Method and apparatus for making an integrated circuit using...

Radiation imagery chemistry: process – composition – or product th – Radiation modifying product or process of making – Radiation mask

Reexamination Certificate

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Reexamination Certificate

active

06645678

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates generally to integrated circuit technology and more particularly to using various properties of light in the making of integrated circuits.
BACKGROUND OF THE INVENTION
As semiconductor technology progresses, the dimensions of features, for example, line widths, gate dimensions, etc., in integrated circuits are shrinking. Many obstacles must be overcome in order to process an integrated circuit with features of these dimensions. One such problem exists in photolithography because the featured dimensions are too small relative to the wavelength of the light being used. Phase shift masks provide a technique for alleviating this problem by providing desirable destructive interference at the areas where the fine dimensions are present. This approach results in other problems associated with leaving under-exposed photoresist in areas where the photoresist was intended to be fully exposed. One known solution of this problem is the use of a complementary phase shift mask (CPSM) process which is also called alternating aperture phase shift mask (AAPSM) process.
Some disadvantages of phase shift masks and of the CPSM process are exemplified by reference to a desired pattern of gate electrodes
14
and
16
as shown in FIG.
1
. Typically, such gate electrodes are the finest dimensions on the integrated circuit and are polysilicon. Thus the most advanced lithographic techniques are typically applied to polysilicon, but it could be a different gate material, and it could be a different purpose than for gates. Using a phase shift mask to attempt to achieve this desired pattern, begins with the formation of a phase shift mask
20
having phase shifting regions
22
and
30
and a transparent region
28
formed on a plate which is transparent to the light used to expose photoresist, for example, a quartz plate for deep ultraviolet light, as shown in FIG.
2
. The difference between phase shifting regions
30
and
22
and the transparent region
28
is the thickness of the plate. Typically, phase shifting regions
22
and
30
are thinned down regions of the plate, and transparent region
28
is not typically thinned. The plate passes light which is referenced to be at a phase angle of 0° and the phase shifting region passes light which is 180° out of phase with the 0° light. The 0° light has a non-zero light intensity that alters a property of the photoresist. Additionally the 180° light also has a non-zero light intensity and alters a property of the photoresist in a manner identical to the 0° light. In the region between the 0° light and the 180° light, light destructively interferes to form a “dark” area of low light intensity. This is the desirable feature of phase shift mask techniques. On mask
20
, regions
24
and
26
correspond to the intended dark regions on the photoresist-covered wafer, are formed out of chromium or another opaque material, and are positioned between phase shifting region
30
or
22
and transparent region
28
.
Developing semiconductor wafer
10
with phase shift mask
20
, however, results in semiconductor
10
shown in FIG.
3
. Gate electrode regions
16
and
14
have been patterned as desired. However a polysilicon phase conflict region
32
exists which arises from under-exposed photoresist as well. At the boundary between the 0 degrees and 180 degrees phase-shifted light there is destructive interference so that the photoresist in this boundary region may not be sufficiently exposed. The result of such insufficient exposure is that the photoresist in that area is not removed so that the subsequent etch of polysilicon results in an undesirable polysilicon phase conflict region
32
being formed. The result is that the very aspect of destructive interference that is desirable for gate formation has a similar effect at the boundary between the 0 degrees and 180 degrees phase shifting regions such as regions
30
and
28
. Although, region
32
is undesirable as shown, there may be other situations where a similar region formed at a boundary between 0 degrees and 180 degrees regions may be used to advantage, for example, to form a thin gate. For general designs, such so-called phase conflicts are mathematically unavoidable.
The CPSM process was developed to prevent this undesirable polysilicon phase conflict region
32
arising from the 0 degrees and 180 degrees boundaries. The CPSM process adds a second, binary mask which is complementary to phase shift mask
20
for use in an exposure subsequent to that using phase shift mask
20
. This second mask exposure occurs before the etch of the polysilicon so that the polysilicon region
32
is not actually formed. Region
32
, however, does correspond to an under exposed portion of the photoresist after exposure using mask
20
. The binary mask is opaque everywhere with regard to
FIG. 3
except over polysilicon phase conflict region
32
. Thus, after exposing semiconductor wafer
10
with the binary mask, removing the exposed photoresist, and etching the polysilicon, the desired semiconductor feature
10
of
FIG. 1
may be substantially achieved. Due to alignment problems between mask
20
and the complementary mask, it is likely that either some portion of region
32
be present or some portion of region
16
not be present, and in either case resulting in a somewhat different pattern than the desired pattern.
As discussed, in the solution provided by the CPSM process, the semiconductor wafer undergoes two exposures using different masks. This is disadvantageous in a semiconductor-processing environment because it increases cycle time and requires highly accurate alignment of two mask exposures. In addition the additional mask is an added cost. Accordingly, there is need for improvement over phase shift mask technology as it currently exists.


REFERENCES:
patent: 5245470 (1993-09-01), Keum
patent: 5292623 (1994-03-01), Kemp et al.
patent: 5308741 (1994-05-01), Kemp
patent: 5541026 (1996-07-01), Matsumoto
patent: 5663016 (1997-09-01), Hong
patent: 5677755 (1997-10-01), Oshida et al.
patent: 6163367 (2000-12-01), Obszarny
patent: 05011434 (1993-01-01), None
patent: 05241324 (1993-09-01), None
patent: 07036174 (1995-02-01), None
patent: 09120154 (1997-05-01), None
Bornig et al., “The Impact of Polarized Illumination on Imaging Characteristics in Optical Microlithography,” Elsevier Science B.V., Microelectronic Engineering 27 (1995) pp. 217-220.
Grobman et al., Reticle Enhancement Technology: Implications and Challenges for Physical Design, Motorola Digital DNA Laboratories, Austin, TX, pp. 73-77.
Kling et al., Practicing Extension of 248 DUV Optical Lithography Using Trim-Mask PSM (2 pgs.).
Kling et al., Practicing Extension of 248 DUV Optical Lithography Using Trim-Mask PSM (12 pp.).

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