esd protection circuits: basics to nano-metric asicsee.sharif.edu/~adic/lecture_esd_40.pdf · 1 esd...
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ESD Protection Circuits: Basics to nano-metric ASICs
Manoj SachdevUniversity of Waterloo
September 2007
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OutlineGroup IntroductionESD BasicsBasic ESD Protection CircuitsNano-metric ESD ChallengeESD circuits for nano-metric regime
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Group Introduction5 PhDs, 2 masters and 2 PDFs
Applied, industrially driven researchGenerous funding levels
Core strengths in circuit design, testing, quality and reliability
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Group: Low Power ResearchDriven by low power signal processing & bio-implantable applications Research focus
Active power reduction, clocking strategiesDynamic voltage scaling architecture for portable app.Leakage power reduction: Investigation of RBB effectiveness with scaling
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Group: High Performance CircuitsDriven by high speed arithmetic circuits (Adders, register files, ALU), and CDRsResearch focus
To build timing diagnostics into multi-GHz ALUsLeakage and active power reductionClock de-skewingThermal issues in high performance circuits
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Group: Memory ResearchDriven by embedded SRAMs and Soft Error RobustnessResearch Focus
SRAM cell stability & ckttechniques for detectionLow power embedded SRAMsSoft Error Robust memories & flip-flopsError Correction Circuit’s for soft error mitigation
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Group: ESD ResearchDriven by reducing chip failures due to ESDResearch Focus
ESD strategies for multiple supply domainsESD protection circuits for High speed I/OsFast response ESD protection circuits
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OutlineGroup IntroductionESD BasicsBasic ESD Protection CircuitsNano-metric ESD Challenge ESD circuits for nano-metric regime
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ESD Basics :Motivation
Electrostatic Discharge (ESD) is responsible for up to 70% of failures in semiconductor industryAn ESD event creates high currents and electric fields in semiconductor devices
High currents may lead to thermal runawayHigh electric fields cause dielectric breakdown
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ESD BasicsWhen two dissimilar materials are separated an ESD charge may develop Caused by the removal of electrons from surface atoms of materialsFactors
Magnitude of static chargeContact qualityRate of separation
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Human Body Model (HBM)
DUT
A BR Rb=1.5k
Cb=100pFV
Mimics the human touching of the Device Under Test (DUT)Voltages as high as 10kV can be developedHBM modeled by series resistance (Rb = 1.5kΩ) and capacitance (Cb = 100pF)
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Machine Model (MM)
DUT
A BR 0.5uH
200pFV
Represents the damage caused by charged machine touching the DUTVoltages as high as 100-500V can be generatedMM is modeled by capacitance (C = 200pF) and series inductance of machine (0.μ5H)
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Charge Device Model (CDM)
DUT
A BR
Cap
V
Discharge event between charged DUT and grounded conductorModeled by Capacitor (Cap) in series with DUTTotal Capacitance (Cap) is dependant on Device, package impedance
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ESD Stress Comparison
HBM rise time ~ 2-10ns, decay time 130-170nsCDM very high amplitude , occurs for 500ps-1000ps
CDM failures on rise due to automated manufacturing
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Negative ESD with respect to VSS
(NS-mode)
Zapping ModesPositive ESD with respect to VSS
(PS-mode)
VDD
VSS
VESD
VDD
VSS
VESD
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Zapping ModesPositive ESD with respect to VDD
(PD-mode)
Negative ESD with respect to VDD
(ND-mode)
VDD
VSS
VESD
VDD
VSS
VESD
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HBM / MM / CDM TestersHBM/MM/CDM testers apply ESD stress to the DUTMagnitude/polarity of the stress set by the userTest can be destructive
Results in pass or fail
The device fails when leakage is increased significantly
ICMS-700 HBM/MM tester
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TLP TesterTransmission Line Pulse (TLP) is becoming popular
Measures I-V characteristic of the DUT Non-destructive
Programmable current pulse of 100ns are applied to the DUT2nd breakdown current determines the ESD robustness
Barth 4002 TLP tester
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OutlineGroup IntroductionESD BasicsBasic ESD Protection CircuitsNano-metric ESD Challenge ESD circuits for nano-metric regime
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ESD Protection MethodsSnapback-based
Turn on before oxide breakdown Minimum parasitics
Non-snapback-basedTrigger and conduct during the whole ESD eventDo not trigger under normal power-up
