ELSEVIER Microelectronie Engineering 41/42 (1998) 83-86
MICROELECTRONIC
ENGINEERING
Sub-Resolution Feature OPC as an Enabler for Manufacturing at 0.2gm and Below
J. Randall@, A. Tritchkov*, K. Ronse*, and P. Jaenen*
@Texas Instruments, Dallas, Texas - on Assignment at IMEC
*IMEC, Kapeldreef 75,
B-3001, Leuven, Belgium
Optical proximity correction (OPC) with sub-resolution assisting features (outriggers) aided by adjustable
numerical apertures and partial coherence is shown to provide improvement in process windows through
tightening printed critical dimensions (CDs) and improving the depth of focus. Printed CD variations due to
mask errors are not exacerbated by the use of outriggers and may even be reduced by this type of OPC.
1. INTRODUCTION
As the critical dimensions (CDs) printed by
optical lithography shrink below the physical
wavelength of the exposing radiation, optical
proximity effects (OPE) are increasingly hard to
ignore. We address three important issues created by
OPE: The shift in size even at best focus of
linewidths as a function of the local pattern
environment (the pitch of an array of lines), depth of
focus (DOF) limitations, and the magnification of
mask CD errors[l]. This paper will deal primarily
with the printing of 0.2p.m lines at various pitches
on a clear field mask with 248mn lithography. We
assume that a manufacturable lithography process
will require mutually overlapping process windows
with at least a 0.6gm depth of field and 10%
exposure latitude for all relevant pattern pitches, not
just the extremes of the range of pitches.
The variable numerical aperture (NA) and partial
coherence (if) as well as off-axis illumination options
on state-of-the-art 248nm lithography systems am
important tools in dealing with OPE. Because
different pattems contain significantly different spatial
frequencies, the optimum optical configuration for
each pattern can be quite different. However, these
variables create a large parameter space that must be
explored to find suitable conditions for specific
applications.
Feature size biasing is the most common type of
OPC. However, feature biasing can only shift CDs
and does little to improve the change in CD with
defocus that is particularly acute with isolated lines.
The use of outriggers has been shown to be effective
in both correcting the CD and decreasing the change
in CD as the image is defocussed. The selection of
appropriate optical conditions and the use of
outriggers is useful for establishing overlapping
process windows for patterns with a wide variety of
pitches. The use of outriggers does require relatively
small features on photomasks, but commercial mask
makers have already demonstrated the ability to
make such masks. Commercial software exists that
automatically assigns placement of outriggers to
mask layouts[2].
2. PROCESS WINDOW IMPROVEMENT
A test reticle called RTP4 was loaned to IMEC
by the MicroUnity Systems Engineering Inc. for
evaluation of its perfommnce at 248nm. The reticle
contains many test structures and had outriggers
placed according to several different rule sets for
different target CDs. The 4X mask was fabricated by
Photronics. We investigated primarily 0.2gm line
patterns with fine-to-space ratios of 1:1, 1:2, 1:3,
and 1:4. The outriggers applied to these patterns
were nominally 75nm (IX) and placed (edge-to-
edge) 0.251ares (IX) from isolated features. There
were no outriggers placed between the 1:1 and 1:2
line arrays. The 1:3 array had a single 75nm
outrigger placed in the center of the space between
the lines. The 1:4 array had two 75nm outriggers in
the space between the lines, each placed 0.25gms
from the nearest 0.2gm line. By selecting these
particular line to space ratios, we avoided the
transition regions at approximately 1:2.5 and 1:3.5
where first one then two outriggers are placed
between the 0.2gm lines. MicroUnity is exploring
techniques to produce smooth transitions[3].
Prior to making test exposures with this mask on
the ASML PAS 5500 /300 deep-UV (248nm)
stepper, we used aerial image simulation to select
settings for the NA, o, and for annular illumination
conditions an inner boundary for the partial
coherence (o-inner). In the simulations, NA was
varied from 0.4 to 0.63, o was varied over 0.3 to
0.8, c-innercovered the range 0 to ~-0.3. We used
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