strong>at</strong>ic and Non-Quasi-St<strong>at</strong>ic models for SPICE analysis.5.3.1 SPICE sub-circuit for NQS modelFigure 5-2 gives the RC-subcircuit <strong>of</strong> NQS model for SPICEimplement<strong>at</strong>ion. An additional node, Q def (t), is cre<strong>at</strong>ed to keep track <strong>of</strong> theamount <strong>of</strong> deficit/surplus channel charge necessary to reach theequilibrium based on the relax<strong>at</strong>ion time approach. <strong>The</strong> bias-dependentresistance R (1/R=G tau ) can be determined from the RC time constant ( τ ).<strong>The</strong> current source i cheq (t) results from the equilibrium channel charge,Q cheq (t). <strong>The</strong> capacitor C is multiplied by a scaling factor C fact (with <strong>at</strong>ypical value <strong>of</strong>1×10 – 9) to improve simul<strong>at</strong>ion accuracy. Q def now becomesQdef() t = V × ( 1⋅C)deffact(5.3.1)<strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley 5-3

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