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Diode Under ESD ConditionsForward biased:
Low trigger voltageLow on resistance
Reverse biased:High trigger voltageHigh on resistance
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MOS Under ESD ConditionsHas a parasitic bipolar transistor
Avalanche breakdown gives Igen and Isub
When Vbase = 0.7V, npn turns on SnapbackWhen I(drain) = It2 , npn can be destroyed
p-sub
Drain
n+ n+Igen
IsubVbase
Rsub
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Snapback Protection: MOSFETMOSFET is used in Grounded- Gate configuration (GGNMOS)
Substrate and Gate triggering is often needed
I/OPAD
VDDPAD
VSSPAD
PreDriver
PreDriver
Buffer stageESD ProtectionDevice
GGNMOS
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ESD Protection Wish ListVt1 < Oxide breakdown
To trigger NMOS before oxide breaks downVt2 > Vt1
To ensure uniform triggering of all fingersVh > VDD
To enhance latch-up immunity (VDD + 10%)It2 as high as possible
Increase current carrying capability ↑ESD
A GGNMOS cannot meet all the above requirements for contemporary technologies
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SCR Under ESD ConditionsSCR is a pnpn device
In CMOS the junctions are: p+-nwell-psub-n+
p-sub
Anode
n-well
n+ p+n+p+I/O
PAD
VDDPAD
VSSPAD
PreDriver
PreDriver
Buffer stageESD ProtectionDevice
n+
p+
n-
p-
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SCR CharacteristicAvalanche breakdown of nwell-psub ↑ IRnwell and IRpsub
When VBE reaches 0.7V, npn (or pnp) turns onPositive feedback turns on the pnp (or npn) Snapback
Anode
Rp-sub
Rn-well
I(anode)
V(anode)
(Vt1, It1)
(Vh, Ih)
(Vt2, It2)
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ESD Devices: ComparisonProtection level:
SCR and FB diode are the best
Trigger voltage:FB Diode is too lowNMOS is the bestSCR should be modified
Holding voltage: NMOS is ok SCR should be modified
Figure of meritProtection level/Capacitance
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Non-Snapback Protection: ClampsESD event V(1) rises turning on M0
RCCC + inverters should keep M0 “on” to discharge all ESD energyAdvantages
Protect against different zapping conditions
DisadvantagesCan turn on during normal power-up
ESD event:tr: between 100ps and 60nsduration: up to 1μs
Regular power-up:In millisecond range
Hot plug app. power-upas low as 1μs
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OutlineGroup IntroductionESD BasicsBasic ESD Protection CircuitsNano-metric ESD Challenge ESD circuits for nano-metric regime
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Challenges with Scaling
Breakdown Voltage of CMOS devices is decreasingTraditional ESD structures not scaling with technology scaling
Larger ULSI, thinner metallization, shallower junctionsIncreasingly difficult to provide low impedance, low capacitancedischarge path
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-6
-4
-2
0
2
4
6
8
10
12
14
0 20 40 60 80 100 120
Current (A)
Time (ns)
HBM
MM
CDM
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Challenges: Charged Device Model
Lower Technologies (90nm , 65nm) damage occur at lower voltagesTraditional ESD circuits trigger slower
High speed chips larger package decoupling capHigher CDM discharge current!!
CDM failures on rise due to automated manufacturing
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Challenges: Multiple Supply Domains
Multiple supply domains in SoC’sPin to pin ESD protection requirementMultiple zapping modes
Challenge to Overcome Noise Coupling & ground-bouncing issues between analog & digital supplies
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Challenges: Multiple Chip Module
Resistance of the path can be very high (Multiple Chip Module)Minimization of Parasitic Capacitance attributed to the High Speed I/O’s due to ESD Circuit
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OutlineGroup IntroductionESD BasicsBasic ESD Protection CircuitsNano-metric ESD Challenge ESD circuits for nano-metric regime
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Strategy – Device SimulationMOS models, circuit simulators are not designed to handle snapback behaviorESD circuits are designed with device simulators (Medici and Sequoia)
Device cross section is created in the simulatorQuasi-DC simulation predicts DC characteristic, i.e. Vt1and Vh
It2 is estimated using thermal simulation and monitoring maximum temperature of the ESD protection device
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Design Steps1. Calibrate the device simulator with the
desired technology Junction depth and substrate doping are available from technology documents
2. Verify the technology model by simulating a MOS transistor
Trial and error is used to achieve the typical I(on), Vth, current gain and
3. Draw the cross-section of the ESD device
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Design Example #1 – LVTSCR
Mesh of the Low-Voltage-Triggered SCR (LVTSCR) created in MediciReducing grid spacing increases accuracy and simulation time
p-typen-typecontactoxide
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Snapback Protection RequirementsReduce first breakdown voltage
