On the Analysis of Parasitic Quantum Effects in Classical MOS Circuits
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Transcript of On the Analysis of Parasitic Quantum Effects in Classical MOS Circuits
MOS-AK ESSCIRC 2004 20.09. Leuven (Belgium)
On the Analysis of Parasitic On the Analysis of Parasitic QuantumQuantum
Effects in Classical MOS CircuitsEffects in Classical MOS CircuitsFrank FelgenhauerFrank Felgenhauer, ,
Simon Fabel, Wolfgang MathisSimon Fabel, Wolfgang Mathis
Institute of Electromagnetic Theory Institute of Electromagnetic Theory and Microwave Techniqueand Microwave Technique
University of Hannover, GermanyUniversity of Hannover, Germany
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
OutlineOutline
IntroductionIntroduction
Simulation StrategySimulation Strategy
SummarySummary
IntroductionIntroduction
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
IntroductionIntroduction
Exponential increase in gate leakageExponential increase in gate leakage– increased power consumptionincreased power consumption– degraded device performancedegraded device performance
Charge carrier quantization in the Charge carrier quantization in the channelchannel– loss of inversion chargeloss of inversion charge– loss of transconductanceloss of transconductance
Polysilicon-gate depletion effectsPolysilicon-gate depletion effects
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MOS-AK ESSCIRC 2004
Scaling into mesoscopic regimeScaling into mesoscopic regime– Increasing influence of qm-effectsIncreasing influence of qm-effects– Changing of device behaviorChanging of device behavior
Question:Question:– Validity of device modelsValidity of device models– Influence in classical circuitsInfluence in classical circuits
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Quantum InterferenceQuantum Interference
Classical Classical CircuitCircuit
Including Including
qm-Effectsqm-Effects
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
OutlineOutline
IntroductionIntroduction
Simulation StrategySimulation Strategy
SummarySummary
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Simulation StrategySimulation Strategy
Spice circuit modelsSpice circuit models
Circuit SimulationCircuit Simulation
Quantum-mechanical modeling Quantum-mechanical modeling and numerical simulationand numerical simulation
Qm-Effects in MOS devicesQm-Effects in MOS devicesQm-Effects in MOS devicesQm-Effects in MOS devices
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
QM-Effects in MOS DevicesQM-Effects in MOS Devices
Tunneling currentsTunneling currents Charge quantizationCharge quantization
Oxide
n+ Gatep Substrate
(or Soure/Drain extension)
EC
EC
TunnelingCurrent
a)
n(x)
b)
quantumclassical
Oxide p Substrate
Gate
Source Drain
Itc
Its Itd
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
MOSFETMOSFET– Tunneling Currents (channel – gate, edge Tunneling Currents (channel – gate, edge
direct tunneling)direct tunneling)– Charge quantizationCharge quantization
MOS CapacitorMOS Capacitor– Channel – gate tunnelingChannel – gate tunneling– Charge quantizationCharge quantization
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Simulation StrategySimulation Strategy
Spice circuit modelsSpice circuit models
Circuit SimulationCircuit Simulation
Quantum-mechanical modeling Quantum-mechanical modeling and numerical simulationand numerical simulation
Qm-Effects in MOS devicesQm-Effects in MOS devices
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Quantum-mechanical Quantum-mechanical ModelingModeling
and Numerical Simulationand Numerical Simulation
Quantum mechanical descriptionsQuantum mechanical descriptions
–Transmission formalismTransmission formalism
–Scattering matrixScattering matrix
–NNon-on-eequilibrium quilibrium GGreen‘s reen‘s ffunction unction formalism (NEGF)formalism (NEGF)
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MOS-AK ESSCIRC 2004
Non-equilibrium, open boundary conditionsNon-equilibrium, open boundary conditions
1-d MOS-structure1-d MOS-structure Time invariant systemTime invariant system Spatial dependent effective mass and Spatial dependent effective mass and
permittivitypermittivity ScatteringScattering
Poisson self-consistencyPoisson self-consistency
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MOS-AK ESSCIRC 2004
Selfconsistent Selfconsistent potentialpotential Tunneling currentTunneling current
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Simulation StrategySimulation Strategy
Spice circuit modelsSpice circuit models
Circuit SimulationCircuit Simulation
Quantum-mechanical modeling Quantum-mechanical modeling and numerical simulationand numerical simulation
Qm-Effects in MOS devicesQm-Effects in MOS devices
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Spice Circuit ModelsSpice Circuit Models
1-d qm simulation1-d qm simulation look-up table modellook-up table model non-linear elements (black box)non-linear elements (black box)
– non-linear current source non-linear current source
tunnelingtunneling– non-linear capacitor non-linear capacitor
MOS C-V, charge quantizationMOS C-V, charge quantization
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Simulation StrategySimulation Strategy
Parasitic effect identificationParasitic effect identification
Spice circuit modelSpice circuit model
Circuit SimulationCircuit Simulation
Quantum-mechanical modeling Quantum-mechanical modeling and numerical simulationand numerical simulation
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Circuit SimulationCircuit Simulation
(Choi et al, Transaction on Electron Devices ´01)
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MOS-AK ESSCIRC 2004
VVoutout
VVinin
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(Choi et al, Transaction on Electron Devices ´01)
VxVxVoutVout
VaVa
VbVb
ClockClock
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ClockClock
VaVa
VbVb
VxVx
VouVoutt
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(Nii et al, IEEE Journal of Solid States ´04)
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Leakage CurrentsLeakage Currents
3.6296
9.1743
0
2
4
6
8
10
12
14
Standby leakage (pA/cell)
1.2
Supply Voltage (V)
Ioff
Ig
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
OutlineOutline
IntroductionIntroduction
Simulation StrategySimulation Strategy
SummarySummary
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
SummarySummary Numerical simulationNumerical simulation
Spice modelsSpice models
Circuit simulationCircuit simulation
Circuit functionality – quantum effectsCircuit functionality – quantum effects
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Felgenhauer Uni Hannover20.09.2004
MOS-AK ESSCIRC 2004
Classical descriptionClassical description– Drift-DiffusionDrift-Diffusion– Hydrodynamic transport equationHydrodynamic transport equation– Boltzmann transport equationBoltzmann transport equation
Semi-classical description (QM-Semi-classical description (QM-corrections)corrections)– Density GradientDensity Gradient– Quantum hydrodynamic equationQuantum hydrodynamic equation
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Poisson equation
Schrödinger equation
Electron density n Potential U
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Schrödinger equationSchrödinger equation
Density matrixDensity matrix
Electron densityElectron density
Poisson equationPoisson equation 2DU q N n
*
',
( ) ( ) ( ')r r
n r r r
0
1( )
2F E A E dE
( ) ( )H U r E r
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Impact in CircuitsImpact in Circuits
Static CMOSStatic CMOS– Off-state power dissipationOff-state power dissipation
Dynamic CMOSDynamic CMOS– Off-state power dissipationOff-state power dissipation– Discharge breakdown, parasitic currentsDischarge breakdown, parasitic currents
Analog – mixed Signal Analog – mixed Signal – Discharge breakdown, parasitic currentsDischarge breakdown, parasitic currents– Magnitude variationMagnitude variation
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QM transport processQM transport process
Integral Integral valuesvalues
I,UI,U
Integral Integral valuesvalues
I,UI,U
Circuit Circuit modelingmodeling
Circuit Circuit modelingmodelingPhysical Physical
LayerLayer