System-level ESD protection of high-voltage tolerant IC pins – A case study
1. System-level ESD protection of high-voltage tolerant IC
pins – A case study
Mirko Scholz 1
, Steven Thijs, Shih-Hung Chen 2
, Alessio Griffoni, Dimitri Linten,
Masanori Sawada 3
, Gerd Vandersteen 1
, Guido Groeseneken 2
imec, Kapeldreef 75, 3001 Leuven, Belgium
(1) also at: Vrije Universiteit Brussels, Dept. ELEC, Brussels, Belgium;
(2) also at: Katholieke Universiteit Leuven, Dept. ESAT, Leuven, Belgium;
(3) HANWA Electronics Ltd., Wakayama, Japan
email: mirko.scholz@imec.be
Zusammenfassung – Mit und ohne anliegende Versorgungsspannung wurde eine Systemebene-ESD
Schutzlösung für HVT IC-Pins untersucht. Die transiente Wechselwirkung des untersuchten SCRs mit
den Komponenten auf Systemebene muss sorgfältig geprüft werden, um einen thermischen Ausfall des SCR
zu verhindern, wenn keine Versorgungsspannung angelegt ist und Latchup, wenn der SCR eingeschaltet ist.
Abstract – A system-level ESD protection solution for HVT IC pins is studied without and with applied
supply voltage. The transient interaction of the studied SCR with the off-chip components needs to be
studied carefully to prevent a thermal failure of the SCR when no VDD is applied and latchup when the SCR
is powered up.
1 Introduction
Integrating high-voltage (HVT) circuitry into a
standard low-voltage CMOS process is one of the
challenging tasks when System-on-chip (SOC)
solutions like line drivers, USB interfaces, display
drivers etc are implemented. These HV-tolerant
(HVT) IC pins operate at higher supply voltages
(VDD) then the used low-voltage technology. Due
to the higher VDD the classical ESD protection
solutions of the used low-voltage process often do
not work. Moreover additional challenges can
occur. For example, due to the higher VDD there is
a higher risk for latch up when the circuit is
powered up.
In this paper, we demonstrate a system-level ESD
protection methodology for HVT IC pins using a
test board and board-level components together
with an on-chip protection device on-wafer. With
measurements and simulations the interaction
between on-chip and off-chip devices is analyzed.
The presented methodology enables the study of
on-chip ESD protection devices under system-
level ESD stress conditions and their interaction
with board-level components even before IC
packaging.
First, we present the test structure and
measurement setup. In the following section the
protection methodology for the non-powered state
is demonstrated. Next we show how to protect the
selected test structure for the case that a supply
voltage is applied to it, followed by some
conclusions.
2 Test structure, test board and
measurement setup
To study the system-level ESD robustness of
HVT IC pins a standard Silicon-Controlled
Rectifier (SCR), manufactured in a 130 nm
CMOS technology, has been selected. The
nominal supply voltages in this technology are 1.2
V and 3.3 V. Due to its high trigger voltage
(~ 15.5 V) during ESD stress and the absence of a
gate oxide it can be safely used as an ESD
protection for HVT circuitry. Due to their known
latchup sensitivity SCRs are usually not used as a
standalone power clamp. In this study we use the
SCR as a “latchup monitor” and thereby working
as a replacement for a latchup sensitive circuit in a
real application.
The SCR used is measured on-wafer. The probe
needles and probe holder parasitic are extracted
beforehand [1] and included in the analysis to
determine the influence of the needle parasitic in
the setup during ESD stress. Off-chip components
are added to the SCR by connecting a dedicated
double layer test board (Figure 1) to the on-wafer
setup. The test board has been manufactured using
an industrial PCB process and FR4 as board
2. material. The top layer contains the PCB traces
and the footprints for required board components
like capacitors, resistors and TVS diodes. The
bottom layer works as ground plane
connected with plated via to the top layer.
