| The SDM Test Method: Past, Present, and Future
Michael Chaine, Jon Barth, Tilo Brodbeck, Leo G. Henry, Mark A. Kelly,
and Tom Meuse
The socketed-device model has been a work in progress since the early
1990s.
Evaluating
the sensitivity of electronic components to electrostatic discharge (ESD)
is a key element in controlling and preventing ESD damage. The test procedures
used to characterize, determine, and classify the ESD sensitivity of components
are based on three basic models of ESD events: the human-body model (HBM),
machine model (MM), and charged-device model (CDM). These models differ
in that HBM and MM simulate the electrostatic transfer of a charge to
a device, whereas CDM simulates the electrostatic transfer of a charge
from a device. This article will focus on the charged-device model and
examine issues surrounding a specialized CDM test method based on the
socketed-device model (SDM).
Since the early 1990s, the ESD Association (ESDA) Device Testing Working
Group 5.3 has labored to draft a socketed-charged-device model (S-CDM)
test standard. In the S-CDM test method, the device under test (DUT) is
placed in a socket, and, in theory, only the capacitances of the DUT and
socket are charged. However, attempts to build a test system capable of
charging only the DUT and socket have been unsuccessful: Elements of the
entire test system are unintentionally charged and affect the discharge
event. Consequently, the Device Testing Group now defines this type of
CDM test method as the SDM test method.
To better understand the differences between S-CDM and SDM tester-simulators,
we will review the history of this complex test method, the current design
of existing ESD test equipment, how charge is stored differently in SDM
versus robotic CDM (R-CDM) test systems, and how this difference can produce
a divergence in test results. Finally, we challenge ESD test-equipment
manufacturers to build a second-generation S-CDM test system.
SDM History
SDM terminology was developed in 1997 by Working Group 5.3.2. The term
was derived from S-CDM testing, which refers to the CDM testing of an
integrated circuit (IC) mounted in a socket. This contrasts with R-CDM,
or nonsocketed CDM (ns-CDM), testing, in which the IC is tested in a dead-bug
(pins facing up) configuration and the plastic package is in intimate
contact with a charge plate during the charging process.1 Figures
1 and 2 illustrate the two types of CDM test equipment.
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Figure 2. Nonsocketed CDM.
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These test methods are intended to simulate discharge events that occur
when a charged IC discharges directly through one of its pins into a very-low-impedance
ground, because real-world CDM events can occur during automatic handling
or placement of ICs during manufacturing operations.2 The discharge-current
waveforms from the test equipment show very fast rise times (<1 nanosecond)
and very short pulse duration (<20 nanoseconds; see Figure 3). Both
test methods can produce failure mechanisms such as gate oxide ruptures
in the ICs.
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Figure 3. Typical CDM and SDM discharge-current
waveforms (charging voltage: 1000 V).
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The first CDM tester-simulator was designed in 1979.3 Tester
design improvements attempting to reproduce real-world air-discharge CDM
events (R-CDM) were made during the late 1980s and early 1990s.4,5
Although these simulators proved valuable for reproducing field failures,
they proved only marginally successful for devices with very small pin
pitches and high pin counts. Consequently, test-equipment manufacturers
were asked to produce an automatic simulator that would increase the IC
manufacturer's throughput; hence, the S-CDM tester-simulator was born.
Although S-CDM and R-CDM test equipment were designed differently, both
produced gate oxide failures in many ICs. Early versions of the ESDA CDM
standard, CDM WIP5.3, included both methods.6 Separate specifications
for peak current, rise time, and pulse duration values were given for
each type of CDM test method due to the significant waveform differences
(see Figure 3). From 1992 to 1996, Working Group 5.3 believed that both
test methods could exist in a combined CDM test standard.
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Figure 4. R-CDM gate oxide
damage.
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However, as more IC manufacturers began using both types of CDM test
equipment, major differences in test results occurred. When ICs with different
package configurationsand therefore, variable package-capacitance valueswere
tested, the S-CDM test system results did not produce failure voltages
comparable to R-CDM levels.710 For example, S-CDM failure
voltages remained constant regardless of package configuration and capacitance,
whereas the R-CDM simulator produced failure voltages that varied as a
function of the package capacitance. In other words, the S-CDM test system
could not distinguish between ICs with different package-capacitance values.811
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Figure 5. S-CDM poly melt
and gate oxide damage.
