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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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Extrinsic CapacitanceFigure 4-4 illustr<strong>at</strong>es the universality <strong>of</strong> CTM model by compariing C gg <strong>of</strong> a SiON/Ta 2 O 5 /TiN g<strong>at</strong>e stack structure with an equivalent T ox <strong>of</strong> 1.8nm between d<strong>at</strong>a,numerical quantum simul<strong>at</strong>ion and modeling [32].10.07.5Measured Q.M. simul<strong>at</strong>ion CTM18A equivalent SiO 2thicknessCgg (pF)5.02.50.0TiN60A Ta 2O 58A SiONp-Si-2 -1 0 1 2 3Vgs (V)Figure 4-4. Universality <strong>of</strong> CTM is demonstr<strong>at</strong>ed by modeling the Cgg <strong>of</strong> 1.8nm equivalentT ox N<strong>MOSFET</strong> with SiON/Ta 2 O 5 /TiN g<strong>at</strong>e stack.4.5 Extrinsic Capacitance4.5.1 Fringing Capacitance<strong>The</strong> fringing capacitance consists <strong>of</strong> a bias independent outer fringingcapacitance and a bias dependent inner fringing capacitance. Only the biasindependent outer fringing capacitance is implemented. Experimentally, itis virtually impossible to separ<strong>at</strong>e this capacitance with the overlapcapacitance. Nonetheless, the outer fringing capacitance can betheoretically calcul<strong>at</strong>ed by2ε⎛ toxCF ln⎜1+π ⎝ Tpoly=ox⎞⎟⎠(4.5.1)<strong>BSIM3v3.2.2</strong> Manual Copyright © 1999 UC Berkeley 4-19

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