| |
 |
| |
 |
 |
 |
SOI Wafer Technology
for CMOS ICs
Robert
Simonton
President, Simonton Associates
Download the .pdf File
of this Article
SOI (Silicon On Insulator) wafers have been used
commercially as starting substrates for several decades in selected
discrete and integrated circuit (IC) semiconductor device applications,
particularly for use in extreme operating environments for military
and space applications. The first SOI devices were developed for
early satellite and space exploration systems in the 1960s. The
key advantage of SOI wafers in these traditional applications was
their resistance to ionization by radiation (e.g., solar wind radiation
in space) and the robust voltage isolation of the IC.
Most of the early SOI devices were fabricated with SOS (Silicon-On-Sapphire)
wafers. The unique feature of today's SOI wafers is that they have
a buried silicon oxide (Buried OXide, or BOX) layer extending across
the entire wafer, just below a surface layer of device-quality single-crystal
silicon. The active elements (e.g., transistors in a CMOS IC) of
semiconductor devices are fabricated in the single-crystal silicon
surface layer over the BOX. The BOX layer provides robust vertical
isolation from the substrate. Standard LOCOS (LOCal Oxidation of
Silicon) or STI (Shallow Trench Isolation) processes are employed
to provide lateral isolation from adjacent devices.
At the present time, most SOI wafers are fabricated by use of one
of two basic approaches. SOI wafers may be fabricated with the SIMOXTM (Separation by IMplanted OXygen) process, which employs high dose
ion implantation of oxygen and high temperature annealing to form
the BOX layer in a bulk wafer [1,2,3]. Alternately, SOI wafers can
be fabricated by bonding a device quality silicon wafer to another
silicon wafer (the "handle" wafer) that has an oxide layer
on its surface. The pair is then split apart, using a process that
leaves a thin (relative to the thickness of the starting wafer),
device-quality layer of single-crystal silicon on top of the oxide
layer (which has now become the BOX) on the handle wafer. This is
called the "layer transfer" technique, because it transfers
a thin layer of device-quality silicon onto an oxide layer that
was thermally grown on a handle wafer. The "layer transfer"
approach has lead to the development of at least three production
methods for fabrication of SOI wafers; SmartCutTM (UNIBOND)
SOI wafers, NanoCleaveTM SOI wafers, and ELTRANTM
SOI wafers [see reference 1 for description of these methods]. The
SmartCutTM and NanoCleaveTM processes both
employ high dose ion implantation (using hydrogen or other light
species), either alone or in combination with other steps, to form
a weakened silicon layer that splits (i.e., "peels off")
the donor wafer, allowing the "layer transfer" to occur.
The ELTRANTM method (Epitaxial Layer TRANsfer) does not
use ion implantation. It employs a layer of porous silicon, which
is formed by anodic etching and annealing, to form the splitting
layer.
Recently, there is strong interest in SOI wafers for application
to the fabrication of advanced CMOS ICs. This is because SOI wafers
provide a way to increase the speed performance of CMOS circuits,
as well as reduce the power (and voltage) requirements to achieve
high performance. The trade-off between performance and power dissipation
is the most fundamentally challenging issue on the horizon for scaling
of CMOS ICs. This issue threatens the roadmap of continuous scaling
of CMOS devices. A solution must be found to insure the commercial
dominance of CMOS ICs in the future, so it is little wonder that
SOI, which offers solutions to this issue, is receiving serious
attention at leading-edge companies developing advanced CMOS ICs.
Compared to similar circuits fabricated on bulk silicon wafers,
CMOS circuits fabricated on SOI wafers can run at 20-35% higher
switching speeds than bulk CMOS, or 2 to 4 times lower power requirements
when operating at the same speed as bulk CMOS [1,4]. These improvements
in CMOS speed and power usage with SOI wafers are equivalent to
1-2 generations of scaling of CMOS devices on bulk silicon wafers
SOI Advantages:
The SOI wafer structure has several important advantages
over CZ bulk or epitaxial starting wafer architectures. SOI wafers
potentially offer "perfect" transistor isolation (lower
leakage), tighter transistor packing density (higher transistor
count/higher IC function at the same lithographic resolution), reduced
parasitic drain capacitance (faster circuit performance and lower
power consumption), and simplified processing relative to bulk or
epitaxial silicon wafers. Due to these advantages, SOI wafers appear
ideal for leading edge integrated circuits with high speed, high
transistor count, low voltage/low power operation, and battery operated
systems requirements, such as portable logic or microprocessor ICs.
