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By Richard Stallcup II, PhD, Zyvex Instruments
Download a printable copy here.
Introduction
Probing integrated circuits (IC) with sharp metal contact
wires under an optical microscope has been, for many years,
the primary means of characterizing an IC’s electrical
performance. Since advances in IC technology follow Moore’s
Law of decreasing scale, the complexity of producing and testing
the more advanced IC’s has increased. More powerful
microscopes and highly precise probe placement is needed in
order to test these next-generation ICs.
Scanning electron microscopes (SEMs) and focused ion beam
(FIBs) systems are widely employed to image and measure the
results of different IC fabrication steps. SEMs and FIBs are
ubiquitous to most fabs and are workhorse instruments for
metrology and failure analysis. The Zyvex KZ100 prober, which
is compatible with both system platforms, greatly enhances
the utility of these common tools by enabling IC electrical
performance measurements at the nano scale.
Extrapolating data from test devices in the scribe line (street)
is a common method of testing. However, scribe line devices
are known to behave differently than devices in the real application.
Alternatively, test modules can be designed and placed on-chip,
but this technique requires valuable real estate. Probing
in die transistors, that are actual devices, at the contact
level has proven to be an invaluable technique. With data
collected from individual on-chip transistors using the KZ100,
IC design engineers can feed actual device data into design
models to improve modeling accuracy.
The Zyvex KZ100 Nanomanipulator/Prober is comprised of a
Zyvex Nanomanipulator (Figure 1A), controller
(Figure 1B) and a Keithley 4200 Semiconductor
Characterization System (Figure 1C). The
KZ100 is capable of landing four sharp probes easily within
a 200 x 200 nm area with less than 5 nm precision. The size
of the minimum landing area is dependent on the sharpness
of the probes. With FIB sharpened probes, the minimum landing
area could be much smaller than that stated above. The KZ100’s
range of motion and precision makes the KZ100 ideal for probing
ICs that are fabricated with 90 nm node technology. As IC
technology advances and the scale decreases, to 60 and then
to 45 nm, the KZ100 is also well-positioned to probe next
generation ICs.
(a)

(b)

(c)

Figure 1
(a) KZ100 head unit with end-effectors installed.
(b) Zyvex KZ100 Controller.
(c) Keithley 4200 Semiconductor Characterization System.
An SEM/FIB is typically optimized for low mechanical and
electrical noise, which is necessary to achieve sub-nanometer
resolution images. Ambient conditions which commonly affect
AFM systems, such as thermal fluctuations and air drafts,
are thus eliminated by the controlled environment of the SEM
or FIB.
Systems that rely on atomic force microscopy (AFM) techniques
in air can require extensive and expensive facilities upgrades.
Requirements can typically include a mechanically quiet room,
stabilized air flow conditions, and air temperature stability
that can exceed many standard clean room HVAC specifications.
In addition, AFM scanning speeds are slow and fields of view
are very limited resulting in very long and tedious exercises
to locate a small specific region of interest. SEMs and FIB’s
offer the user the ability to image large areas quickly to
find a region, and then magnify specific portions to highlight
particular areas. The KZ100 system benefits from utilizing
the optimized vacuum chamber environment where high-resolution
images of the IC test site can be generated with low electrical
and mechanical noise, probe placement can be directed without
ambient interferences, and external influences on probe drift
are minimized.
Application
The KZ100 can be outfitted with as many as four probes which
are independently and linearly operated in X, Y, and Z with
less than 5 nm precision. For the purposes of this paper,
the KZ100 was installed in a high-resolution SEM for precise
imaging and probe placement similar to the arrangement shown
in Figure 2. Tungsten probes with a 45-degree
bend were prepared using a proprietary Zyvex process and installed
in the four positioners. The 90 nm node IC test chip was deprocessed
to the contact level and etched for five seconds in 20 parts
H2O to 1 part 49% HF. The IC chip was mounted to
the grounded center rotational stage of the KZ100.

