Introduction: Lithographic scaling
Lithographic scaling has historically been accomplished by
optimizing the parameters in the Rayleigh model for image resolution:
In this model, image resolution =
k /NA,
and depth of focus (DOF) =
k /NA²,
where =
exposure wavelength and NA = numerical aperture
(k ,
k
= constants for a
specific lithographic process). To pattern devices with decreasing
feature sizes, photoresist exposure wavelengths were reduced and
numerical apertures were increased.
During the last ten years, image resolution was sufficiently increased
to scale minimum dimensions from 1-µm feature sizes for the 1Mb DRAM
devices to 0.25-µm features for the 256Mb DRAM. The depth of focus is
proportional to the inverse of the square of the numerical aperture;
thus, if resolution is enhanced by increasing NA, the depth of focus
becomes very small. If the resolution is enhanced by decreasing the
wavelength, the corresponding decrease in depth of focus is less
severe. As shown in Figure 1 for
lithography at the diffraction limit, a shorter wavelength
provides more depth of focus at a particular resolution value because
the shorter wavelength allows a lower-NA photolithography tool to
achieve equivalent resolution.
Figure 1
The IBM Microelectronics Division has been active in the evolution of
lithography throughout the development of the semiconductor industry
(Figure 2). DRAM production of 64Kb devices
utilized scanning exposure equipment operating at a G-line wavelength
of 436 nm. These tools were capable of operating at several different
exposure wavelengths, including 436 nm, 313 nm, and 245 nm
[1]. IBM used these tools for
256Kb DRAM chips by formulating a resist, TNS, which was functional at the 313-nm exposure
region [2], allowing the critical feature
size to be scaled from 2
µm to 1.4 µm. This approach was repeated for 1Mb DRAM chips, and a
245-nm exposure region was used to obtain the 1-µm critical features
with the same tool set, which required the development of the first
production deep-UV (DUV) chemically amplified, negative-tone resist
[3]. At this time, G-line steppers
were introduced at a NA of 0.35,
and the process for the production of 1Mb DRAM reverted to G-line
lithography. For the 4Mb DRAM generation, stepper technology was
extended by scaling the wavelength to the I-line
( = 365
nm). High-NA (0.42-0.45) G-line steppers were used to manufacture
4Mb pilot line products at 0.8-µm ground rules, while lower-NA (0.35)
I-line steppers were used for final qualification of products with
0.6-0.7-µm critical features. For the 16Mb generation, DUV in the
245-nm exposure region was utilized for development and initial
production, while very high NA (0.5-0.6) I-line (365 nm) was used for
volume production at 0.4-0.5-µm image sizes. The 64Mb and 256Mb DRAM
generations use high-NA (0.5-0.6) DUV tools at
= 248 nm for images
at 0.25-0.35-µm resolution.
Figure 2
During this scaling process, several DUV resist materials were
developed and utilized by IBM. While I-line resists were composed
of modified G-line materials, the DUV resists operated by a different
mechanism. The DUV region of the mercury arc lamp is of relatively low
intensity compared to the I-line and G-line regions. To compensate for
low DUV exposure intensities, a chemical amplification method
[4,5]
was used to enhance the speed of the DUV resist. This catalytic
amplification process, combined with new resins that were less
absorbing at = 245 nm
than the traditional novolak
materials, introduced significantly different resist processing
requirements for DUV lithography. These unique process requirements
were characterized and included as part of the process of implementing
DUV lithography in product applications.
DUV processing for product applications
1Mb DRAM: 1985-1986
DUV resist was used at
= 245 nm
to print the first level of
the 1Mb DRAM, which was recessed oxide (Rox) isolation
[5]. This level required
the printing of a 1-µm resist spacing between features
on a 100-nm silicon nitride film. The image was transferred into the
nitride film with an RIE process. DUV was used on this level because
the initial G-line steppers were limited to a resolution of 1.2
µm, and insufficient wafer stage control was available to
establish a uniform grid at the first mask level. The scanning exposure
tools, which were commonly available in manufacturing areas at that
time, were capable of 1-µm feature resolution at DUV exposure
wavelengths (
= 240-250 nm). Since these tools were full-wafer
scanners, the first level was printed as a regular grid, with the
relative positioning of each chip predominantly established by the
reticle fabrication tool. Product overlay could be achieved within the
required tolerance by using this regular and repeatable first level as
a reference point for the alignment of subsequent mask levels.