Silicon-on-insulator (SOI) wafers have traditionally been used for
extreme environmental applications, such as high temperature and
severe environments (e.g., outer space). However, they are expected
to expand into mainstream CMOS applications due to these advantages:
|
| |
| |
|
|
|
| |
-
More functions per die area or reduced die
area per function; SOI allows tighter layout design rules (higher
integration density), mainly due to reduced STI layout area
required for lateral junction isolation (resulting from the
absence of wells and the possibility of direct contact of the
source-drain diodes in the NMOS and PMOS transistors) [4,5]
|
| |
| |
| As noted above, SOI wafers
offer the potential to simplify the process presently used for CMOS
devices fabricated in bulk wafers. The process used for deep sub-micron
CMOS on bulk wafers may be described in the following (highly simplified)
way:
|
| 1)
Formation of shallow trench isolation (STI) regions, which surround
and define the active areas where transistors will be fabricated
2) Formation of deep n-type
and p-type wells in the active areas, using high energy ion implantation;
these wells are vertically "profiled" using multiple ion implantation
steps to achieve:
|
2a) A deep
doping peak (the "deep well"), which suppresses latch-up, reduces
soft errors (caused by charge pairs generated from radiation effects),
and which provides part of the ESD protection path NOTE: if a
deeper "triple well" (which is typically a deep n-well structure
beneath and around a shallower p-well) is used for voltage isolation
from substrate, it is formed just prior to formation of these
n-type and p-type "twin wells"
2b) A shallower doping peak
(the "field channel stop"), located just below the STI
trench bottom, which suppresses lateral leakage between adjacent
transistors within the wells (intra-well) and between adjacent
transistors at the well boundaries (inter-well)
2c) A very shallow doping
peak at the silicon surface (the "Vt adjust"), which
sets the threshold voltage of the transistors
|
| 3)
Formation of the gate stack, including the gate oxide
insulator and the polysilicon gate on top of it (the polysilicon
gate is highly doped, n-type for the n-channel transistors and p-type
for the p-channel transistor); the gate electrode is subsequently
defined by lithography and anisotropic etching.
4) Formation of the transistor
body and contacts, including:
|
4a) Formation
of source-drain extensions using ultra-low energy ion implantation
(which is self-aligned to the gate electrode) and rapid thermal
annealing (RTA)
4b) Formation of halo (punch-through
stop) regions by self-aligned, high tilt implantation (and RTA)
4c) Following the formation
of a sidewall spacer on the gate, formation of source-drain contact
regions by high dose, low energy implantation (and RTA)
4d) Formation of salicide
(Self-Aligned siLICIDE) contact metal on the top of the gate and
source-drain regions
|
| The opportunity
for fabrication process simplification mainly occurs in step 2 (specifically
2a and 2b), above. The use of SOI wafers eliminates the need for
the high-energy ion implantation processes that form the deep n-type
and p-type "twin" wells (step 2a) and field channel stop
isolation regions (step 2b), which are presently required in leading
edge bulk CMOS IC fabrication. Also, the formation of deep "triple
well" structures using high energy ion implantation processes
(see note in step 2a, above) is unnecessary with SOI wafers to achieve
voltage (electrical) isolation from the substrate. Note that the
ion implantation and RTA processes for the formation of transistors,
e.g., extension and contact source/drain formation (steps 4a and
4c), polysilicon gate doping (in step 3), and threshold voltage
adjustment (step 2c) are still required with SOI wafers. However,
it should be noted that ultra-shallow junction formation processes
(steps 4a and 4c, above) could be less challenging in SOI wafers.