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Failure analysis of ICs tested using both R-CDM and S-CDM simulators
frequently showed the same failure site, but the ICs tested using S-CDM
exhibited more-severe gate oxide damage (see Figures 4 and 5).1214
In some IC technologies, the S-CDM simulator produced electrical failure
signatures that could not be reproduced by the R-CDM test system.14
Attempts to find a general failure-voltage correlation between the test
simulators were unsuccessful, although a very limited one was achieved
for some complementary metal-oxide semiconductor (CMOS) technologies.12
In 1996, Working Group 5.3 split the R-CDM and S-CDM test procedures
into separate documents due to inconsistent failure results and no failure
voltage correlation between test simulators. The same committee decided
in 1997 to rename the S-CDM test method to the SDM test method and create
the new SDM Working Group 5.3.2. A detailed analysis of the operation
of the commercially available SDM tester was published in 1998.15
The paper discussed how the test simulator operated and why a separate
SDM standard test method could not be written. In 2000, 5.3.2 published
a technical application report explaining the SDM test system's unique
capabilities and limitations, as well as how it could be used to perform
CDM testing.16
First-Generation SDM Test System
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Figure 6. Existing SDM test
systems.
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A simplified block diagram of the major components within existing SDM
test systems is shown in Figure 6. The basic elements consist of a high-voltage
(HV) power supply, computer-controlled relay-switch matrix, test-fixture
board and sockets, HV relays, and computer-controlled ground-switch relays.
This design enables the user to place an IC into a socket on the test-fixture
board, define the pins to be charged and discharged, set a charging-voltage
level, and automatically run the test. In addition, test systems typically
include parametric curve trace and leakage measurement equipment, which
can be used to check for pin electrical characteristics before and after
stress. The parametric curve trace measurement, which can only partially
detect electrical failure signatures, has proven very useful for screening
weak or extremely sensitive pins.16
Differences in Device and Tester Capacitances
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Figure 7. Device capitance
for R-CDM test simulators.
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In SDM testers, a significant amount of parasitic capacitance and inductance
is added to the DUT (see Figures 710).14 When a packaged
IC is placed into a socket and the stress voltage is raised to a specific
value, the IC, socket, and background tester parasitics are all raised
to the same potential. After the HV relay switch connects a specified
pin to ground, the total charge in the system is discharged. This total
charge represents the charge stored in the IC, as well as the socket,
test-fixture board, parasitic capacitors in the HV charge line, and unused
floating pins in the socket or test-fixture-board assembly. Generally,
the total background charge can be much more than the charge stored in
the IC and its package.15
In contrast, device capacitance for R-CDM test simulators is generally
defined as the capacitance formed by an IC in relation to a ground plane
(see Figure 7). With the device in a dead-bug configuration (see Figure
2), the capacitance contributions can be summarized as follows: First,
the field-charging electrode of the tester represents one electrode of
the device capacitor. Second, the package material and the dielectric
on the field-charging electrode represent the dielectric of the device
capacitor. Finally, the lead frame and silicon die represent the second
electrode of the device capacitor. Prior to discharge, the first electrode
(the field-charging electrode) will be at ground, and the second electrode
(the lead frame and silicon die) will be at a charging potential (i.e.,
1 kV). Note that within the IC there is no voltage difference after charge-up
and before discharge.
In the R-CDM method, the charge is stored mainly in the IC package (between
the lead frame and the external ground plane), and not in the parasitic
elements of the simulator. In small plastic-packaged devices, the majority
of the charge is stored between the silicon die or die-mounting paddle
and the ground plane, with minor contribution from the lead-frame pins.5
However, the location of the stored charge differs as the number of device
pins increases.
SDM Background Tester Parasitic Elements
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Figure 8. SDM tester parasitics
can be defined as variable and fixed RLC parasitic elements.15
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SDM test simulators enhance test-system parasitics by placing the device
in a socket mounted on a changeable test-fixture board and connected via
pogo pins to a fixed relay-switching matrix. Since the device itself is
not in intimate contact with a ground plane, the stored energy is located
in the tester parasitic capacitive and inductive components, associated
wiring, and, to a lesser degree, the device socket (see Figures 810).15
The SDM discharge sequence is qualitatively similar to the R-CDM sequence
(e.g., discharge pin, device, and capacitance on other nongrounded pins)
but is quite different in quantitative terms. For SDM, the IC package
capacitive components are relatively small, whereas the parasitic capacitance
on the pins due to the tester can be quite large. In fact, it can be so
large that failures can occur to a pin not used as a direct-discharge
pin.15
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Figure 9. Variable external
RLC parasitics.
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Figure 11 shows a simplified schematic of the background tester impedance
at each socket pin of a typical SDM test system. The changeover relay
normally connects to four reed relays. Hence, the capacitance (Cp)
associated with these four relays is connected to the socket pin via a
copper trace on the test-fixture board between the device socket and the
relay matrix. Each device pin electrically inserted into the socket sees
this same parasitic background capacitance. When energized, the changeover
relay is connected to ground and provides a discharge path for the SDM
event.
