Method for modeling a conductive semiconductor substrate

Computer-aided design and analysis of circuits and semiconductor – Nanotechnology related integrated circuit design

Reexamination Certificate

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C716S030000

Reexamination Certificate

active

06311312

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a method for modeling a semiconductor structure. In particular, the present invention relates to a method for modeling capacitance in conductive regions in a semiconductor substrate.
2. Discussion of the Related Art
Accurate extraction of impedance (e.g., capacitance) is essential for evaluating and predicting the performance of an integrated circuit manufactured under a given manufacturing process. Accurate values of impedance can be obtained only with accurate modeling of semiconductor structures manufactured under that process. A number of techniques for accurate extraction of impedance from interconnect structures of a semiconductor structure are disclosed in U.S. Pat. No. 5,901,063 (the “'063 Patent”), entitled “System and Method for Extracting Parasitic Impedance From an Integrated Circuit Layout,” Ser. No. 08/804,524, filed on Feb. 21, 1997, issued on May 4, 1999, and assigned to Frequency Technology, Inc., which is also the Assignee of the present application. The disclosure of the '063 Patent is hereby incorporated by reference in its entirety.
FIGS. 1
a
and
1
b
depict corresponding cross-sectional and top views of a typical CMOS semiconductor structure
100
using a conventional thermal oxide isolation technique, showing only two conductor layers
101
and
102
above the substrate. In more recent integrated circuit processes, the number of conductor layers is typically more numerous than is shown in
FIGS. 1
a
and
1
b
, often consisting of multiple layers of polysilicon and metal.
FIGS. 1
a
and
1
b
show two conductor layers merely for illustrative purposes. As shown in
FIGS. 1
a
and
1
b
, a semiconductor substrate
106
includes doped regions
106
a
and
106
b
of opposite conductivities, forming a P-well and an N-well for forming N-channel and P-channel transistors respectively. Thermal oxide regions
103
a
,
103
b
,
103
c
and
103
d
are provided to electrically isolate semiconductor regions
108
a
,
108
b
and
108
c
from each other. Thermal oxide regions
103
a
-
103
d
are typically formed by the well-known LOCOS process that oxidize the substrate silicon surface at high temperature. Devices, such as transistors and capacitors, are formed within the semiconductor regions.
The first conductor layer
101
above substrate
106
is used to provide both device electrodes and interconnect conductor traces between device electrodes. For example, in
FIGS. 1
a
and
1
b
, conductors
101
b
,
101
c
and
101
e
may be used as gate electrodes, and conductors
101
a
and
101
d
can be used as interconnect conductor traces. Conductor layer
101
is typically provided by doped polysilicon. Conductor layer
101
is isolated from substrate
106
by one or more dielectric layers
111
. Conductors
101
a
and
101
d
are routed over thermal oxide regions
103
a
and
103
c
. To form diffusion (e.g., source and drain regions for an active device) regions, a well-known self-aligned process step introduces impurities (“dopants”) into the regions
104
a
,
104
b
,
104
c
,
104
d
,
104
e
and
104
f
, using interconnect conductor layer
101
as a masking layer.
A layer of dielectric
109
is provided to isolate conductor layer
101
from conductor layer
102
. Conductor layer
102
can be provided by either polysilicon or metal. Openings in dielectric layers
109
and
111
are provided and filled with a conductive material
105
to electrically connect (as “contacts”) conductors in conductor layer
101
or diffusion regions
104
with conductors in conductor layer
102
. For example, contacts
105
a
and
105
b
are provided to connect conductors
102
a
and
102
b
to diffusion regions
104
a
and
104
b
, and contacts
105
c
and
105
d
are provided to electrically connect conductors
102
c
and
102
e
to conductors
101
c
and
101
e
, respectively.
Because thermal oxide (e.g., thermal oxide formed under the LOCOS process) is much thicker than the portion of silicon substrate from which the thermal oxide is formed, thermal oxidation results in an undulating surface topography at the surface of the substrate, as shown in Figure la. Subsequent growth or depositions of materials, such as dielectric layers
111
, conductor
101
and dielectric layer
109
, are typically conformal to this surface topography, as can be seen in
FIG. 1
a
. In the prior art, the capacitance in an active area between an electrode and a conductive portion of the substrate (e.g., a source or a drain region) is evaluated with the operation of the active device, and a capacitance between a conductor line in the “field region” (e.g., thermal oxide regions
103
a
and
103
c
) and a conductive portion of the substrate is simply ignored because of the width of the field region. Under thermal oxide isolation, the width of the field region is relatively large because of the so-called bird's beak structure (e.g., bird's beak
112
).
Recently, the width of the field region is greatly reduced by using deposited oxide isolation. One deposited oxide isolation technique is known as “shallow trench isolation” (STI), which is illustrated by
FIGS. 2
a
and
2
b
.
FIGS. 2
a
and
2
b
depict corresponding cross-sectional and top views of a semiconductor structure
200
, which includes two interconnect conductor layers
201
and
202
. (To simplify discussion of the figures, like reference numerals are provided like features). Unlike semiconductor structure
100
, however, rather than providing thermal oxide regions
103
a
-
103
d
, shallow trenches are etched in substrate
106
to isolate areas
108
a
,
108
b
and
108
c
. An oxide is then deposited over the surface of substrate
106
and to fill the trenches. A chemical-mechanical polishing (CMP) step planarizes the surface of substrate
106
by polishing the deposited oxide away from the surface of substrate
106
, thus providing the filled STI trenches
203
a
,
203
b
,
203
c
and
203
d
. Dielectric layers
111
,
109
and
110
, conductor layers
201
and
202
, and contacts layer
105
can be provided in substantially the same manner as dielectric layers
111
,
109
and
110
, conductor layers
101
and
102
and contacts layer
105
, respectively, as discussed above with respect to
FIGS. 1
a
and
1
b
. Alternatively, after each layer of conductor material (i.e., conductor layers
201
and
202
) is deposited, a CMP step can be applied to planarize the resulting surface, as shown in
FIG. 2
a.
Because STI trenches
203
a
-
203
d
can be made much narrower than corresponding thermal oxide regions
103
a
-
103
d
, capacitance between a conductor in the first conductor layer
201
(e.g., conductor
201
a
or
201
d
) and a conducting portion of the substrate(e.g., any of diffusion regions
104
a
,
104
c
-
104
f
) can no longer be ignored. In addition, even though one goal of CMP is to provide a completely planarized surface, because of selectivity of the process and local non-uniformity, “dishing” can often occur. At submicron feature sizes, to achieve high performance, accurate extraction of impedance can be achieved only with accurate modeling of the conductor layers and the substrate.
SUMMARY OF THE INVENTION
In accordance with the present invention, a method extracts capacitance in a semiconductor structure including a substrate, and two or more conductor layers above the substrate. The method includes (a) computing the capacitance between each conductor in the conductor layers and conductors in the proximity of the conductor, without regard to any conductor that is in the substrate; (b) grouping the conductors in the conductor layers with the conductors in the substrate; and (c) computing the capacitance between each of the conductors in the conductor layers and the conductors within the substrate. An example of a conductor in the substrate is a diffusion region. The method of the present invention is applicable to conductive layers of polysilicon.
According to one embodiment, the capacitance between each conductor in the cond

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