|
|
|
| United States Patent | 4652134 |
| Link to this page | http://www.wikipatents.com/4652134.html |
| Inventor(s) | Pasch; Nicholas F. (Mt. View, CA);
Hubbard; James L. (San Jose, CA) |
| Abstract | A system for aligning a semiconductor wafer with a mask bearing a pattern
to be formed on the wafer, in which both the wafer and the mask bear an
alignment mark, and in which light used for alignment is filtered to
transmit only in a selected bandwidth, uses a reflector system to gather
light reflected from edges of the alignment mark on the wafer. In order to
minimize the effect of erroneous alignment signals from standing waves
generated when the alignment signal is reflected from a wafer coated with
a layer of photoresist, a second filter is placed in the path of light
after it has reflected from the target. This second filter transmits a
range of the reflected light which does not produce standing waves. |
|
|
|
Title Information  |
|
|
|
|
|
Drawing from US Patent 4652134 |
|
|
Mask alignment system |
|
|
|
|
|
| Publication Date |
March 24, 1987 |
|
|
|
|
|
| Filing Date |
August 28, 1984 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Title Information  |
|
|
Description  |
|
|
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to the fabrication of integrated circuit devices and
in particular to an improved system and method for aligning the masks used
during formation of patterned photoresist on an integrated circuit.
2. Description of the Prior Art
One processing step used in the fabrication of integrated circuits is a
photolithographic step, where a semiconductor wafer is coated with a light
sensitive photoresist. Using a mask, the photoresist is exposed to light
in a pattern in order to prepare the photoresist for etch processes. One
method for projecting an appropriate pattern is the use of a projection
system such as the Ultratech Stepper Model 900 projection stepper. One
type of mask used during photolithographic steps is a chromed glass or
quartz plate bearing the image to be projected onto the integrated
circuit. Light is projected onto the mask and those areas on the mask
which are not chromed transmit the light, with chromed areas of the mask
preventing transmission of light. The transmitted light is projected by a
complex system of prisms and lenses so that a clear and accurate image of
the pattern on the mask is projected onto a portion of the photoresist
layer formed on the semiconductor wafer.
A simplified diagram of a projection stepper such as the Ultratech Model
900 is shown in FIG. 1. Light source 8 provides white light which is
filtered to remove ultraviolet light. Light from light source 8 passes
through light tunnel 7. Light tunnel 7 limits the light which passes
through light tunnel 7 to those light rays which lens 9 can focus. The
light passing through light tunnel 7 is controlled by actinic shutter 5
and high-speed shutter 6. Actinic shutter 5 does not block light, as does
a conventional shutter. Instead, actinic shutter 5 allows light of a
selected wavelength and/or pattern to pass. In the Ultratech Model 900,
actinic shutter 5 passes only light having wavelengths within the range of
450 to 600 nanometers, and is thus used to limit the bandwidth of the
light used for aligning mask 1 with wafer 4. Actinic shutter 5 is not used
during the actual exposure of photoresist and thus the light from light
source 8 is not limited in bandwidth during exposure of the photoresist.
The light from light source 8 is focused by lens 9 toward mask 1 and prism
unit 2. Mask 1 carries the desired pattern for exposing the photoresist on
wafer 4. The patterned light provided by mask 1 is directed by prism unit
2. The light from prism unit 2 is focused on the area wafer 4 containing
photoresist which is to be exposed with the image of mask 1.
Before exposing wafer 4 to the image on mask 1, the image on mask 1 must be
properly aligned with wafer 4, so that components of the integrated
circuit formed using the patterned photoresist produced by this
photolithographic step will be properly aligned on wafer 4. During the
alignment stage, high speed shutter 6 is opened and actinic shutter 5
remains closed. Actinic shutter 5 passes only light having wavelengths
within the range of 450 nanometers to 600 nanometers. The light used in
the alignment process must not expose the photoresist. Thus the light
allowed to pass by actinic shutter 5 is limited to wavelengths having
insufficient energy to cause the photoresist to chemically react.
Therefore, the light provided through actinic shutter 5 has no effect on
the photoresist on wafer 4.
An alignment target is a relief pattern on wafer 4 in a specific selected
pattern. One example of an alignment target is shown in FIG. 2. For
example, this relief area can be formed by polycrystalline silicon etched
into a selected pattern. Alignment target 15 is used to align mask 1 with
wafer 4, thereby insuring that components of the integrated circuit formed
using the photoresist exposed during this photolithographic step are
properly aligned.
Actinic shutter 5 includes a pattern which corresponds in shape to the
shape of alignment target 15. With actinic shutter 5 closed and high-speed
shutter 6 open, the pattern borne by actinic shutter 5 is projected onto
an image on mask 1 of alignment target 15. The pattern projected by light
source 8 through actinic shutter 5 is slightly larger than the image of
alignment target 15 on mask 1, therefore the light transmitted from mask 1
has a pattern corresponding to an outline of alignment target 15.
