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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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Methodology for Intrinsic Capacitance <strong>Model</strong>ings<strong>at</strong>ur<strong>at</strong>ion region is assumed to be zero. This is a good approxim<strong>at</strong>ion forlong channel devices but fails when L eff < 2 µm. If we define a drain bias,V ds<strong>at</strong>,cv , in which the channel charge becomes a constant, we will find th<strong>at</strong>V ds<strong>at</strong>,cv in general is larger than V ds<strong>at</strong> but smaller than the long channel V ds<strong>at</strong> ,given by V gt /A bulk . However, in old long channel charge models, V ds<strong>at</strong>,cv isset to V gt /A bulk independent <strong>of</strong> channel length. Consequently, C ij /L eff has nochannel length dependence (Eqs. (4.3.6), (4.37)). A pseudo short channelmodific<strong>at</strong>ion from the long channel has been used in the past. It involvedthe parameter A bulk in the capacitance model which was redefined to beequal to V gt /V ds<strong>at</strong> , thereby equ<strong>at</strong>ing V ds<strong>at</strong>,cv and V ds<strong>at</strong> . This overestim<strong>at</strong>ed theeffect <strong>of</strong> velocity s<strong>at</strong>ur<strong>at</strong>ion and resulted in a smaller channel capacitance.<strong>The</strong> difficulty in developing a short channel model lies in calcul<strong>at</strong>ing thecharge in the s<strong>at</strong>ur<strong>at</strong>ion region. Although current continuity stipul<strong>at</strong>es th<strong>at</strong>the charge density in the s<strong>at</strong>ur<strong>at</strong>ion region is almost constant, it is difficultto calcul<strong>at</strong>e accur<strong>at</strong>ely the length <strong>of</strong> the s<strong>at</strong>ur<strong>at</strong>ion region. Moreover, due tothe exponentially increasing l<strong>at</strong>eral electric field, most <strong>of</strong> the charge in thes<strong>at</strong>ur<strong>at</strong>ion region are not controlled by the g<strong>at</strong>e electrode. However, onewould expect th<strong>at</strong> the total charge in the channel will exponentiallydecrease with drain bias. Experimentally,VV,< V,< V,=active →∞Agsteff ,cvds<strong>at</strong> iv ds<strong>at</strong> cv ds<strong>at</strong> iv Lbulk(4.3.9)and V ds<strong>at</strong>,cv is modeled by the following4-8 <strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley

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