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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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Extraction Procedureeffects. Regardless <strong>of</strong> device geometry, each device will have to bemeasured under four, distinct bias conditions.(1) I ds vs. V gs @ V ds = 0.05V with different V bs .(2) I ds vs. V ds @ V bs = 0V with different V gs .(3) I ds vs. V gs @ V ds = V dd with different V bs . (V dd is the maximum drainvoltage).(4) I ds vs. V ds @ V bs = V bb with different V gs . (|V bb | is the maximum bodybias).6.3.2 Optimiz<strong>at</strong>ion<strong>The</strong> optimiz<strong>at</strong>ion process recommended is a combin<strong>at</strong>ion <strong>of</strong> Newton-Raphson's iter<strong>at</strong>ion and linear-squares fit <strong>of</strong> either one, two, or threevariables. This methodology was discussed by M. C. Jeng [18]. A flowchart <strong>of</strong> this optimiz<strong>at</strong>ion process is shown in Figure 6-2. <strong>The</strong> modelequ<strong>at</strong>ion is first arranged in a form suitable for Newton-Raphson's iter<strong>at</strong>ionas shown in Eq. (6.3.1):(6.3.1)( m) ( m) ( m)∂f P P P f P P P sim fP P m ∂ fsim m ∂ fsim P sim mexp ( 10, 20,30) − ( 1 , 2 , 3 ) = ∆ 1 + ∆ 2 + ∆P3∂ 1 ∂ P2∂ P3<strong>The</strong> variable f sim () is the objective function to be optimized. <strong>The</strong> variablef exp () stands for the experimental d<strong>at</strong>a. P 10 , P 20, and P 30 represent thedesired extracted parameter values. P(m) 1 , P2(m)and P(m) 3 representparameter values after the mth iter<strong>at</strong>ion.6-4 <strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley

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