In SOI wafers the ultra-shallow junction formation process may be
designed so that the junction depth is determined by the silicon
layer thickness, rather than the ion implantation and RTA processes.
This results in a simplified process control challenge (e.g., it
eliminates the impact of "transient enhanced diffusion"
on final junction depth). Also, the requirement for the high tilt
halo (punch through stop) ion implantation (step 4b) may be eliminated
in "fully depleted" (FD) CMOS in SOI. [FD SOI CMOS will
be defined later in this article.]
SOI Applications:
The application of SOI wafers to semiconductor devices
may be segmented into three categories according to the thickness
of the buried oxide (BOX) layer: thick, thin, and ultra-thin BOX
layer wafers. The thin and ultra-thin BOX segments represent the
highest growth potential segments for SOI wafers, because they can
be used as starting wafers for CMOS IC fabrication. The table below
summarizes the SOI wafer classification, the IC applications, and
the key performance requirement. Note that the thickness boundaries
delineating the thick, thin, and ultra-thin BOX classifications
are somewhat arbitrary and not rigorously defined. Consequently,
the values selected to delineate the thick, thin, and ultra-thin
BOX categories will vary somewhat between different sources and
will, to some degree, depend upon the perspective of the author.
The thickness of the device-quality, single-crystal silicon surface
layer is also an important factor in the classification of SOI for
applications. "Thick" SOI wafers, with silicon layers
thicker than one micron (1000nm), are typically used for a wide
variety of applications in power switching devices, high-speed bipolar
circuits, and MEMS (Micro-Electro-Mechanical Systems)[1]. At the
moment, most commercial CMOS ICs are fabricated on SOI wafers with
"thin" silicon surface layers (100-300nm), mainly using
SIMOXTM or SmartCutTM SOI wafers, although
ELTRANTM SOI wafers are also being evaluated and qualified
for use with commercial CMOS ICs. The trend in CMOS applications
is clearly to thinner and thinner silicon surface layers. It is
expected that commercial SOI CMOS fabrication will move from "thin"
to "ultra-thin" silicon layers (30-100nm) in the near
future (1-3 years) to support 0.1 micron CMOS fabrication. Furthermore,
active industrial R&D is under way now at advanced IC companies
on CMOS fabricated in "ultra-thin" silicon layers of 10-30nm,
and there is conceptual and academic research activity on "nano-SOI"
using layers less than 10nm.
SOI Wafer Classification, IC
Applications, and Key Performance Requirements
|
SOI Wafer Classification
(BOX) |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
| |
|
|
|
|
|
SOI
Challenges and Issues:
The main barrier to the widespread adoption of SOI
wafers for mainstream CMOS fabrication in the past has been the
uncertain material quality and the higher cost of SOI wafers. However,
these wafers are now demonstrating technical (materials quality)
and economic (cost) readiness for use in mainstream CMOS IC production.
The key materials quality issues are the continuity and thickness
uniformity of the BOX and the defectivity and thickness uniformity
of the device-quality, single-crystal silicon layer. Important BOX
defects include voids and inclusions; the defects in the silicon
top layer include threading dislocations and pits (COPs). Also,
the interface charge trapped at the interface of the top silicon
layer and the BOX must be kept small (less than ~1011/cm2).
[The amount of charge at the BOX/silicon layer interface affects
the electrical behavior of SOI CMOS transistors, e.g., threshold
voltage and saturation current.] The suppliers of SOI wafers continue
to aggressively improve materials quality and reduce cost, driven
by the considerable economic motivation of a rapidly growing commercial
market for SOI wafers and a clearly defined roadmap for SOI material
quality on the ITRS Roadmap [8]. In this fast developing arena,
reports of SOI materials quality measurements that are only a year
old may be out of date.
Assuming that the issues of materials quality and cost will be adequately
addressed, the adoption of SOI wafers for CMOS fabrication is a
non-trivial task. Fabricating CMOS devices in SOI presents challenges
in device design and process integration, as well as in the process
simulation, device simulation and circuit simulation TCAD tools.
For example, dopant diffusion in the thin silicon layer over the
BOX is dramatically altered in SOI by interaction of the diffusing
dopants with the silicon/BOX interface (at the top of the BOX) [1].