SCR has higher Vt1 compared to MOSVt1 of both MOS and SCR are higher than oxide breakdown voltage
Latch-up immunityVery important in SCR devices
Increasing second breakdown currentSCR has higher It2 per width
Reducing parasitic capacitanceSCR provides protection with less capacitance
I(anode)
V(anode)
(Vt1, It1)
(Vh, Ih)
(Vt2, It2)
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3.4
3.6
3.8
4
4.2
4.4
4.6
4.8
5
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5
V(Gate) (V)
Vt1
(V)
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Gate-Coupling↑Vgs ↑Isub npn triggers faster ↓Vt1
For higher Vgs (strong inversion region): impact ionization is decreased Vt1 increases
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2
2.5
3
3.5
4
4.5
5
0 0.25 0.5 0.75 1 1.25 1.5
V(Sub) (V)
Vt1
(V)
40
Substrate Triggering↑Vsub Transistor triggers with lower ↓Vt1
n+n+
p-sub
Drain
Sub
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GST-LVTSCRSCR is modified by adding a gate electrode to reduce Vt1(LVTSCR)MG provides gate triggering
Can be as small as 5μm
MS provides substrate triggeringSimulation results
Vt1 reduces from 12V to 4.85V
Semenov et. al., Microelectronics Reliability, 2005
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GST-LVTSCR (Measurement)GST-LVTSCR was fabricated in 0.13μm CMOS technologyTLP measurements
Vt1 = 5VIt2 = 1.8A
HBM measurementsDevice passes ±3kV 0.00E+00
5.00E-01
1.00E+00
1.50E+00
2.00E+00
2.50E+00
0 2 4 6 8 10
Voltage (V)
Current (A)
1.00E-12 1.00E-10 1.00E-08 1.00E-06 1.00E-04
Leakage (A)
TLP I-VTLP Leakage
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Example #2 – Increasing VhIn holding region both Q1 and Q2 are in saturationSCRVh= VEB1+ VCE2(sat)
High Vh SCR (RE is added)Vh = VEB1+ VCE(sat) + REI1Vh = VEB1 + VCE(sat)+ VEB1RE/Rn-well
RE↑ → Vh↑
Cathode
Anode
RE
Rn-well
Q1
Q2
Rp-sub
I1
I2
n+ p+ n+ p+
p-sub
n-well
Anode CathodeRE
Semenov et. al., ISQED, 2004
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1E-12
1E-10
1E-08
1E-06
0.0001
0.01
10 5 10 15 20 25
V(anode) (V)
Log I(anode) (A)
SCR
R=2k
R=5k
0.00E+00
2.00E-02
4.00E-02
6.00E-02
8.00E-02
1.00E-01
1.20E-01
0 1 2 3 4 5 6 7 8
V(anode) (V)
I(anode) (A)
LVTSCRHighVhMOSHighVhDiode
Increasing Holding VoltageSimulation results
Applied to SCRVh is increased without an increase in Vt1
RE is implemented with diode and MOS and applied to LVTSCRTLP Measurement results
Vh is increased from 2.29V to 3.49V and 4.55VIncrease in Vt1 is less than 8%
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Example #3 – ESD Clamps
To solve false triggering, the triggering circuit is divided into rise time detector and delay elementTime constant is approximately 40nsDelay of the delay element should be more than 1μs
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Thyristor-Based Clamp
CMOS thyristor is used to create the delay elementRCCC= 40nsR1 to keep M0 off under normal conditions
VDD
CC
RC
M1
M2 M3
M4
M0
R1
VSS
Rise Time Detector
Delay Element
1 2 3
Hossein et. al., ESD Symposium 2007
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Circuit-Level SimulationThe clamp is circuit simulated with 2kV HBM stressV(3) shows that clamp turns off after 1μsPeak voltage of the clamp is less than 6V
-1
0
1
2
3
4
5
6
7
0E+0 3E-7 5E-7 8E-7 1E-6 1E-6 2E-6
Time (s)
Volta
ge (V
)
VDD
V(1)
V(3)
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Device-Level SimulationDevice simulation is done with SequoiaPeak temperature is in transistor M0
During a 2kV HBM stress Tmax of the clamp is 375KHot-spot is in the gate-drain boundary
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MeasurementsClamp was fabricated in 0.18μm technologyHBM test
Clamp passes 3kV stress and fails at 3.5kV
TLP testLeakage current is 7nASecond breakdown current is 1.8A
0
0.5
1
1.5
2
2.5
0 5 10 15
Voltage (V)
Cur
rent
(A)
1E-09 0.0000001 0.00001 0.001 0.1 10Log Leakage (A)
TLP I-VTLP Leakage
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Example #4 – CML Driver Design
Two stage 3Gbps CML driver is designed in 0.13μm CMOS tech.Bias of the driver is provided through an external resistor
Diff. Input 400mV
Diff. Output 800mV
Rise/fall time 150ps
Jitter 1ps
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Measured Results
0
1000
2000
3000
4000
5000
0 100 200 300 400 500 600 700
ESD Capacitance (fF)
Jitter (fs)
Vout tr Jitter
CML (simulation) 850mV 116ps 229fs
CML+MOS (measured) 500mV 315ps 3.7ps
CML+LVTSCR (measured) 700mV 148ps 700fs
Beyond CESD=150fF jitter increases significantly
Both Protection schemes achieved 3kV HBM protection
Hossein et. al., CICC 2007
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ConclusionESD remains major cause of chip failures
ESD affects entire manufacturing from devices systems
Significant challenges for nano-metric technologiesESD circuit design is an art
Device simulator are useful in design process
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AcknowledgementHelp of Hossein Sarbishaei, SumanjitSingh, and Oleg Semenov is greatly appreciated for this presentation