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T.J. Kazmierski T.J. Kazmierski l modelling of carbon nanotube field-effect transistors l modelling of carbon nanotube field-effect transistors 1 MOS-AK MOS-AK Munich Munich 14 September 2007 14 September 2007 School of Electronics and Computer Science School of Electronics and Computer Science Southampton University Southampton University Circuit-level modelling of carbon nanotube field- effect transistors Tom J Kazmierski School of Electronic and Computer Science University of Southampton, United Kingdom [email protected] , http://www.syssim.ecs.soton.ac.uk

T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

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Page 1: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 11

MOS-AKMOS-AKMunichMunich

14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Circuit-level modelling of carbon nanotube field-effect

transistors

Tom J KazmierskiSchool of Electronic and Computer ScienceUniversity of Southampton, United Kingdom

[email protected], http://www.syssim.ecs.soton.ac.uk

Page 2: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 22

MOS-AKMOS-AKMunichMunich

14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Outline

o Introduction New efficient methodology for numerical CNT FET modelling based on

piece-wise non-linear approximation o PNL modelling of non-equilibrium mobile charge density

Two PNL approximations leading to closed-form solution of self-consistent voltage equation

o Drain current calculationo Equivalent circuito Simulation experiments demonstrating speed up and modelling

accuracyo Conclusion: what next?

Page 3: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 33

MOS-AKMOS-AKMunichMunich

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Introduction

o CNT FET theory and operation are gradually better understood.o Early CNT FET models simply used MOS equations – no good.o Now a physical theory of ballistic CNT transport exists.o Circuit-level models have been developed based on theory but they

are very complex in terms of computational intensity.o Recently fast models appeared, based on numerical approximation.o Focus of this talk: new, efficient piecewise non-linear approximation

of mobile charge three orders of magnitude faster than evaluation of physical equations,

but still maintaining high accuracy.

o Important for circuit design where very large numbers of CNT devices will need to be simulated.

Page 4: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 44

MOS-AKMOS-AKMunichMunich

14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Non-equilibrium mobile chargeo Non-equilibrium mobile charge is injected into CNT when drain-source voltage

is applied:

o State densities are determined by Fermi-Dirac probability distribution:

VSC – self-consistent voltage

Page 5: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 55

MOS-AKMOS-AKMunichMunich

14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Self-consistent voltage equationVSC - recently introduced concept

Strongly non-linear, requires Newton-Raphson iterations and calculation of integrals – standard approach to CNT FET modelling

Total charge at terminal capacitances

Total terminal capacitance

Page 6: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 66

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14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Standard approaches to evaluate charge density

o Newton-Raphson technique and finite integrationo Non-equilibrium Green’s function (NEGF)o Recently piece-wise linear and piece-wise non-linear

approximations have been proposed to obtain closed-form symbolic solutions The aim is to eliminate the need for computationally intensive

iterative calculations in development of models for circuit simulators

Page 7: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 77

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Total drain currentIf VSC is known, total drain current can be

obtained form Fermi-Dirac statistics directly:

Closed-form solution for Fermi-Dirac integral of order 0 exists:

hence:

Page 8: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 88

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Circuit model of a top-gate CNT FET

If equal portions of the equilibrium charge qN0 are allocated to

drain and source, non-equilibrium charges at drain and

source can be modelled asnon-linear capacitances.

A hypothetical inner node can be created to represent

the self-consistent potential

Page 9: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

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MOS-AKMOS-AKMunichMunich

14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

New technique to accelerate VSC calculationModel 1: 3-piece non-linear approximation of charge density:

solid line: theory

dashed-line: approximation

Linear and quadratic pieces

Page 10: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

New technique to accelerate VSC calculationModel 2: 4-piece non-linear approximation:

solid line: theory

dashed-line: approximation

Region boundaries are optimised for best fit

Linear, quadratic and 3rd order pieces

Page 11: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 1111

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Speed-up due to PNL approximation

FETToy – reference theoretical model implemented in MATLAB

CPU times for PNL Model 1 and Model 2 obtained also from a MATLAB script

Model 1 runs 3500 faster and Model 2 – 1100 times

Page 12: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 1212

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Loss of accuracy due to PNL approximation

Model 1 – dashed, FETToy - solid

Typical parameters: T=300K, Ef = -0.32eV

Model 2 – dashed, FETToy - solid

Page 13: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 1313

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

RMS errors for Ef=-0.32eV

Model 2 accurate within 2%, Model 1 – 4.6%, at T=300K

Page 14: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

T.J. KazmierskiT.J. KazmierskiCircuit-level modelling of carbon nanotube field-effect transistors Circuit-level modelling of carbon nanotube field-effect transistors 1414

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Accuracy at extreme temperatures and Fermi levels

Model 1 – dashed, FETToy - solid

Extreme parameters: T=150K, Ef = 0eV

Model 2 – dashed, FETToy - solid

Page 15: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Accuracy at extreme temperatures and Fermi levels (2)

Model 1 – dashed, FETToy - solid

Extreme parameters: T=450K, Ef = -0.5eV

Model 2 – dashed, FETToy - solid

Page 16: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

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MOS-AKMOS-AKMunichMunich

14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

RMS errors for Ef=-0.5eV

Across T and EF ranges - Model 2 is accurate within 2.8%, Model 1 – 4.8%

Page 17: T.J. Kazmierski Circuit-level modelling of carbon nanotube field-effect transistors 1 MOS-AKMunich 14 September 2007 School of Electronics and Computer

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14 September 200714 September 2007

School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

RMS errors for Ef=0eV

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School of Electronics and Computer ScienceSchool of Electronics and Computer ScienceSouthampton UniversitySouthampton University

Conclusion

o New, fast, numerical CN FET model has been proposedso Suitable for a direct implementation in SPICE-like circuit-level

simulatorso Further evidence to support suggestions that costly Newton-

Raphson iterations and Fermi-Dirac integral calculations can be avoided leading to a substantial speed-up.

o Two models proposed and tested in simulationsso Future work will involve CN FET analysis of speed and modelling

accuracy of circuit structures built of CN FETs.