The initial DUV resist formulation was a negative-tone material with a
new resin, solubility inhibitor, photoactive compound, and developer
solution compared to the previously utilized mid-UV resists. The resin
was a para-hydroxy-styrene polymer (PHOST) modified with a
tertiary-butoxy-carbonyl (tBOC) functionality to impart insolubility in
polar solvents and aqueous-base solutions. A sulfonium salt was used as
a photo-acid generator, and a post-exposure bake was used to cause a
catalytic cleavage of the tBOC group from the exposed resist
(Figure 3)
[4,6]. Development in
anisole of the exposed and baked resist selectively removed the
unexposed material, providing a negative-tone image.
Figure 3
This resist was very sensitive, requiring a 1-5-mJ/cm²
exposure dose, depending on the formulation and process conditions.
Contrast was high, with a
value of 8-10, and the 1-µm
resolution requirement of this product application was easily achieved.
With this system, throughput levels of 100 wafers per hour could be
achieved with existing scanning exposure equipment. However, a number
of difficulties with this system soon became apparent as product
application work progressed. While resist adhesion was acceptable on
silicon wafers, poor adhesion was obtained on the silicon nitride
product film. The hexamethyldisilazane (HMDS) adhesion priming
operation, which was effective for conventional development of resists
in aqueous solutions, was ineffective for the hydrophobic solvent used
in this DUV develop process. Thermal oxidation at the nitride surface
to form a silicon oxynitride surface improved resist adhesion
sufficiently to warrant further product development.
Metallic oxide residues were identified in the resist stripping baths
and traced to the photosensitizer materials used in the DUV resist.
These residues were reduced by specifying smaller wafer batches between
bath changes and, ultimately, by replacing the metallic components in
the resist formulation with organic materials.
Attention also focused on control of the post-exposure bake process,
because this parameter became more important for linewidth control than
exposure dose levels in the photolithography tool
(Figure 4). The catalytic chemical amplification reaction
which produced the high resist sensitivity needed for operation at the
low light intensities available in DUV was exponentially dependent on
the bake temperature used to induce the catalysis. As a result,
resist sensitivity also became exponentially dependent on the bake
temperature [7].
Figure 4
Not only was the catalytic amplification process of this resist
dependent on the bake conditions, but it could also be affected by the
presence of contaminants from chemicals in the manufacturing
environment. It was observed that freshly coated wafers, when placed in
a cassette on the photolithography tool and exposed in sequence, often
displayed a continuous shift in linewidth from wafer to wafer across
the cassette. The resist steadily became one to three times less
sensitive as the delay time from application of resist to its exposure
increased. After two to three hours, the resist stabilized at a
lower sensitivity value (Figure 5)
This behavior was caused by the absorption of chemical bases, such as
N-methylpyrolidone (NMP), into the resist at part-per-billion
levels, which interrupted the catalytic image formation process
[8] and
caused a large change in resist sensitivity. Initially,
wafers were deliberately allowed to stand in the manufacturing
environment and absorb the chemical contaminants. The resist
sensitivity became relatively stable and then could be processed with
acceptable linewidth control after the contaminants were absorbed.
Because of variations in the manufacturing environment, however,
significant shifts in resist sensitivity were observed for each
subsequent batch of product wafers. This required "send-ahead"
wafers to control image size for each lot, thereby significantly
reducing throughput from the DUV sector (Figure 6)
Figure 5
Figure 6
While these difficulties rendered the process cumbersome, the
development cycle of the 1Mb DRAM proceeded on schedule, and initial
product demand was supplied. Several million fully functional 1Mb DRAM
chips were produced with DUV (245-nm) technology.
In the laboratory, the negative-tone resist used on the 1Mb DRAM was
shown to act as a positive-tone material if an appropriate polar
developer was used [4].
In practice, the positive-tone image was
distorted by an insoluble film at the surface of the exposed resist
(Figure 7). After the experience with the
negative-tone resist, it was realized that this inhibition effect was
caused by chemical contamination inadvertently poisoning the resist,
and that a suitable positive-tone image could be formed if the effect
of this contamination process was reduced or eliminated. When the
resist was formulated to provide a higher dissolution rate of unexposed
resist, the surface layer of contaminated resist could be removed in
the development process, and a resist image with an acceptable profile
was obtained.
Figure 7
As work on the 1Mb DRAM production shifted to more advanced G-line
steppers (0.35 NA), the DUV effort was refocused on the 16Mb DRAM and
the development of a positive-tone material which would overcome the
limitations of this first-generation negative-tone DUV resist.