Figure 1: Photo of test board for system
experiments; TVSx : TVS diode, Cx
capacitor, Rx: serial components (ESD resistor,
ferrite bead), VDDx: optional supply voltage input,
ESD_IN: input for ESD stress and supply voltage
(optional), OUTx: output to wafer prober (SMA)
The used ESD stress sources are a Transmission
Line Pulse (TLP) and very fast (vf) TLP
HANWA T-5000 for extracting the IV curves of
the devices used. The system-level ESD stress
source is a Human Metal Model (HMM) tester
HANWA HED-W5000M. Next to current probes,
a high impedance passive voltage probe is
connected to the SCR in a KELVIN configuration
to capture the transient behavior of the SCR
during different stress conditions and with
different off-chip configurations.
3 Power-off protection
3.1 Applying the SEED methodo
In white paper 3 [2] the Industry Council on ESD
target levels proposed the so called System
efficient ESD design (SEED) methodology for the
design of off-chip ESD protections meeting
system-level ESD specifications.
suitable off-chip protection the TLP IV curves of
the on- and off-chip ESD protection devices are
captured and compared. If required additional off
chip devices can be added to obtain the desired
system-level protection level.
Figure 2 shows the 100 ns of the SCR and a
selected off-chip ESD protection device
applications. The selected TVS diode turns
around 6.2 V. It has a junction capacitance of
80 pF and a HMM/IEC61000-4-2 robustness of
±30 kV.
the PCB traces
and the footprints for required board components
like capacitors, resistors and TVS diodes. The
bottom layer works as ground plane and is
via to the top layer.
: Photo of test board for system-level ESD
: TVS diode, Cx: decoupling
: serial components (ESD resistor,
: optional supply voltage input,
ESD_IN: input for ESD stress and supply voltage
output to wafer prober (SMA)
The used ESD stress sources are a Transmission-
and very fast (vf) TLP tester
5000 for extracting the IV curves of
level ESD stress
Human Metal Model (HMM) tester
W5000M. Next to current probes,
a high impedance passive voltage probe is
a KELVIN configuration
to capture the transient behavior of the SCR
during different stress conditions and with
odology
In white paper 3 [2] the Industry Council on ESD
target levels proposed the so called System-
efficient ESD design (SEED) methodology for the
chip ESD protections meeting
To select a
chip protection the TLP IV curves of
protection devices are
captured and compared. If required additional off-
chip devices can be added to obtain the desired
shows the 100 ns of the SCR and a
chip ESD protection device for 5 V
d TVS diode turns-on
s a junction capacitance of
2 robustness of
0
1
2
3
4
5
6
0 5 10
Current[A]
Voltage [V]
V
DD
Figure 2: 100ns TLP and 5 ns vfTLP
SCR and TVS diode(On-Semi ESD5Z5.0T1)
Because the TVS diode trigger voltage
is much lower than the V
the TVS diode should shunt the system
stress current until 5.4 A without triggering the
SCR. At higher current level
and goes into snapback
TVS diode. At the moment of snapback
current through the SCR is much higher than the
TLP failing current and thermal
will occur.
However, HMM measurements on the
device with the TVS diode in parallel show
different results. Already at low stress level the
SCR turns on. Figure 3 shows the current through
the SCR device at a HMM
with the TVS diode in parallel
(region A) of the HMM current is conducted
mainly by the TVS diode.
0
0.5
1
1.5
2
0 10 20 30 40
current[A]
Time [ns]
A B
Figure 3: Measured HMM stress current and
current through SCR at SCR
region A: 1st
pulse, region B: 2
At low stress level the TVS diode turns
the 2nd
pulse (region B)
flows mainly through
However at higher stress level the
shared between the SCR and TVS diode
indicating a turn-off of the TVS diode
duration of the HMM current.
10 15 20
SCR
TVS
Voltage [V]
V
T1 SCR
and 5 ns vfTLP IV curves of
Semi ESD5Z5.0T1)
Because the TVS diode trigger voltage VT1 (6.2 V)
VT1 of the SCR (15.5 V)
the TVS diode should shunt the system-level ESD
A without triggering the
At higher current level the SCR will trigger
snapback thereby turning off the
At the moment of snapback the
current through the SCR is much higher than the
thermal failure of the SCR
measurements on the SCR
device with the TVS diode in parallel show
. Already at low stress level the
shows the current through
HMM stress level of 500 V
TVS diode in parallel. The 1st
pulse
HMM current is conducted
40 50 60 70 80
SCR current
HMM source
Time [ns]
: Measured HMM stress current and
current through SCR at SCR trigger level (0.5 kV);
pulse, region B: 2nd
pulse
the TVS diode turns-off before
(region B) rises and the 2nd
pulse
the SCR (Figure 4).