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Figure 10. Fixed internal RLC
parasitics to SDM tester.
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Although one pin is designated as the charge pin, capacitive coupling
charges all adjacent pins on the HV-relay board when the pin under test
is charged. After the charge-up sequence of the SDM test, all pins on
the board reach an equal voltage. Hence, the total charge in the test
system includes the charge stored in the device and all of the charge
associated with the other internal tester RLC parasitic elements (see
Figures 810). Because there is significant background tester capacitance
of all device pins in the tester (2030 pF), a change in the package
configuration design (e.g., from PLCC28 to PQFP44) may be insignificant
to the total capacitance of the test system.9 For example,
a small change in device capacitance, from 2.8 to 4.4 pF, represents an
increase of 157% for the device in the R-CDM test system; however, the
same change represents much less than 5% of the distributed capacitance
in the SDM test system. This small difference in SDM test-system capacitance
can easily explain why the SDM tester is unable to detect any difference
in failure voltages due to large changes in package capacitance.
Second-Generation SDM Test System
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Figure 11. Simple model for
the SDM tester parasitic elements for each test socket pin. Each
pin has parasitic inductance (Lp), resistance (Rp),
and capacitance (Cp).
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Can the commercially available SDM test systems continue to be used today?
The answer is yes, if overstressing an IC is acceptable. In fact, for
many users, the SDM test system has become a valuable tool in isolating
CDM-sensitive pins and then in verifying the success of redesigns. The
simulator successfully identifies sensitive device pins in some, but not
all, CMOS technologies. The IC failure signatures frequently do agree
with R-CDM failures, but again, not for all CMOS technologies.
Can the existing SDM simulator be expanded to meet the demand for testing
high-pin-count devices? The answer is both yes and no. Attempts to increase
the physical size of the test system to increase the pin count have resulted
in even larger background capacitive and inductive elements. Other efforts,
including customized test-socket boards that divide the high pin count
into smaller pin subgroups, have been more successful since they do not
add more background tester parasitics.
The design of the existing SDM simulator is unique. The amount of charge
stored in the test system is distributed through a complex network of
test-fixture boards, sockets, relays, and other unique RLC elements.15
Changing any of these elements, like replacing a test fixture and socket
board, will modify the amount of charge stored in the system. Any discharge
currents measured from an IC will be a distinct product of this distributive-charge
network. Consequently, writing a standard test method for this type of
ESD test equipment is impossible.
A standard test method must be written in general terms, so that any
test-equipment manufacturer can build a similar system. The existing SDM
design introduces parasitic capacitive and inductive elements that must
be duplicated in order to generate discharge-current waveforms with similar
time-amplitude characteristics. If these waveforms cannot be duplicated
by other SDM test equipment, then the SDM failure voltages will not correlate.
Consequently, the unique properties of the SDM test system prohibit the
development of another system.
Conclusion
In summary, this type of SDM test system cannot be fundamentally improved.
Consequently, a new design for S-CDM test systems must be developed. In
fact, the need increases as the number of IC pins continues to increase
and the pin pitch continues to decrease. If a second-generation S-CDM
test system were to be built today for the purpose of correlating with
R-CDM, the new system would need to include and achieve the following:
- Eliminate or significantly reduce the discharging of tester parasitic
capacitive elements while the DUT is discharged.
- Give the DUT a known
ground-capacitance value by replicating the R-CDM ground-plane capacitance
effects.
- Generate discharge-current waveforms with similar time-amplitude
characteristics observed in the R-CDM test systems.
- Measure the discharge
current through a low-inductance resistor (identical to the method used
in the ns-CDM test method).6
- Establish correlation between
S-CDM and R-CDM testers, to accelerate industry acceptance.
Can a second-generation S-CDM test system that can meet these requirements
be built? This is the current challenge for ESD test-equipment manufacturers.
To date, the IC manufacturing community is waiting for someone to design
and build a better S-CDM test system. Meanwhile, the ESDA Working Group
5.3.2 is developing a standard-practice document scheduled for release
in early 2002. This document will recommend general test procedures to
use with current SDM test systems to obtain meaningful information.
Acknowledgments
The authors would like to thank Natarajan Mahadeva Iyer, Marti Farris,
Michael Brandt, and Mike Hopkins for their constructive critique of this
article. Their comments and suggestions were much appreciated.
References
1.RG Renninger et al.,"A Field Induced Charged-Device Model Simulator,"
in Proceedings of the EOS/ESD Symposium (New Orleans, LA: ESD Association,
1989): 5971.
