1993
DOI: 10.1109/16.277326
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A universal large/small signal 3-terminal FET model using a nonquasistatic charge-based approach

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Cited by 54 publications
(32 citation statements)
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“…If present, dispersive effects on the displacement current are assumed to be negligible. On the other hand, nonquasi-static effects at high-frequencies are here neglected on the purely conductive device current, as also widely accepted by many authors [e.g., 5,6]. Since dynamic effects due to dispersive (long-term memory) and nonquasi-static phenomena (short-term memory) are associated to separate current contributions (conductive and displacement, respectively), each of the voltage deviations Dv c , D d may be simply associated in our approach with the modeling of a single kind of dynamics.…”
Section: Gan Large-signal Modelingmentioning
confidence: 96%
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“…If present, dispersive effects on the displacement current are assumed to be negligible. On the other hand, nonquasi-static effects at high-frequencies are here neglected on the purely conductive device current, as also widely accepted by many authors [e.g., 5,6]. Since dynamic effects due to dispersive (long-term memory) and nonquasi-static phenomena (short-term memory) are associated to separate current contributions (conductive and displacement, respectively), each of the voltage deviations Dv c , D d may be simply associated in our approach with the modeling of a single kind of dynamics.…”
Section: Gan Large-signal Modelingmentioning
confidence: 96%
“…This is especially true when dealing with GaN-based circuits, since important self-heating and trap states in the energy bands affect the low-frequency behavior of this kind of devices [2][3][4]. In addition, by considering the increasing operating frequencies of many applications, the nonquasi-static effects related to chargecarriers delay [e.g., [5][6][7][8] should be also accurately taken into account.…”
Section: Introductionmentioning
confidence: 99%
“…The state-dependent (nonlinear) resistors Rcs(x), RcG(x), RCD(x), have the meaning of charging resistors, and implicitly introduce statedependent delay times for the charge storage process (x is the vector of state variables). Their dynamic effects are similar to those produced by the nonlinear relaxation-time approximation [4]. Thus the assumed topology provides a nonquasi-static charge-storage model while preserving the mathematical simplicity required for efficient nonlinearcircuit simulation by the HB technique [3].…”
Section: Model Descriptionmentioning
confidence: 96%
“…Expressions valid for all values of x2 can be derived for the capacitances as well: (4) CGS(X,T)a2E(x,_T) 32E(x, T) CGS(X T) = _(X2 + -'XjX ax,2 +a1x…”
Section: Model Equations and Constitutive Relationsmentioning
confidence: 99%
“…Therefore, in this case, an equivalentcircuit, shown in Figure 7, is first extracted from bias-dependent S-parameter measurements [8]. The bias-dependent intrinsic parameters provide current and charge partial derivatives [9,10]:…”
Section: Large-signal Mesfet Modelmentioning
confidence: 99%