Control trimming of hard mask for sub-100 nanometer...

Semiconductor device manufacturing: process – Coating with electrically or thermally conductive material – Insulated gate formation

Reexamination Certificate

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C438S592000, C438S197000

Reexamination Certificate

active

06482726

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates generally to semiconductor fabrication technology, and, more particularly, to techniques for manufacturing semiconductor devices with reduced critical dimensions.
2. Description of the Related Art
There is a constant drive within the semiconductor industry to increase the operating speed of integrated circuit devices, e.g., microprocessors, memory devices, and the like. This drive is fueled by consumer demands for computers and electronic devices that operate at increasingly greater speeds. This demand for increased speed has resulted in a continual reduction in the size of semiconductor devices, e.g., transistors. That is, many components of a typical field effect transistor (FET), e.g, channel length, junction depths, gate dielectric thickness, and the like, are reduced. For example, all other things being equal, the smaller the channel length of the FET, the faster the transistor will operate. Thus, there is a constant drive to reduce the size, or scale, of the components of a typical transistor to increase the overall speed of the transistor, as well as integrated circuit devices incorporating such transistors. Additionally, reducing the size, or scale, of the components of a typical transistor also increases the density, and number, of the transistors that can be produced on a given amount of wafer real estate, lowering the overall cost per transistor as well as the cost of integrated circuit devices incorporating such transistors.
However, reducing the size, or scale, of the components of a typical transistor also requires being able to form and pattern components such as the gate conductor and gate dielectric on such reduced scales, consistently, robustly and reproducibly, preferably in a self-aligned manner. The ability to form and pattern components such as the gate conductor and gate dielectric on such reduced scales, consistently, robustly and reproducibly, is limited by, among other things, physical limits imposed by photolithography. Diffraction effects impose limits on the critical dimensions of components such as gate conductors and gate dielectrics that correspond roughly to the wavelengths of the light used to perform the photolithography. Retooling wafer fabs to use shorter wavelengths, as in deep ultraviolet (DUV) photolithography and/or in high-energy electron beam lithography, is very expensive.
One conventional approach to achieving reduced critical dimensions, resorting to expensive DUV photolithography and/or high-energy electron beam lithography, is schematically illustrated in
FIGS. 1-4
. As shown in
FIG. 1
, for example, a conventional MOS transistor
100
may be formed on a semiconducting substrate
105
, such as doped-silicon. The MOS transistor
100
may have a doped-polycrystalline silicon (doped-polysilicon or doped-poly) gate conductor such as an N
+
-doped-poly (P
+
-doped-poly) gate
110
formed above a gate oxide
115
formed above the semiconducting substrate
105
. The N
+
-doped-poly (P
+
-doped-poly) gate
110
and the gate oxide
115
may be separated from active areas such as N
+
-doped (P
+
-doped) source/drain regions
120
of the MOS transistor
100
by dielectric spacers
125
. The dielectric spacers
125
may be formed above N

-doped (P

-doped) source/drain extension (SDE) regions
130
. As shown in
FIG. 1
, shallow trench isolation (STI) regions
140
may be provided to isolate the MOS transistor
100
electrically from neighboring semiconductor devices such as other MOS transistors (not shown).
The N

-doped (P

-doped) SDE regions
130
are typically provided to reduce the magnitude of the maximum channel electric field found close to the N
+
-doped (P
+
-doped) source/drain regions
120
of the MOS transistor
100
, and, thereby, to reduce the associated hot-carrier effects. The lower (or lighter) doping of the N

-doped (P

-doped) SDE regions
130
, relative to the N
+
-doped (P
+
-doped) source/drain regions
120
of the MOS transistor
100
(lower or lighter by at least a factor of two or three), reduces the magnitude of the maximum channel electric field found close to the N
+
-doped (P
+
-doped) source/drain regions
120
of the MOS transistor
100
, but increases the source-to-drain resistances of the N

-doped (P

-doped) SDE regions
130
.
As shown in
FIG. 1
, typically the N
+
-doped-poly (P
+
-doped-poly) gate
110
and the gate oxide
115
have a critical dimension &dgr;
DUV
that effectively determines a channel length &lgr; of the MOS transistor
100
. The channel length &lgr; is the distance between the N

-doped (P

-doped) SDE regions
130
adjacent the N
+
-doped-poly (P
+
-doped-poly) gate
110
and the gate oxide
115
.
As shown in
FIGS. 2-4
, typically the critical dimension &dgr;
DUV
of the N
+
-doped-poly (P
+
-doped-poly) gate
110
and the gate oxide
115
is determined as follows. As shown in
FIG. 2
, a gate oxide layer
215
is formed above the semiconducting substrate
105
, and a gate conductor layer
210
is formed above the gate oxide layer
215
. An antireflective coating (ARC) layer
230
is formed above the gate conductor layer
210
. For the sake of comparison, a photoresist layer
220
is shown, as if formed and patterned using conventional non-DUV photolithography, above the ARC layer
230
. The photoresist layer
220
is patterned to have a smallest, non-deep ultraviolet diffraction-limited dimension &dgr;
non-DUV
that may be larger than about 1800 Å.
As shown in
FIG. 3
, a photoresist mask
320
is formed and patterned, using conventional DUV photolithography and/or high-energy electron beam lithography, above the ARC layer
230
. The photoresist layer
220
is indicated in phantom, for the sake of comparison. The photoresist mask
320
will typically have the smallest, deep ultraviolet diffraction-limited critical dimension &dgr;
DUV
that may be about 1800 Å that will determine the size of the N
+
-doped-poly (P
+
-doped-poly) gate
110
and the gate oxide
115
.
As shown in
FIG. 4
, the photoresist mask
320
having the critical dimension &dgr;
DUV
is used as a mask to remove respective portions
410
(shown in phantom) from the gate conductor layer
210
(
FIGS. 2-3
) to form a gate structure
400
that includes the N
+
-doped-poly (P
+
-doped-poly) gate
110
and a portion of the gate oxide layer
215
that will eventually become the gate oxide
115
after subsequent etching and/or processing. The gate structure
400
, and, hence the N
+
-doped-poly (P
+
-doped-poly) gate
110
, will also have the critical dimension &dgr;
DUV
defined by the photoresist mask
320
. Nevertheless, the critical dimension &dgr;
DUV
defined by the photoresist mask
320
and total etch is still too large. It would be desirable to have a less expensive technique that would be sufficiently controllable, reliable and feasible to form and pattern components such as gate conductors on even more reduced scales, consistently, robustly and reproducibly, preferably in a self-aligned manner.
The present invention is directed to overcoming, or at least reducing the effects of, one or more of the problems set forth above.
SUMMARY OF THE INVENTION
In one aspect of the present invention, a method is provided, the method including forming a gate dielectric layer above a substrate layer, forming a gate conductor layer above the gate dielectric layer, forming a first hard mask layer above the gate conductor layer, and forming a second hard mask layer above the first hard mask layer. The method also includes forming a trimmed photoresist mask above the second hard mask layer, and forming a patterned hard mask in the second hard mask layer using the trimmed photoresist mask to remove portions of the second hard mask layer, the patterned hard mask having a first dimension. The method further includes forming a selectively etched hard mas

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