However at higher stress level the 2nd
pulse is
shared between the SCR and TVS diode
of the TVS diode after the
duration of the HMM current.
3. 0
1
2
3
4
5
0 500 1000 1500 2000
SCR
HMM source
TVS
Current[A]
HMM pre-charge voltage [V]
Figure 4: Currents at 30 ns: measured HMM
stress current and current through SCR; calculated
current through TVS diode
The triggering of the SCR already at low HMM
stress level cannot be explained using only the
SEED methodology. Transient information like
for example the voltage overshoot of the TVS
diode is required in addition to the TLP IV data.
Figure 5 shows the vfTLP IV data of the
standalone TVS diode extracted with two different
averaging windows.
(a)
0
5
10
15
20
25
30
0
0.5
1
1.5
2
2.5
3
3.5
0 0.5 1 1.5 2
Voltage[V]
Current[A]
Time [ns]
I II
(b)
0
5
10
15
0 10 20 30 40 50
averaging window I
averaging window II
Current[A]
Voltage [V]
V
T1 SCR
Figure 5: vfTLP IV testing (pulse width: 2 ns; rise
time: 200 ps) of standalone TVS diode: definition
of averaging windows (a) and extracted vfTLP IV
curves (b); averaging window I (0.3 ns to 0.6 ns)
and II (1.7 ns to 1.9 ns)
Averaging window I is defined at the beginning of
the vfTLP pulse. Voltage and current have a more
transient character. Averaging window II is
defined at the end of the vfTLP pulse where
voltage and current are more quasi-static.
The vfTLP IV curve extracted with averaging
window I reaches already at low vfTLP stress
level (1.6 A) the VT1 of the SCR. This agrees well
with the measured HMM peak current (1.65 A) at
the SCR trigger level. By adding this transient
information the SEED methodology can be
extended with data which is required to fully
understand the interaction between on-chip and
ESD off-chip protection device.
The SCR triggering already at low stress level
impacts the system-level ESD robustness of the
device when the TVS diode is placed in parallel.
The expected failure level from the SEED
methodology and by using the relation established
in [3] would be 2.9 kV. However the real failure
level with added TVS diode is only 2.1 kV (Table
1).
Table 1: Failure level of standalone SCR and SCR
with TVS diode in parallel (no VDD applied)
HMM [kV]
SCR standalone (measured) 1.4
SCR with TVS (measured.) 2.1
SCR with TVS
(predicted by SEED)
2.9
Most of the 2nd
pulse current goes through the
SCR and only a smaller part is conducted by the
TVS diode. At a HMM stress level of 2.1 kV, the
residual current through the SCR causes thermal
breakdown (Figure 6).
Figure 6: Current through SCR with and without
TVS diode in parallel; stress level: failure level
Similar to the triggering of the SCR at low stress
level the sharing of the 2nd
pulse current at higher
stress level between SCR and TVS diode cannot
be explained by the SEED methodology. HMM
simulations are required which are demonstrated
in the following section.
0
1
2
3
4
5
0 50 100 150 200
SCR standalone 1.4 kV
SCR with TVS, 2.1 kV
current[A]
Time [ns]
4. 3.2 Transient analysis with SPICE
simulations
3.2.1 Simulation setup
To study the transient behavior of on- and off-chip
protection devices SPICE simulations are carried
out with LTSPICE (Figure 7).
HMM
tester
TVS SCR
probe
needles
IHMM
ITVS ISCR
Figure 7: Simulation setup for transient analysis;
IHMM – HMM current, ITVS – current through TVS
diode, ISCR – current through SCR
The HMM tester is modeled according to [4]. The
TVS diode is modeled with a standard SPICE
model based on the datasheet and TLP data. To
approximate and model the overshoot of the TVS
diode an inductance is added in series and its
value matched to measurement data obtained from
the standalone TVS diode mounted in the test
board. This simplification is used because the
TVS diode consists of only one physical diode
and it is used in reverse mode.