16Mb DRAM: Positive-tone DUV resist, 1987-1992
The experience gained from the 1Mb DRAM DUV development effort was
used as a foundation for 16Mb DUV applications. When the 16Mb work
began in 1987 at 500-nm resolution, conjecture centered on whether
conventional optical lithography with single-layer resist processing
would be attainable at the reduced depth-of-focus margins, or
whether bilayer and top-surface imaging resists would be required
[9].
At this time, I-line steppers were barely achieving the 0.7-µm
resolution requirements of the 4Mb DRAM. A new DUV photolithography
tool with a NA of 0.36 (discussed below in the section on
photolithography tools) was developed which was suitable for 0.5-µm
lithography. This tool was used for the 16Mb DRAM development
program.
The 16Mb DRAM had six critical mask levels with resolution requirements
of 0.5-0.6 µm and an overlay tolerance of 0.2 µm. Several of these
levels contained critical features which were small openings (0.5-0.6
µm) printed in a field of resist. A positive-tone resist was
desirable for these levels because of an enhanced focus window compared
to negative-tone imaging and reduced reticle defects. (The
positive-tone reticle was primarily a chrome area, which would mask
particulates on the reticle surface, whereas a negative-tone reticle
would have been mostly clear, allowing particles on the reticle to
print as defects.) The negative-tone resist formulation used for the
1Mb DRAM was modified to create a positive-tone resist that overcame
many of the initial DUV process control problems. The resin composition
was modified to reduce loss of mass by decreasing the concentration of
solubility inhibitor (which provided increased etch resistance and
reduced image distortion) and to reduce the resist contrast. Reduced
contrast allowed the resist to be more robust to chemical contamination
by an airborne organic base. This, in turn, allowed aqueous-base
developers to be used without adverse effects on the positive-tone
resist profile. Resist chemical amplification was reduced by using
lower post-exposure bake temperatures and adding acid-quenching
materials to the resist during formulation. While resist sensitivity
was reduced by these changes, process latitude with respect to profile
and sensitivity variations caused by unintended interruption of the
chemical amplification process was increased. The use of aqueous-base
developer allowed conventional HMDS surface treatments to be used for
the enhancement of resist adhesion, thereby avoiding problems with
lifting and cracking resist. Resin molecular weight was sharply
reduced, which enhanced depth of focus and resulted in an absence of
resist residuals after development. Nonmetallic photosensitizers were
implemented, which further reduced residuals after resist-stripping
processes. In addition, bottom antireflective coatings (ARC) and
topcoat materials were developed to provide barriers to chemical
contamination from both the wafer substrate and the processing
atmosphere. As a result, the chemical amplification process in the
resist could proceed without unintended interruption. These
enhancements provided sufficient process stability for development and
fabrication of the 16Mb critical mask levels. Since resist stability
was sufficient, exposure dose could be controlled with statistical
process control (SPC) charts rather than with send-ahead test wafers
(Figure 8)
[10]. The exposure dose was
modified only if the average image size for a lot was outside the
indicated control limits, or if seven lots in succession were above or
below a target image size. The process steps for the first-generation
positive-tone DUV resists are as follows:
- Adhesion prime or ARC apply/bake.
- Apply resist.
- Bake.
- Apply topcoat.
- Bake.
- Expose.
- Post-exposure bake.
- Develop in aqueous base.
SEM cross sections of selected features from the 16Mb DRAM
critical mask levels are shown in Figures 9 and
10.
The deep-trench storage capacitor (Figure 9)
was printed with a resist opening 0.7 µm wide
with a 0.5-µm separation between adjacent trenches. The isolation
trench contained 0.5-µm resist lines with 0.6-µm spaces in the DRAM
support structures. The surface strap, an electrical connection between
the trench capacitor and the diffusion area, was printed as an 0.8-µm
resist island with a 0.4-µm separation between adjacent straps. The
straps were printed over the gate conductor topography, which was
0.8 µm in depth. The gate conductor (Figure 10)
was a serpentine 0.6-µm line/space combination in the memory array, with
0.5-µm lines in the memory support features.
