Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
1998-08-17
2001-10-30
Lee, Eddie (Department: 2815)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S347000, C257S348000, C257S350000, C257S352000, C257S369000
Reexamination Certificate
active
06310377
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a semiconductor device, and more particularly to a transistor using an SOI (Semiconductor On Insulator) substrate.
2. Description of the Background Art
An ASIC (Application Specific Integrated Circuit) is desired to operate at high speed with low power consumption, like a logic LSI such as a microprocessor, and so is a gate array which is a form of the ASIC.
FIG. 36
is a cross section showing a structure of a bulk NMOS transistor. A junction capacitance C
1
caused by a depletion layer
104
existing between an Si substrate
101
and a source region
102
(or a drain region
103
) is large and a wiring capacitance C
2
between a metal wire
105
disposed on an NMOS transistor and the Si substrate
101
through a LOCOS oxide film
108
is also large.
In this situation, proposed is a use of an SOI layer in a gate array.
FIG. 37
is a cross section showing a structure of an SOI NMOS transistor. Since a transistor on an SOI layer
106
has a thick buried oxide film
107
thereunder, both the junction capacitance C
1
and the wiring capacitance C
2
thereof are smaller than those of the bulk NMOS transistor. That allows higher-speed operation and lower power consumption.
Moreover, a transistor of which the source and drain are formed in the SOI layer
106
(referred to as “SOI transistor” hereinafter) has a semiconductor (body)
110
which is in an electrically-floating state between a source region
102
and a drain region
103
. A “body effect”, which refers to an action that a threshold value Vth of the transistor rises due to a potential difference between the Si substrate
101
and the source region
102
when a source potential rises (in case of an NMOS transistor), is not caused in the SOI transistor unlike the bulk transistor. Therefore, the SOI transistor may be always used with a small threshold value and operate with low voltage. Thus, the SOI transistor needs only low power consumption.
In the SOI transistor, however, when the source-to-drain voltage reaches a certain level or more, impact-ionized charges near the drain region
103
, e.g., positive holes in the NMOS transistor, do not escape into the Si substrate
101
to raise a potential at the body
110
which acts as a base of an NPN type parasitic bipolar transistor consisting of the body
101
, the source region
102
and the drain region
103
since the body
101
where a channel is formed is in the floating state. Then, a current driven by the bipolar transistor is superposed on an original current of the SOI transistor.
FIG. 38
is a graph showing a rise in current due to a parasitic bipolar effect. To avoid the parasitic bipolar effect, it is needed to fix the potential at the body
110
of the SOI transistor.
FIG. 39
is a plan view of a structure of field-shield isolation (referred to as “FS isolation” or “FS-isolated structure” hereinafter).
FIGS. 40 and 41
are cross sections of
FIG. 39
taken along the lines XXXX—XXXX, and XXXXI—XXXXI, respectively. An active region
111
having a width Lf is formed to become the source region
102
or the drain region
103
. The active region
111
is provided with a source-drain contact
96
to establish an electrical connection with a wire (not shown). For simple illustration, a gate contact
97
of a gate electrode
109
is not shown in FIG.
39
.
Similarly to a gate isolation by fixing a potential of the gate electrode
109
(e.g., by connecting the gate electrode
109
to the around GND through the gate contact
97
in a case of NMOS transistor) made in a direction of arrangement of the active region
111
(in vertical direction of FIG.
39
), the FS isolation is a device isolation with an FS gate
91
achieved in a direction perpendicular to the vertical direction (in a horizontal direction of FIG.
39
).
Specifically, the FS gate
91
, like the gate electrode
109
, is opposed to the SOI layer
106
with an insulative interlayer film interposed therebetween on both sides of the NMOS transistor, and when it is connected to the around GND, the NMOS transistor is isolated in the horizontal direction.
FIG. 42
is a cross section showing an isolation using a LOCOS oxide film (referred to as “LOCOS isolation” hereinafter) in the horizontal direction. When the LOCOS isolation is used, the SOI layer
106
is separated in the horizontal direction by the LOCOS oxide film
108
and hence it is impossible to provide a contact for supplying the SOI layer
106
with a predetermined potential. In contrast, when the FS isolation is used, the SOI layer
106
can extend also in the horizontal direction and hence it is possible to supply the SOI layer
106
with the predetermined fixed potential in the extension of the SOI layer
106
. In this case, it is necessary to provide an FS gate contact
92
for supplying the FS gate
91
with the predetermined potential and a contact plug
93
for FS isolation as shown in
FIG. 41
, and on the other hand, it is necessary to provide a body contact
94
for supplying the body with the predetermined potential and the contact plug
93
(a region indicated by hatching can have higher impurity concentration in the SOI layer
106
with which the contact plug
93
comes into contact). Therefore, there is a need for a chipped portion
95
at a position to provide the body contact
94
in the FS gate
91
, as shown in
FIGS. 39 and 40
.
This gate array, which supplies the body
110
with the predetermined potential, allows reduction in wiring capacitance, ensures high-speed operation and low power consumption and further prevents the parasitic bipolar effect. For example, the SOI transistor with FS-isolated structure may be used in an inverter.
FIG. 43A
shows a symbol of an inverter and
FIG. 43B
shows a specific configuration thereof. The inverter consists of a PMOS transistor P
1
and an NMOS transistor N
1
connected in series between a potential point supplying a potential Vcc and the ground GND. Specifically, the source of PMOS transistor P
1
is fixed to the potential Vcc and the source of NMOS transistor N
1
is fixed to the ground potential GND. In this configuration, even if the SOI transistors with FS-isolated structure are used as the transistors P
1
and N
1
and the bodies of the transistors P
1
and N
1
are fixed to the potential Vcc and the ground potential GND, respectively, no potential difference exists between the respective bodies and sources and hence no body effect works ill on the inverter.
However, there may be a case where it is preferable not to fix the potential at the body
110
so as not to lose the advantage of no body effect.
FIG. 44A
shows a symbol of an NAND circuit and
FIG. 44B
shows a specific configuration thereof. The NAND circuit consists of PMOS transistors P
1
and P
2
connected in parallel and NMOS transistors N
1
and N
2
connected in series between the potential point supplying the potential Vcc and the ground GND.
Since the sources of transistors P
1
, P
2
and N
2
are supplied with the potential Vcc, Vcc and the ground potential GND respectively, if the bodies of the transistors P
1
, P
2
and N
2
are supplied with the potential Vcc. Vcc and the ground potential GND respectively, no body effect is produced on the transistors. However, there may be a case where a potential higher than the ground potential GND is applied to the source of the transistor N
1
which is not supplied with a fixed potential, and when the ground potential GND is applied to the body of the transistor N
1
, a threshold voltage rises due to the body effect. In this situation, the NAND circuit can not operate with low voltage and hardly avoids slow operation.
FIG. 45
shows a layout where vertical alignments of the active regions (referred to as “fields” hereinafter) are arranged in the horizontal direction (this layout is referred to as “master layout” hereinafter). As illustrated in disregard of the gate electrodes, the fields
10
a
to
10
i
are seen rectangular. The characters “P” and “N” in rectangles indicate fields to be provi
Inoue Yasuo
Ipposhi Takashi
Kim Il Jung
Maeda Shigenobu
Maegawa Shigeto
Lee Eddie
Ortiz Edgardo
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