This and other differences must be comprehended in process simulations
and in process integration for IC fabrication. Adopting SOI wafers
is not a simple transfer of a bulk CMOS device fabrication process
into an SOI substrate.
There are also significant differences between the way a bulk or
epitaxial silicon CMOS device and an SOI CMOS device behave electrically.
For example, "short channel effects" (SCE) are typically
suppressed more effectively in SOI CMOS devices than in bulk CMOS,
and SOI CMOS devices typically have lower subthreshold leakage ("off
current") and higher saturation current ("on current")
than bulk CMOS counterparts [5]. Consequently, the SOI CMOS circuits
typically demonstrate higher speed performance and lower power dissipation
than bulk or epitaxial CMOS. Also, the SOI CMOS device exhibits
several parasitic phenomena that are not typically observed in the
bulk or epitaxial CMOS device [5,6]. These phenomena are related
to impact ionization in the high electric field that occurs near
the drain in CMOS devices, and the fact that the channel terminal
in the SOI CMOS device is isolated from the substrate, unless specific
measures, such as body ties [6], are explicitly employed. In other
words, the body of the SOI device is "floating". There
are several anomalous electrical behaviors in SOI CMOS devices that
arise from these "floating body effects" (such as a "kink"
in the output I-V characteristic of the SOI CMOS device and degraded
drain breakdown voltage). Note that floating body effects are not
necessarily all bad, as they may be employed to increase the current
output from an SOI CMOS device [6]. The point is that the SOI CMOS
transistor is different than the bulk CMOS transistor and these
differences must be reflected in the simulators employed to design
devices and circuits for CMOS ICs fabricated in SOI wafers.
SOI CMOS transistors also exhibit so-called self-heating effects
[5,6]. These effects arise in SOI devices because the device is
thermally insulated from the substrate by the buried oxide (BOX).
Consequently, removal of excess heat generated within the device
by device switching is not removed as efficiently in SOI devices
as it is in bulk devices. This leads to a substantial elevation
of temperature within the SOI device (50-150°C). This modifies
the output I-V characteristics of SOI devices, once sufficient power
has been dissipated within the devices. Note that this self-heating
effect only appears when power is being dissipated within the device
(that is, when the transistor is on, conducting current through
its channel). This only occurs in CMOS circuits when a logic stage
is switching state, not when it is in a stand-by state (e.g., holding
a logic high or low state).
These effects certainly will not prevent the widespread adoption
of SOI for CMOS ICs, but they must be taken into account by thoughtful
device and circuit design approaches that specifically address the
peculiarities of the SOI CMOS transistor vs. the bulk or epitaxial
wafer CMOS transistor. Obviously, the process simulation, device
simulation, circuit simulation, and layout TCAD tools employed by
designers must accurately model the peculiarities (and advantages)
of SOI CMOS to achieve optimal device design, circuit design, layout
and processing approaches for CMOS ICs fabricated with SOI wafers.
CMOS transistors designed for use with SOI wafers are classified
by the thickness of the device-quality single-crystal silicon layer
(at the surface above the BOX) relative to the depths of the source-drain
junction and channel depletion layers in the device with the operating
voltages applied. An SOI CMOS transistor is classified as "partially
depleted" (PD) if the silicon surface layer is thicker than
the depth of the depletion region in the transistor's channel. The
SOI CMOS transistor is classified as "fully depleted"
(FD) if the silicon surface layer is equal to the depth of the depletion
region in the transistor's channel. The transistor will be partially
depleted or fully depleted depending on the silicon layer thickness
above the BOX and the doping concentration in the channel. To form
a fully depleted SOI transistor, the channel doping concentration
must be low enough that the gate depletion region extends throughout
the entire thickness of the silicon layer. When the silicon surface
layer is thicker than about 200nm, the transistor will typically
be partially depleted, unless the channel doping concentration is
reduced to such low values that the threshold voltage is too low
for practical CMOS applications (less than 100mV) [5]. If the silicon
layer thickness is reduced to about 100nm, the transistor will be
fully depleted, even when the channel doping concentration is increased
to produce threshold voltages of 300-400mV. If the silicon layer
thickness is reduced further (70nm), the transistor will remain
fully depleted even if the channel doping concentration is increased
to produce even higher threshold voltages (700mV).