Figure 8
Figure 9
Figure 10
While the formulation changes for the 16Mb application of DUV resist
relieved many of the initial problems, a continuing concern was the
dependence of sensitivity on the post-exposure bake temperature
(Figure 11). When more than one resist bake
plate was used in a "clustered process," maintaining the
temperature matching of the plates was often difficult. In a clustered
process, the bake station is physically attached to the
photolithography tool, and it is desirable to use a sufficient number
of bake plates to match the throughput capability of the
photolithography tool. In this arrangement, different bake plates are
often used for successive wafers as they emerge from the
photolithography tool. Gradual drift in bake-plate temperature could
cause variation in wafer-to-wafer or lot-to-lot linewidth. Defects at
the resist bake step, either from particles lodged between the wafer
and the surface of the bake plate, or from failure of the
positioning pins on the hot plate, could cause linewidth variation
within a wafer. Prototype linewidth monitoring equipment was developed
to monitor the image formation on a bake plate, both as a potential
means of controlling the photolithographic-image size and as a means of
detecting excursions in the bake process
(Figure 12)
[11], but are not implemented in
manufacturing at present. The second-generation positive-tone DUV
resist materials which are currently appearing in the marketplace
provide more stability in the post-exposure bake process, as well as
stability to airborne chemical contamination [12].
Figure 11
Figure 12
Logic gate conductor: 1992-1994
During the characterization of the DUV positive-tone resist
process, systematic within-chip differences in printing were observed.
At the memory gate conductor level, in particular, isolated lines in
the support areas were consistently wider than corresponding nested
lines in a memory array. Because of the timing circuits which are
present in the gate conductor features, this systematic difference
caused yield reductions due to a loss in chip performance
(Figure 13)
[13]. For the memory product, this
linewidth deviation can be caused by both systematic etch and
photolithography causes
(Figures 14 and 15)
[13(b)]. Polymer
by-products of an etch plasma deposit more rapidly on the isolated
features than the nested features, thereby causing the isolated lines
to become wider than the nested lines[14].
The diffraction effects of the positive-tone aerial image caused the resist
to print with a
similar systematic bias, with isolated lines printing approximately 8%
larger than nested lines. For the memory product, it was possible to
optimize the reticle image size compensations to reduce this effect by
using manual image inspection and compensation procedures. For logic
applications, however, the irregular nature of the circuit pattern was
too complex for manual alteration, and the features could not be
automatically compensated with the available software technology.
Figure 13
Figure 14
Figure 15
The aerial image of negative-tone lines contains a minimal offset
between nested and isolated lines
[15].
In fact, the isolated lines print slightly
smaller than the nested lines for negative-tone resist
(Figure 15). This aids in
compensating for the etch effect, which can be modified
with etch chemistry and process, but which generally causes
isolated lines to increase in width compared to nested lines for
polysilicon etch processes (Figure 14).
A second-generation negative-tone resist was formulated to further
enhance the DUV process capability [16].
This resist was used with a 0.5-NA step-and-scan exposure tool to achieve
0.35-µm gate conductor
lithography. The mechanism of this resist is different from the initial
DUV material in that the resin is cross-linked to impart insolubility
to the exposed area. The previous resist had used a polarity change of
the resin to impart insolubility to the exposed area. This new approach
allowed a resist to be formulated which could be developed with an
aqueous base, providing the good adhesion characteristics obtainable
with such systems. Cross-linking in this resist is very efficient,
providing high-speed resist materials. As a result, chemical additives
can be used to stabilize the resist to chemical amplification poisons
without degrading the resist sensitivity or reducing wafer throughput.
This negative-tone resist does not require a topcoat for process
stability.
The cross-linking mechanism also provides a low-activation-energy
image-formation process during the post-exposure bake. This results in
a smaller variation of image size with post-exposure bake temperature,
thereby further enhancing the manufacturability of DUV processes.
Developer process latitude is also enhanced, since the image size for
negative-tone resist is considerably more stable to develop time than
for positive-tone resists.
The use of this resist, combined with enhanced etch processes and
reticle uniformity, led to improvements in across-chip linewidth
control for CMOS logic gate conductor programs. This enhanced linewidth
control provides higher performance and yield values, which are the
primary components for process manufacturing costs
(Figure 16)
[12,13].
Figure 16
While the photoresists described were largely developed at IBM, an
essential component in chip fabrication for device applications is the
exposure tool used to image the semiconductor patterns into the resist.
During this application activity, IBM interacted closely with equipment
suppliers to ensure that both the resist process and tool capabilities
were commensurate with product requirements.