Figure 8 shows the voltage across the TVS diode
during simulated and measured HMM stress.
Similar current and voltage waveforms are
obtained with the simulated TVS model.
(a)
0
0.5
1
1.5
2
2.5
3
3.5
4
0 50 100 150 200
simulation
measurement
Current[A]
Time [ns]
(b)
0
5
10
15
20
25
30
35
0 10 20 30 40 50 60
simulated
measured
Voltage[V]
Time [ns]
Figure 8: Current through (a) and voltage (b)
across the TVS diode, comparison measurements
and simulations; stress level: 1 kV
The SCR is modeled by modifying a SPICE
model of a commercial discrete SCR. This
behavioral model contains information like the
trigger behavior, on-resistance and holding current
and gives a good approximation of the real device
behavior in the transient domain.
Figure 9 shows the simulated and measured
voltage across the SCR. Measurement and
simulation data include the parasitic of the probe
needle and probe needle holder. A good
agreement for the voltage after snapback is
obtained. The overshoot before device snapback
in the simulation is significant higher. This is
attributed to bandwidth limitations of the voltage
probe used during the measurement.
0
10
20
30
40
50
0 10 20 30 40 50 60
simulated
measured
Voltage[V]
Time [ns]
Figure 9: Voltage across standalone SCR;
comparison simulation and measurement; stress
level: 0.5 kV
To verify the accuracy of the simulation setup,
first the SCR triggering is simulated with the TVS
diode in parallel. In Figure 10a the current
through the SCR is shown for the stress level
when the SCR turn on. In Figure 10b the current
through the SCR at a higher stress level is plotted.
For both stress level a good agreement between
simulation and measurement is obtained.
5. (a)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
0 50 100 150 200
simulation
measurement
Current[A]
Time [ns]
(b)
0
0.5
1
1.5
2
2.5
3
3.5
0 50 100 150 200
simulation
measurement
Current[A]
Time [ns]
Figure 10: Current through SCR with TVS diode in
parallel: a) stress level: 0.5 kV, b) stress level:
1.5 kV; comparison between measurement and
simulation; no VDD
3.2.2 Transient analysis
For the transient analysis different pre-charge
voltages are simulated and the voltages and
currents at different locations in the schematic are
extracted. Figure 11 shows the voltage across the
TVS diode and across the SCR for two pre-charge
voltages. The TVS turns-off at low stress level
(Figure 11a). The low holding voltage of the SCR
and the voltage across the probe holder and probe
needle parasitic are not high enough to keep the
TVS diode on. More voltage drops at a higher
stress level keeping the TVS diode also on during
the duration of the 2nd
pulse of the HMM current
(Figure 11b).
(a)
(b)
Figure 11: Simulated voltages across TVS diode
and SCR: (a) stress level: 0.5 kV, (b) stress level:
1.5 kV
The current distribution between the SCR and
TVS during HMM stress is directly influenced by
this device behavior. Figure 12a shows the current
through TVS diode and SCR when the TVS diode
turns off during the duration of the HMM pulse.
Only the 1st
pulse of the HMM current is
conducted by the TVS diode. The 2nd
pulse is
fully conducted by the SCR.
(a)
-0.5
0
0.5
1
1.5
2
0 50 100 150 200
TVS
SCR
Current[A]
Time [ns]
(b)
0
1
2
3
4
5
0 50 100 150 200
TVS
SCR
Current[A]
Time [ns]
Figure 12: Simulated currents through TVS diode
and SCR: (a) stress level: 0.5 kV, (b) stress level:
1.5 kV
Figure 12b shows the current distribution when
the TVS diode stays on during the 2nd
pulse. The
1st
pulse and the 2nd
pulse are shared between SCR
and TVS diode.
The obtained results clearly show why the SEED
methodology cannot be used. Depending on the
0
5
10
15
20
25
30
0 50 100 150 200
SCR
TVS
Voltage[V]
Time [ns]
V
T1
TVS
0
5
10
15
20
25
30
0 50 100 150 200
SCR
TVS
Voltage[V]
Time [ns]
V
T1
TVS
6. applied HMM stress the TVS diode can be turned
off by the SCR snapback or stays on during the
duration of the HMM stress. HMM simulations or
measurements are required to fully explain this
device behavior.