2.JE Vinson and JJ Liou, "Electrostatic Discharge in Semiconductor Devices:
An Overview," in Proceedings of the IEEE International Symposium on
EMC 86, no. 2 (New York: IEEE EMC Society, 1998): 399418.
3.TS Speakman, "A Model for Failure of Bipolar Silicon Integrated Circuits
Subjected to Electro-Static Discharge," in Proceedings of the IEEE
IRPS Symposium 12 (Las Vegas, NV: International Reliability Physics
Symposium, 1974): 6069.
4.PR Bossard, RG Chemelli, and BA Unger, "ESD Damage from Triboelectrically
Charged IC Pins," in Proceedings of the EOS/ESD Symposium (San
Diego, CA: ESD Association, 1980): 1722.
5.L Avery, "Charged Device Model Testing; Trying to Duplicate Reality,"
in Proceedings of the EOS/ESD Symposium (Orlando, FL: ESD Association,
1987): 8892.
6.EOS/ESD-CDM-WIP5.3-1994, "ESD Association Work In Progress for Electrostatic
Discharge (ESD) Sensitivity TestingCharged-Device Model (CDM)Component
Level," ESD Association, Rome, NY.
7.H Gieser and P Egger, "Influence of Tester Parasitics on 'Charged-Device
Model'Failure Thresholds," in Proceedings of the EOS/ESD Symposium
(Las Vegas, NV: ESD Association, 1994): 6984.
8.LG Henry, "Failure Thresholds and Failure Signatures for the Same
Device in Different Packages Using Socketed and Non-socketed CDM Simulators,"
WG 5.0 Report (Rome, NY: ESD Association, 1995).
9.T Brodbeck et al., "Reproducibility of Field Failures by ESD ModelsComparison
of HBM, Socketed CDM and Non-Socketed CDM," Microelectronics Reliability
36, no. 11/12 (Oxford, UK: Elsevier Science, 1996): 17191722.
10.K Verhaege et al., "Influence of Tester, Test Method, and Device
Type on CDM ESD Testing," in Proceedings of the EOS/ESD Symposium
(Las Vegas, NV: ESD Association, 1994): 4962.
11.K Verhaege et al., "NMOS Transistor Behavior under CDM Stress Conditions
and Relation to Other Models," in Proceedings of the Sixth ESREF Conference
(Bordeaux, France: European Symposium on Reliability of Electron Devices,
Failure Physics, and Analysis, 1995): 117124.
12.M Chaine, CT Liong, and HF San, "A Correlation Study Between Different
Types of CDM Testers and 'Real' Manufacturing In-Line Leakage Failures,"
in Proceedings of the EOS/ESD Symposium (Las Vegas, NV: ESD Association,
1994): 6368.
13.A Olney, "A Combined Socketed and Non-Socketed CDM Test Approach
for Eliminating Real-World CDM Failures," in Proceedings of the EOS/ESD
Symposium (Orlando, FL: ESD Association, 1996): 6275.
14.H Gossner and T Brodbeck, "Dangerous Parasitics of Socketed CDM ESD
Testers," Microelectronics Reliability 37, no. 10/11 (Oxford, UK:
Elsevier Science, 1997): 14651468.
15.M Chaine et al., "Investigation into Socketed CDM (SDM) Tester Parasitics,"
in Proceedings of the EOS/ESD Symposium (Reno, NV: ESD Association,
1998): 301310.
16.ESD Association WG5.3.2, "Socket Device Model (SDM) Tester," ESD
TR 08-00 (Rome, NY: ESD Association, 2000): 122.
Michael Chaine is a fellow technical member of Micron Technology
(Boise, ID). He can reached at mchaine@micron.com.
Jon Barth is the founder and chief engineer of Barth Electronics (Boulder
City, NV) and has been a technical consultant to ESD Standards Committees.
He can be reached at jonbarth@ieee.org.
Tilo Brodbeck, PhD, is a technical consultant at the central laboratory
for ESD and latch-up device testing at Infineon Technologies (Munich,
Germany). He can be reached at tilo.brodbeck@infineon.com.
Leo G. Henry, MSc, MS, PhD, is an ESD consultant for Ion (Berkeley, CA).
He can be reached at lghenry@ion.com.
Mark A. Kelly is a senior project engineer for Delphi Delco Electronics
Systems (Kokomo, IN). He can be reached at mark.a.kelly@delphiauto.com.
Tom Meuse is the component reliability product line manager for Thermo
KeyTek (Lowell, MA). He can be reached at tmeuse@thermokeytek.com.
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