Figure 2: KZ100 Manipulator in an FIB at
52 degree tilt. The sample being probed on the center stage
is a deprocessed integrated circuit chip.
After SEM pump down and the microscope image parameters were
determined, the IC test area was located and the probes were
positioned above the test area. The probes were moved towards
the IC surface and probe-to-surface contact was established.
Once the probes were in contact with the IC, the probes were
lifted just above the surface and then moved parallel to the
surface until each probe was relocated above its intended
circuit contact. While the probe was re-lowered to the circuit
contact, the probe was swept back and forth to determine contact
and its location. Once the probe made contact, the probe’s
sweeping motion became a pivoting motion with the pivot point
at the location where the probe touched the IC surface. The
probe was then positioned so that the pivot point was coincident
with the IC device contact. Figure 3 shows
four probes in electrical contact with the drain, source,
gate and P substrate contacts of an n-channel MOSFET device.

Figure 3: Four probe contact on an n-channel
MOSFET. The Gate probe is connected to the pass-gate shared
by four n-channel transistors. The Psub is connected to the
substrate contact and the S/D probes are connected to the
source and drain of the transistor being tested. The KZ100
is capable of connecting to contacts that are separated by
as little as 70 nm and as large as 10 millimeters.
A Keithley 4200 Semiconductor Characterization System was
used for biasing the probes and collecting the IC device drain
current vs. drain source voltage (IDVDS)
data. The system was equipped with four 4200-SMUs (source
measurement unit) and triaxial cabling. The IDVDS
curves were acquired with the mode set to “sweeping”
and the speed setting of “fast.” The current compliance
for the source and drain current IS and ID
respectively was set to 500 µA and the voltage VDS
was swept with steps of 5 mV from 0.0 V to 1.5 V. A series
of IDVDS curves were measured by additionally
stepping the gate voltage VGS with limits of 1.5
V and 100 nA. Before and during data acquisition, the microscope’s
scanning beam was blanked to minimize any charge-induced influence.
Results and Discussion
MOSFETs behave like transconductance devices over most of
their operational range where ID is nearly constant
for a given VGS. This operational range is commonly
referred to as the “saturation region.” At small
drain source voltage VDS, MOSFET devices behave
like a resistor where the drain current ID is linearly
proportional to VDS and this region is commonly
referred to as the “linear region.”
The IDVDS data, shown in Figure
4, collected from a 90 nm node n-channel MOSFET device
using the KZ100 system has both the linear and saturation
regions of a typical MOSFET. Figure 4a shows
the drain current with forward bias and Figure 4b
shows the same IC’s drain current with reverse bias.
This comparison is one way to determine if the device is functioning
properly. The IDVDS curves of 4a
and 4b are very similar which this shows
that the current device under investigation is functioning
as expected.
(a)

(b)

Figure 4:
(a) The IDVDS curves of an integrated
n-channel MOSFET generated by a Zyvex KZ100 Nanomanipulator
System.
(b) The reverse bias of the device under test of Figure 4a.
With p-channel MOSFETs, the current ID flows when the gate
voltage VGS is negative with respect to the source
voltage VDS. Typically, p-channel MOSFETs have
a higher gate threshold voltage and lower saturation current.
Figure 5 shows a family of IDVDS
curves of a 90 nm node p-channel MOSFET device. These p-channel
curves, collected using the KZ100, show the expected lower
performance of a p-channel MOSFET in comparison with the n-channel
MOSFET.

Figure 5:
The IDVDS curves of an integrated p-type
MOSFET generated by a Zyvex KZ100.
Conclusion
Electrical characterization of integrated circuits is an
integral component of the fabrication and design loop. As
high magnification scanning particle beam microscopes are
needed to keep up with the decreasing scale of IC technology,
electrical characterization using probing systems that are
designed and optimized for operation in these microscopes
is needed. The Zyvex KZ100 System is designed and optimized
for characterizing current and next-generation IC device properties
which require very precise probe placements, accurate current
and voltage measurements, and high magnification inside a
high resolution SEM or FIB system. With this system IC designers
and failure analysis engineers are better equipped to tackle
performance and failure issues of the next generation integrated
circuits.
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