This outline of the alignment target is projected by prism unit 2 onto
reflector 10. A samll aperture 17 is provided in the center of concave
reflector 10. The outline of the alignment target is reflected off
reflector 10, through prism unit 2, and onto wafer 4. A diagram excluding
prism unit 2 and isolating reflector 10 and wafer 4 is shown in FIG. 3.
Reflector 10 is designed so that light waves reflected from prism 2 onto
reflector 10, and from prism 2 onto wafer 4 and thus reflected from wafer
4 back to prism unit 2 strike reflector 10 at a right angle. As shown in
FIG. 4, light from reflector 10 which is reflected by a flat portion of
the surface of wafer 4 is reflected at an angle equal to the angle of
incidence .phi.. Therefore, light that is reflected from flat surfaces on
wafer 4 does not enter aperture 17 (FIG. 1). However, light that strikes
the edge of alignment target 15 as shown in FIG. 4 is scattered upon
reflecting off the edge of alignment target 15. Some of the scattered
light enters into aperture 17.
When the outline of the alignment target transmitted from mask 1 and
reflected from reflector 10 is misaligned, for example as shown in FIG.
5a, very little of the light provided by the outline of the alignment
target strikes the edges of alignment target 15. Therefore, very little
light passes through aperture 17. Conversely, when the outline of the
alignment target is properly aligned as shown in FIG. 5b, all of the edges
of alignment target 15 are struck by light from the outline of the
alignment target. Therefore, the light that passes through aperture 17 in
reflector 10 is at peak intensity when the outline of the alignment target
is properly aligned with alignment target 15.
Referring back to FIG. 1, the light that passes through aperture 17 is
focused by lens 11 and passes through alignment target mask 12. A plan
view of alignment target mask 12 is shown in FIG. 6. Alignment target mask
12 allows light to pass which conforms to the pattern of alignment target
15. The image projected through aperture 17 in reflector 10 is most
intense in a pattern conforming to the shape of alignment target 15.
Therefore, alignment target mask 12 confines the light passing through
alignment target mask 12 to the pattern of alignment target 15. This helps
insure that the light passing through the aperture of reflector 10 is
reflecting from alignment target 15 and is not reflected from some other
feature on wafer 4 which does not have a pattern conforming to alignment
target 15. When the light reflected from reflector 10 strikes a pattern on
wafer 4 which does not conform to alignment target 15, the light reflected
from this pattern which passes through aperture 17 is an image which
conforms to the other feature and not to the target. Alignment target mask
12 blocks enough of this light to prevent the erroneous reflected light
from being perceived as a true alignment signal.
The light passing through alignment target mask 12 is focused by lens 13
onto photomultiplier tube 14. Photomultiplier tube 14 provides an
electrical signal to alignment circuitry (not shown) proportional to the
intensity of the light incident on photomultiplier tube 14. Thus, when the
signal provided by photomultiplier tube 14 is at peak intensity, the image
of alignment target 15 on mask 1 and alignment target 15 on wafer 4 are
properly aligned.
Various phenomena can introduce error into the alignment system. A major
source of error is standing waves of light which are generated in the
photoresist on wafer 4. This phenomenon is particularly troublesome when
the surface of wafer 4 is coated by unpatterned metalization which is
covered by photoresist. When these standing waves occur, they cause
spurious variations in the light intensity pattern of the alignment mask
seen by photomultiplier tube 14.
FIG. 7a is a diagram depicting an ideal alignment signal as provided by
photomultiplier tube 14 when mask 1 and wafer 4 are being aligned. The
ideal alignment signal provides a clear peak when mask 1 and wafer 4 are
properly aligned, as shown in FIG. 7a. FIG. 7b is a diagram depicting a
typical alignment signal provided by photomultiplier tube 14 in FIG. 1
when photolithographic projection stepper 20 is aligning a wafer 4 which
is coated by a metal layer covered with photoresist. The deviation of the
signal in FIG. 7b from the ideal signal of FIG. 7a is caused by standing
waves. The signal of FIG. 7b has not one peak as does the signal of FIG.
7a, but three peaks which leaves the computer of photolithographic
projection stepper 20 guessing as to which peak, if any of the three,
indicates proper alignment.
Others have attempted to control this phenomenon by limiting the light
transmitted through actinic shutter 5 to frequencies of light which will
not generate standing waves. For unknown reasons, this technique has
proven to be ineffective.
SUMMARY
A photolithographic system designed in accordance with this invention
includes a filter which limits an optical alignment signal to light within
a selected frequency range, and also includes a filter which limits the
light which has been reflected from a target on a wafer to be aligned
thereby eliminating or minimizing extraneous light caused by standing
waves. The filter is placed between the optical system generating the
alignment signal, which indicates when proper alignment has been achieved
between the photolithographic mask and the wafer which receives its
photolithographic pattern from that mask, and the photosensitive device
which receives the alignment signal.