3.3 Designing the system-level ESD
protection
An additional current limiting resistor is required
to limit the residual current through the SCR to a
safe value. The methodology in [5] is used to
calculate the required resistance value for the peak
current of 8 kV HMM. The safe current level is
taken at 2 A for the SCR. With this data, the on-
resistance of TVS diode and SCR and by applying
Kirchhoff’s current laws a resistor value of about
7.3 Ω is obtained. The closest available value in
the lab was 8.2 Ω. With the added isolation
resistor the residual current through the SCR stays
at a safe level even at 8 kV HMM stress (Figure
13).
0
1
2
3
4
5
0 50 100 150 200
SCR standalone 1.4 kV
SCR + TVS + RISO, 8 kV
current[A]
Time [ns]
Figure 13: Current through standalone SCR
(failing waveform) and with added TVS diode and
ESD resistor
4 Power-on protection
To study the behavior of the protected SCR under
powered conditions a typical decoupling capacitor
(SMD1206, thick film, 1 µF) and a VDD source
(Agilent E3136A) with an additional 75 V
discrete zener diode as blocking device are added
to the setup (Figure 14). For all power-on testing
the VDD is set to 5 V and the VDD compliance to
100 mA.
Figure 14: Setup for power-on testing [6]
At a HMM stress level of 800 V the SCR triggers
and goes into latchup (Figure 15 a). This is
indicated by a sudden drop of the supply voltage
and a strong increase of the supply current. The
fast rise time of the HMM current together with
the intrinsic inductance of the capacitor used
cause a voltage overshoot which is not suppressed
fully by the TVS diode.
(a)
0
2
4
6
8
10
12
14
0 500 1000 1500
700V
800V latchup
Voltage[V]
Time [ns]
I
VDD
@ 600 V: < 1 µA
I
VDD
@ 800 V: 100 mA
(b)
-0.1
0
0.1
0.2
0.3
0.4
0.5
0 500 1000 1500
700V
800V latchup
Current[A]
Time [ns]
Figure 15: Measured voltage across (a) and
current (b) through SCR before and during latchup
After turn-on the SCR snaps back to its holding
voltage. Due to the low on-resistance after
snapback the SCR conducts part of the HMM
current and an additional current which is
discharged from the decoupling capacitor (Figure
15 b). Due to its low holding current of 25 mA the
additional discharge current keeps the SCR in the
latched state even when the HMM current is fully
decayed. Over a longer time scale the SCR
continues staying in the latched state due to a
permanent current flow from the power supply to
the board which is sourced by the power supply to
restore the programmed supply voltage.
4.1 SPICE simulation setup for transient
analysis
To analyze the interaction of the on-chip and off-
chip components under powered conditions,
SPICE simulations are carried out. The setup in
section 3.2 is extended with the components
which are required for the powered ESD testing
(Figure 16).
7. Figure 16: Schematic of power-on simulation setup
in SPICE
The zener diode is modeled with the same
breakdown voltage (75 V) like during
measurements. The decoupling capacitor is
modeled with its equivalent model which consists
of the intrinsic inductance, the parasitic resistance
and the capacitance value.
To verify the power-on simulation setup the
latchup situation is simulated. Figure 17 shows the
simulated voltage across and the current through
the SCR before and during latchup. In the
simulation the SCR latches at the same HMM
stress level like in the measurements proving the
accuracy of the simulation.
0
5
10
15
20
25
0 20 40 60 80 100
0.7 kV
0.8 kV latchup
Voltage[V]
Time [ns]
Figure 17: Simulated voltage across SCR before
and during latchup; VDD = 5 V
With the simulation setup the current distribution
between the off-chip components is extracted.
Below the latchup trigger level (Figure 18a) most
of the HMM current is conducted by the
decoupling capacitor. Only a small part of the 1st
pulse is conducted by the TVS diode. During
latchup (Figure 18b) the SCR triggers. When
reaching its holding voltage the SCR and
decoupling capacitor share first the HMM current.
