Accurate model generation is becoming a progressively more important part of the computer-aided design process. Of special importance are large signal models capable of accurately predicting the performance of nonlinear circuits.
LASIMO, part of the MMICAD Suite of software solutions, further expands the data acquisition and modeling capabilities of the MMICAD Version 3 simulator by the fitting of large signal modeling parameters to measured DC and RF data.
This is accomplished in three steps:
| 7 large signal bias-dependent MESFET models | ![]() |
| 2 large signal bias-dependent HEMT models | |
| 4 small signal MESFET and HEMT models | |
| 10 user-defined models | |
| 5 user-reconfigurable large signal models | |
3 small signal analysis modes:
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| 4 versatile optimizers with unique solution search algorithms. |
Supported Large Signal Models
Alpha Own Model, Advanced Curtice, Curtice, Curtice-Ettenberg, Lehovic-Zuleeg, Materka-Kacprzak, Raytheon, Triquint.
BUILT-IN STANDARD MODELS
Ids MESFET Models:
Model 1: Curtice
Model 2: Statz (Raytheon)
Model 3: Materka-Kacprzak
Model 4: Triquint Own Model
Model 5: Advanced Curtice
Model 6: Curtice-Ettenberg
Model 7: Lehovic Zuleeg
Cgs and Cgd MESFET Models:
Model 1: Junction Model
Model 2: Statz (Raytheon)
Model 3: A physically based model
Ids HEMT Models:
Model 1: Curtice
Model 2: Advanced Curtice
Cgs and Cgd HEMT Models:
Model 1: A physically based model
RECONFIGURABLE MODELS
Model 1,2: DC Curtice and Basic Semi-Junction Capacitance
Model 3: TOM3 (room temperature)
Model 4: Alpha Own Model (AOM)
Model 5: TOM3 (with temperature dependence)
USER -DEFINED MODELS
Model 1-5: User assignable. Can also be substituted for the reconfigurable models.
Details on Advanced Models
Alpha Own Model
AOM is a comprehensive model for GaAs MESFETs which expands upon aspects of the Triquint Own Model (TOM) to account for dispersion, self-heating effects, and charge conservation. A set of capacitance and charge equations are used for consistent small- and large-signal models. Transconductance and output conductance dispersion are modeled by combining a feedback network and a subcircuit which describes the self-heating effects. The new model accurately predicts the I-V, CV, bias-dependent S-parameter, waveform, power, and linearity characteristics of the MESFET. This model has been implemented in PSPICE.
Triquint Own Model, Level 3
TOM3 is also a comprehensive model for GaAs MESFETs. It was developed to improve existing MESFET capacitance models for SPICE using conservation of charge in the implanted layer. The capacitance model calculates the gate charge from the drain current and the gate capacitance from the drain conductances. Relating the gate charge to the channel current creates gate capacitances dependent upon the channel current derivatives linking the small-signal model to the large-signal equations. Drain dispersion and self-heating effects are modeled by a GD model using a set of device equations and a specific subcircuit in SPICE.
Triquint Own Model, Level 3, Modified
A variant of the TOM3 model is also provided where the parameters assigned to temperature are not included. For many applications the model can be used quite effectively without the temperature parameters. Speed of extraction is improved.
[1] Optotek Limited, "GaAs MESFET and HEMT Model Extraction Software", Microwave Journal, Vol 38 No 4, April 1995, pp. 274-276
[2] Optotek Limited, "Large-Signal Modelling of MESFETs and HEMTs", Microwave Journal, Vol 40, No 11, November 1997, pp. 162-166).
[3] "C.J. Wei, Y.A.Tkachenko, D. Bartle, S. Dindo, and D. Kennedy, "A Compact Large-Signal Model of a GaAs MESFET", Microwave Journal, Vol 40, No 12, Dec 1997, pp. 22-34
[4] C.J. Wei, Y.A. Tkachenko, and Dylan Bartle, "An Accurate Large-Signal Model of GaAs MESFET which Accounts for Charge Conservation, Dispersion, and Self-Heating", IEEE Transactions on Microwave Theory and Techniques, Vol. 46, No. 11, November 1998.
[5] R.B. Hallgren and P.H. Litzenberg, "TOM3 Capacitance Model: Linking Large- and Small-Signal MESFET Models in SPICE", IEEE MTT, Vol. 47, No. 5, May 1999, pp. 556-561.
[6] R.B. Hallgren and D.S. Smith, "TOM3 Equations", Triquint report dated 14 September, 1998.