Evolution of DUV photolithography tool
Prior to 1985
The first tool used for DUV manufacturing was a Perkin-Elmer
full-wafer scanner (Table 1) with a
curved-arc capillary mercury arc lamp source and reflective ring field
projection optics (Figure 17). The reticle
and wafer are mounted together on an air-bearing carriage which is
scanned to image the entire wafer in a single pass. The tool achieves
high wafer throughput in manufacturing because of the single scan per
wafer.
Figure 17
Table 1 Comparison of attributes for a progression of DUV tools.
| Equipment principle | Full wafer scanner | Step and scan | Step and repeat | Step and scan |
| Supplier | Perkin-Elmer | Perkin-Elmer/ SVG Lithography | Nikon | SVG Lithography |
| Exposure source | Mercury arc capillary lamp | Mercury-xenon arc lamp | KrF excimer laser | Mercury-xenon arc lamp |
| Lamp power (kW) | 1 | 2.4 | -- | 2.4 |
| Laser power | -- | -- | 3 W/200 Hz | -- |
| Bandwidth(nm) | 235-285 | 240-260 | 3 pm @ 248 | 244-252 |
| Uniformity (%) | ±3 | ±2 | -- | ±1 |
| Projection optics |
| Type | Reflective | Catadioptric | Refractive | Catadioptric |
| NA | 0.167 | 0.35 | 0.42 | 0.5 |
| Scanned field |
| Shape | Arc | Arc | Circle | Rectangle |
| Height (mm) | 125 | 20.3 | -- | 22 |
| Radius (mm) | 115 | 20 | -- | -- |
| Width (mm) | 4 | 1 | -- | 5 |
| Printed field | 125-mm wafer | 20 mm × 32.5 mm | 15 mm × 15 mm | 22 mm × 32.5 mm |
| Stage |
| Bearings | Air | Air | Needle | Air |
| Wafer (mm) | 125 | 200 | 200 | 200 |
| Alignment | TTL | TTL | Off-axis | TTL |
| Illumination | Dark field | Reverse dark field | Dark field | Reverse dark field |
| Distortion (nm) | ±250 (98%) (Dist & Mag) | ±70 | ±120 | ±35 |
| Overlay |
| Tool to tool (nm) | 350 (98%) | 150 (98%) | 150 (x + 3 ) | 90 (x + 3 ) |
| Ideal throughput | 100/hr | 50/hr | 24/hr | 50/hr |
The tool is adapted to DUV exposures using a filter in the
illuminator/condenser. Since the illumination source is broadband
and the reflective projection optics are corrected to less than 240 nm,
resolutions of 1 µm needed for 1Mb DRAM manufacturing could be
achieved. This scanner was used in the 1Mb DRAM application described
earlier.
The use of this tool at resolutions below 1 µm was not pursued
because astigmatism was not fully corrected in some systems, and
vertical and horizontal lines could differ by as much as 0.2 µm for a
nominal 1.0-µm feature. Also, exposure uniformity was difficult
to achieve because the DUV illumination was not centered in the
scanned slit.
1985 to 1992
As the 16Mb DRAM development program was initiated, there was a
need for resolutions of 0.5 µm, the introduction of larger product
chips, and the use of 200-mm wafers. This led IBM to acquire
a tool from Perkin-Elmer designed specifically for DUV. This was the
first tool (Table 1) based on the step-and-scan principle
[17]. In tools of this type, the wafer is
stepped to a new field, which is then
scanned; this continues until all fields have been scanned
(Figure 18).
Figure 18
Tools of the step-and-scan type are attractive for microlithography
because they are able to print large fields at high wafer throughputs.
Good resolution and low distortion can be obtained because the scanned
field is small compared to the printed field and can be well corrected
optically at higher NA values. Good linewidth control and overlay can
be obtained because focus and alignment can be adjusted during the scan
of each field to match the topography and previous level pattern. With
a bright illumination source, high throughput can be achieved because
the stage can be scanned at high speeds.
The first step-and-scan tool from the Silicon Valley Group
[18]
required a 2.4-kW lamp and an arcuate light tunnel to provide a
high-intensity uniform exposure dose at full scan speed. The 0.35-NA
projection optics are of the reflective ring-field type with 4×
magnification capability added (Figure 19).
In practical implementation, lenses are added for aberration
correction. The alignment of the projection optics required a specially
developed DUV interferometer to reach diffraction-limited performance.