After the decay of the HMM current the discharge
current from the decoupling capacitor keeps the
SCR on. The negative current in Figure 18 b
indicates this current which flows from the
capacitor through the latched SCR.
(a)
-0.5
0
0.5
1
1.5
2
2.5
3
0 50 100 150 200
HMM
C
decoup
TVS
Current[A]
Time [ns]
(b)
-0.5
0
0.5
1
1.5
2
2.5
3
3.5
0 200 400 600 800 1000
HMM
C
decoup
TVS
Votlage[V] Time [ns]
Figure 18: Simulated currents before and during
latchup: HMM current, current through
decoupling capacitor and TVS diode
4.2 Designing the system-level ESD
protection for the power-on state
Going into latchup during ESD stress is not
allowed for ESD power clamps. Therefore the
design target for the power-on state is to prevent
triggering and subsequent latching of the SCR at a
HMM stress level of 8 kV. The SCR in this case
study is used as a latchup monitor. Therefore the
latchup protection will be demonstrated with
board level components only.
By using the presented SPICE simulation setup a
protection solution preventing SCR triggering is
designed. The proposed solution (Figure 19)
consists of a ferrite bead which is added between
the TVS diode and one decoupling capacitor.
Figure 19: Protection solution with ferrite bead
and RC filter; RISO: 8.2 Ω; Cdecoup: 1 µF; ferrite
bead: Tyco Electronics BMB1-J0070-B08
Ferrite beads are passive components which block
high frequency noise in supply lines. The use of
ferrite beads for preventing latchup has been
8. proposed before [7]. However, a design
methodology was not given.
The isolation resistor together with a second
decoupling capacitor works as a RC filter. It
directs most of the HMM current through the first
decoupling capacitor leaving only a small residual
current for the TVS diode, ferrite bead and second
decoupling capacitor (Figure 20). When
simulating the presented design no latchup occurs
at a stress level of 8 kV HMM.
-5
0
5
10
15
20
25
30
-5
0
5
10
15
20
25
30
0 50 100 150 200
SCR voltage
current through C1
Voltage[V]
Current[A]
Figure 20: Simulated voltage across SCR and
current through first decoupling capacitor (C1)
when SCR is protected with presented protection
solution and powered-up to 5 V; stress level: 8 kV
Figure 21 shows the experimental verification of
the protection solution. At a HMM stress level of
8 kV and a supply voltage of 5 V no latch up in
the SCR occurs.
0
2
4
6
8
10
0 200 400 600 800 1000
SCR voltage
Voltage[V]
Time [ns]
V
DD
Figure 21: Measured voltage across SCR when
protected with presented protection solution and
powered-up to 5 V, HMM stress level: 8 kV
All components of the proposed protection
solution are typically used to decouple and
stabilize the voltage in supply lines and do not add
any additional devices to the bill of material of a
application board.
5 Conclusions
A system-level ESD protection solution for HVT
IC pins has been studied without and with applied
supply voltage. It has been found, that the
transient interaction of the studied SCR with the
off-chip components needs to be carefully studied
to prevent any low failure level of the SCR when
no VDD is applied and moreover to prevent latch
up when the device is powered up. It was
demonstrated that the SEED methodology needs
transient information in addition to the TLP IV
data to ensure a protection design which takes also
into account the transient interaction of on-chip
and off-chip ESD protection with other board-
level components.
By using a SPICE simulator together with suitable
models for all on-chip and off-chip components
an ESD protection solution for the power-on state
during system-level ESD stress has been designed
and experimental verified.
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HBM measurements for quasi-static and
transient device analysis”, in Proc.
EOS/ESD Symposium, 2007, pp. 89–94
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I”, Industry Council on ESD Target Levels,
2011
[3] G. Notermans et al, “HMM and TLP
Correlation”, IEW, 2011
[4] M. Scholz et al, “On-wafer Human Metal
Model measurements for systemlevelESD
analysis”, Proc. EOS/ESD Symposium,
2009, pp. 405–413
[5] S. Marum et al, “Protecting circuits from
the transient voltage suppressor's residual
pulse during IEC 61000-4-2 stress”, Proc.
EOS/ESD Symposium, 2009, pp. 377-386
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