There are significant differences in partially depleted and fully
depleted SOI CMOS transistors [5]. For example, the threshold voltage
of the fully depleted (FD) device is very sensitive to the silicon
surface film thickness. This results in an addition source of manufacturing
variance in the fabrication of FD SOI CMOS. Typically, this is on
the order of 10mV in threshold voltage per nanometer of variation
in the silicon film over the BOX. This is the main reason why, at
the present time, the fabrication of commercial CMOS on SOI typically
employs partially depleted (PD) devices. However, careful device
design and optimizing the channel implant process can reduce this
sensitivity in FD devices. It is also important to note that the
variation of drain (saturation) current does not have the same sensitivity
to film thickness as the threshold voltage in FD SOI CMOS [5].
There are significant advantages for FD transistors over PD transistors,
and the trend in SOI CMOS is toward the use of fully depleted devices.
A fundamentally important point is that in FD SOI CMOS the subthreshold
slope can be very low (less than ~65 mV/decade (i.e., a 65 mV increase
in gate voltage will result in a tenfold increase in the subthreshold
drain current). This is significantly closer to the theoretical
minimum (~60 mV/decade) than the typical values of 80-85 mV/decade
in PD SOI CMOS and 85-90 mV/decade (best case) in bulk CMOS. This
is a critical advantage. It allows the threshold voltage of the
FD SOI CMOS device to be very low (150-200mV) with acceptable subthreshold
leakage ("off current"), which determines off-state power
dissipation. Lowering the threshold voltage also means that the
supply voltage can be reduced significantly without degrading CMOS
IC speed performance (the supply voltage needs to be 4-5 times the
threshold voltage; below this ratio, the speed performance of the
circuit will degrade rapidly). The reduction of the supply voltage
produces a significant reduction in active (switching) power dissipation,
without unacceptable performance degradation. [Note: the active
power dissipation is also reduced somewhat by reduction of parasitic
capacitance in SOI CMOS relative to bulk CMOS.] Also, in the FD
CMOS device the variation of threshold voltage with temperature
is significantly less (2-3 times less) than in the PD CMOS device.
Furthermore, in general, the anomalous electrical behaviors arising
from floating body effects in SOI CMOS transistors are less of a
problem in FD transistors than they are in PD transistors. Consequently,
it is expected that FD SOI CMOS transistors will be generally adopted
in the near future [1]. Converting an existing PD SOI CMOS device
and circuit design into FD CMOS is expected to be straightforward
[6], at least in comparison with to the challenges in the conversion
from bulk CMOS to SOI CMOS.
SOI Prospects:
SOI wafers are now viewed as the most important
emerging wafer engineering technology for use in leading edge CMOS
IC production during the next 3-5 years. One plausible scenario
during this period is the rapid adoption of SOI wafers in place
of epitaxial silicon wafers now employed as starting substrates
for high-end logic device (e.g., microprocessors) and SOC (System
On Chip) applications at the 0.13 and 0.10 micron technology nodes.
SOI wafers appear to offer an excellent platform for integrating
RF and digital circuits on the same chip.
Major semiconductor market research firms have forecasted the possibility
that SOI wafers may make up 10% of all silicon wafers used by 2010.
Almost all of the "top 20" chipmakers have publicly expressed
high interest in the inherent advantages of SOI wafers (e.g., IBM,
Intel, AMD, etc.). A bright spotlight was cast on SOI wafer technology
production in August 1998 due to an IBM announcement that they would
adopt SOI wafer technology using the SIMOX SOI wafer process in
high volume manufacturing on leading edge microprocessor architecture.
It is in production now, using a partially depleted transistor architecture
[4]. Furthermore, Intel has recently unveiled their vision of the
CMOS device they will pursue in the future, to achieve continuous
scaling of CMOS with high performance and acceptable power (and
voltage) requirements. This is the Intel "TeraHertz Transistor",
which employs the use of a fully depleted (FD) CMOS transistor on
thin SOI wafers [7], among other design changes (such as a high-K
gate dielectric and raised source-drain regions).