DESCRIPTION OF THE DRAWING
FIG. 1 is a diagram depicting a simplified photolithographic projection
stepper machine;
FIG. 2 is a drawing depicting an example of an alignment target;
FIG. 3 is a diagram isolating the relationship between reflector 10 and
wafer 4 of FIG. 1;
FIG. 4 is a diagram illustrating the effect of wafer 4 upon light waves
incident upon wafer 4 and alignment target 15;
FIG. 5a depicts a slightly misaligned image projected from mask 1 onto
wafer 4 near alignment target 15;
FIG. 5b depicts a properly aligned image reflected from mask 1 onto wafer 4
aligned with alignment target 15;
FIG. 6 is a diagram depicting alignment target mask 12 of FIG. 1;
FIGS. 7a and 7b are diagrams depicting an ideal alignment signal and an
actual alignment signal produced by a photolithographic projection stepper
such as photolithographic projection stepper 20 of FIG. 1;
FIG. 8 is a diagram depicting one embodiment of this invention; and
FIG. 9 is a diagram depicting an actual alignment signal provided by a
photolithographic projection stepper such as photolithographic projection
stepper 21.
DETAILED DESCRIPTION
FIG. 8 is a diagram depicting one embodiment of a photolithographic
projection stepper constructed in accordance with this invention.
Components in the embodiment of FIG. 8 function in the same manner as
components having corresponding reference numbers in FIG. 1. In the
structure shown in FIG. 8, an image reflected from alignment target 15
(FIG. 2) on wafer 4 passes through aperture 17, lens 11, aperture mask 12,
lens 13, and filter 16, to photomultiplier tube 14. In one embodiment of
this invention, filter 16 is a magenta photographic filter such as a Kodak
Wratten #31, 32, 33 or 34 filter. Filter 16 filters out light waves having
wavelengths of less than 450 nanometers and greater than 560 nanometers.
Therefore, standing waves generated when the alignment system shown in
FIG. 8 is used to align a wafer having a layer of metal underneath a layer
of photoresist which are caused by wavelengths less than 450 nanometers or
greater than 560 nanometers are filtered out, and thus not presented to
photomultiplier tube 14.
Empirical evidence has shown that a photoresist layer having a thickness of
approximately 17,000 angstroms creates standing waves of light having
wavelengths in the range of 560 to 600 nanometers. Photoresist layers of
other thicknesses will generate standing waves of light of associated
wavelengths, and thus require the use of a filter to filter out the
standing waves, whatever their wavelengths might be. If a selected
thickness of photoresist creates standing waves of light having
wavelengths between 450 and 560 nanometers, the thickness of the
photoresist is preferably adjusted slightly to a thickness which does not
create standing waves of light having wavelengths between 450 and 560
nanometers, but provides a layer of photoresist of substantially desired
thickness. In this manner, the use of a magenta filter in accordance with
the teachings of this invention removes standing waves for substantially
all thicknesses of photoresist.
Use of a magenta filter in accordance with this invention to filter the
light which generates the alignment signal greatly enhances the difference
in magnitude between the alignment signal when the mask and wafer are
properly aligned and the alignment signal when the mask and wafer are
misaligned by eliminating most standing waves which often cause erroneous
alignment signals. Thus an alignment system constructed in accordance with
this invention filters the light reflected from alignment target 15 on
wafer 4 to limit this light to the wavelengths provided by light source 8
through actinic shutter 5 which do not generate standing waves.
By enhancing the difference between the aligned and misaligned signals,
alignment is more accurately performed because the background noise and
distortion of the alignment signal produced by photomultiplier tube 14 in
response to standing waves is minimized, thereby decreasing the number of
integrated circuits discarded because of improper alignment during the
photolithographic process.
FIG. 9 is a diagram depicting a typical alignment signal provided by
photomultiplier tube 14 in FIG. 8 when photolithographic projection
stepper 21 is aligning a wafer 4 on which is formed a metal layer covered
with photoresist. Photolithographic projection stepper 21, which is one
embodiment of this invention, produces an alignment signal much closer to
the ideal alignment signal depicted in FIG. 7a. The operator of
photolithographic projection stepper 21 is provided with a clearly
predominant peak which clearly indicates proper alignment, unlike the
ambiguous signal of prior art photolithographic stepper 20 (FIG. 1)
depicted in FIG. 7b.
While this specification illustrates the specific embodiments of this
invention, it is not to be interpreted as limiting the scope of the
invention. Other embodiments of this invention will become evident to
those of ordinary skill in the art in light of the teachings of this
specification.
* * * * *
|
|
|
|
|
Description  |
|