13.07.2015 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Mobility <strong>Model</strong>µeffµ=01 + ( E E )eff0ν(2.2.2)Values for µ 0 , E 0 , and ν were reported by Liang et al. [15] and Toh et al. [16] to bethe following for electrons and holesParameter Electron (surface) Hole (surface)µ 0 (cm 2 /Vsec) 670 160E 0 (MV/cm) 0.67 0.7ν 1.6 1.0Table 2-1. Typical mobility values for electrons and holes.For an NMOS transistor with n-type poly-silicon g<strong>at</strong>e, Eq. (2.2.1) can be rewrittenin a more useful form th<strong>at</strong> explicitly rel<strong>at</strong>es E eff to the device parameters [14]EeffVgs+ Vth≅6Tox(2.2.3)Eq. (2.2.2) fits experimental d<strong>at</strong>a very well [15], but it involves a very timeconsuming power function in SPICE simul<strong>at</strong>ion. Taylor expansion Eq. (2.2.2) isused, and the coefficients are left to be determined by experimental d<strong>at</strong>a or to beobtained by fitting the unified formul<strong>at</strong>ion. Thus, we have2-16 <strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!