One of the more compelling reasons why support for migration from
bulk to SOI CMOS is growing is due to the problems created by the
exponential growth of the power dissipated by high performance,
high density CMOS ICs in bulk (or epitaxial) silicon as scaling
has been pursued [7]. For example, as Intel microprocessors have
evolved by scaling through the 286, 386, and 486 generations into
and through the Pentium generations, power dissipation has dramatically
(exponentially) increased. The 286 generation ran warm (to the touch
by your fingers), the 386 ran very hot, and the 486 ran so hot that
it needed a small fan to cool it. As evolution proceeded through
the Pentium generations, the cooling requirement was more demanding
at each generation, using more powerful fans and adding cooling
fins to the microprocessor package to improve heat transfer out
of the IC. Assuming that the Intel microprocessor stays on its historical
trend lines (Moore's Law), then by about 2005 these ICs will have
about 1 billion transistors and operate at about 10 GigaHertz [7].
They will also dissipate so much power that they would require cooling
by refrigeration of a liquid coolant in good thermal contact with
the IC package. This is unacceptable as a computer systems requirement,
and it illustrates that power dissipation is becoming a major barrier
to scaling high performance, high density CMOS in the very near
future. SOI CMOS offers a way to avoid this barrier without sacrificing
high performance or high density.
SOI devices also appear to offer a sustainable, long-term pathway
beyond the multiple barriers to scaling planar, bulk CMOS to 50nm
and below [1]. If the present understanding of the barriers and
problems to scaling planar, bulk CMOS below 50nm is correct, then
it is expected that a dramatic shift to fully-depleted SOI CMOS
will occur in the 2006-2008 timeframe. If the many challenges in
the fabrication of "ultra-thin" SOI wafers are met (adequate
materials quality and acceptable cost), and if device design and
lithography challenges are met, the way to 25nm CMOS is open, enabled
in part by SOI substrates.
SOI wafers will have a very significant impact on both the IC fabrication
process and process equipment. For example, SOI wafers create a
requirement for new types of ion implantation process equipment.
Most SOI wafers are fabricated using an ion implantation step employing
a high dose of oxygen (Ibis' SIMOXTM SOI wafer process)
or hydrogen (SOITEC's SmartCutTM SOI wafer process).
These process requirements create a requirement for two new types
of specialized ion implantation machines: a high dose oxygen implanter,
and a high dose hydrogen implanter.
© 2002 Simonton Associates
NOTE: Robert Simonton is developing a new course on SOI that
will describe these topics in far more technical detail than is
provided here in this special report. Keep an eye on this website
for more information on the content and availability of this new
course.
References:
[1] D. K. Sadana and M. Current, "Fabrication
of Silicon-On-Insulator (SOI) Wafers Using Ion Implantation",
in Ion Implantation Science and Technology, Edited by J. F. Ziegler,
Ion Implantation Technology Co., 2000, p. 341-374. (NOTE:
This book may be purchased at www.latticepress.com)
[2] J.P. Colinge, "Silicon-On-Insulator Technology: Materials
to VLSI, Second Edition", Kluwer Academic Publishers, 1997,
Chapter 2, pgs. 32-44. (NOTE: This book may be purchased
at www.latticepress.com)
[3] Ibis Technology Corporation, Danvers, MA, USA, www.ibis.com
[4] www.chips.ibm.com/bluelogic
[5] J.P. Colinge, "Silicon-On-Insulator Technology: Materials
to VLSI, Second Edition", Kluwer Academic Publishers, 1997,
Chapters 4 & 5.
www.soisolutions.com/design.html
[6] A. Marshall and S. Natarajan, "SOI Design: Analog, Memory,
and Digital Techniques", Kluwer Academic Publishers, 2002.
[7] www.intel.com/research/silicon
[8] http://public.itrs.net/files/2001itrs/home.htm
|
back
to top |
| |
|
 |