Figure 19
A novel permanent magnet planar motor system and air-bearing wafer
stage were developed to step and scan the wafer at velocities of 50 to
65 mm/s. The reticle and wafer stage were synchronized by master-slave
servo control to ±40 nm. Through-the-lens viewing was implemented at
the 488-nm and 512-nm argon laser lines to provide flexibility against
thin-film interference effects. Active vibration isolation and
temperature-controlled, chemically filtered air were provided to limit
environmental influences on the projection optics and wafer.
This tool achieved a DOF greater than ±0.75 µm at a resolution of
0.5 µm. Full-field distortion was measured at
70 nm, and
overlay capability on oxide wafers of 150 nm (98%) was achieved by
using six-field global fine alignment. Product overlay performance for
manufacturing tools of this type was 120 nm to 200 nm depending on the
level. In production, the step-and-scan tool was capable of several
hundred wafers per day and achieved reliability in excess of 200 hr
mean time between fails (MTBF).
A 0.42-NA DUV Nikon stepper (Table 1) was also used for applications
with ground rules of 0.5 µm or less. The all-quartz refractive lens
of this tool required a <3-pm-bandwidth excimer laser illumination
source because of the single-material optical design. An advanced Cymer
laser source was required for pulse-to-pulse stability and dose
accuracy. The condenser optics relied on a fly's-eye lens and a
vibrating mirror to achieve dose uniformity and low speckle. The
condenser optics were pressurized slightly to prevent the accumulation
of airborne contaminants on the lens surfaces.
This tool achieved a DOF of approximately 1.0 µm at a resolution of
0.45 µm and an overlay of <150 nm on product. The DUV stepper, which
provided reliable production capacity, has a throughput of
approximately two hundred wafers per day.
1993 to 1995
A 0.5-NA DUV step-and-scan tool (Table 1) was developed for
resolutions of 0.35 µm and smaller
[19]. The optics and development
of the optional off-axis broadband viewing system represent significant
changes from the original step-and-scan tool. A fly's-eye lens and
light polarization are used to more than double the uniform
exposure power to 20 mJ/cm². The 5-mm-by-22-mm
rectangular scanned field is produced using a compact
beam-splitter cube design [19]
(Figure 20).
Through-the-lens viewing was improved and an
off-axis viewing system added to provide viewing at higher NA with
broadband illumination.
Figure 20
This tool achieves a DOF of ±0.40 µm at a resolution of 0.35 µm
and a full-field distortion that is significantly lower at
35 nm.
Global fine alignment achieves an overlay of 90 nm on oxide films and a
product overlay of 90 to 150 nm depending on the level.
Beyond 1996
Step-and-scan tools equipped with a 0.6-NA lens for
0.25-µm resolution will soon be the standard DUV tool.
A high-repetition-rate excimer laser exposure source for these tools
will provide enough power to expose less sensitive resists at higher
stage speeds. The 0.6 NA will provide 0.25-µm images, but with a very
small (0.4-µm) depth of focus. The use of off-axis illumination and
variable
should partially alleviate the depth-of-focus limitations.
Overlay will be improved because optical distortions become smaller,
and better viewing and stage capabilities will be available. Wafer
throughputs and productivity will improve because the stages are being
driven faster.
Lithography outlook: 1996-2000
Optical lithography continues to push beyond the anticipated
limits, as state-of-the-art I-line production approaches 0.35-µm
features and as high-NA DUV tools achieve sub-0.25-µm capability
[20]]. DUV resist performance will
continue to improve as diffusion
effects related to the chemical amplification process are minimized and
resin dissolution characteristics are enhanced. Circuit designs
compatible with off-axis illumination, combined with the availability
of phase-shift reticle inspection and repair equipment, will further
extend the capability of optical lithography. Scaling the exposure
wavelength an additional 20% with 193-nm systems
[21], combined with
these other techniques, should provide a path to a sub-0.15-µm
lithography capability.
Acknowledgments
The authors gratefully acknowledge Grant Willson, Hiroshi Ito,
Nick Clecak, Russ Wendt, Clint Snyder, Bill Brunsvold, Will Conley, Rob
Wood, George Hefferon, Karey Holland, Al Bergendahl, John Sturtevant,
Paul Rabidoux, Denis Poley, K. C. Norris, Steve Lapine, Curt Rude,
Roger Barr, Bob Cogley, Bob Batterson, Mike Charney, and Hal Linde.
References
Received February 9, 1996; accepted for publication December 2, 1996
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