Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
2001-03-19
2004-01-13
Zarabian, Amir (Department: 2822)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S330000
Reexamination Certificate
active
06677643
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to semiconductor devices which include, between the major surfaces thereof, a layer with low electrical resistance and an alternating conductivity type layer formed of regions of a first conductivity type and regions of a second conductivity type alternately arranged with each other. Specifically, the present invention relates to vertical semiconductor devices, which facilitate the realization of a high breakdown voltage and a high current capacity, such as MOSFET's (insulated gate field effect transistors), IGBT's (conductivity-modulation-type MOSFET's), bipolar transistors and diodes. The present invention relates also to the method of manufacturing the semiconductor devices described above.
BACKGROUND
The semiconductor devices may be roughly classified into lateral semiconductor devices arranged with electrodes on a major surface, and vertical semiconductor devices which distribute electrodes on both major surfaces facing opposite to each other. When the vertical semiconductor device is ON, a drift current flows in the thickness direction of the semiconductor chip (vertical direction). When the vertical semiconductor device is OFF, the depletion layers caused by applying a reverse bias voltage also expands in the vertical direction.
FIG. 7
is a cross sectional view of a conventional planar-type n-channel vertical MOSFET. Referring now to
FIG. 7
, the vertical MOSFET includes an n
+
-type drain layer
11
with low electrical resistance, a drain electrode
18
in electrical contact with n
+
-type drain layer
11
, a highly resistive n
−
-type drift layer
12
on n
+
-type drain layer
11
, p-type base regions
13
formed selectively in the surface portion of n
−
-type drift layer
12
, a heavily doped n
+
-type source region
14
formed selectively in p-type base region
13
, a gate insulation film
15
on the extended portion of p-type base region
13
extended between n
+
-type source region
14
and n
−
-type drift layer
12
, a gate electrode layer
16
on gate insulation film
15
, and a source electrode
17
in electrical contact commonly with n
+
-type source regions
14
and p-type base region
13
, and a drain electrode
18
on the back surface of n
+
-type drain layer
11
.
In the vertical semiconductor device shown in
FIG. 7
, highly resistive n
−
-type drift layer
12
works as a region for making a drift current flow vertically when the MOSFET is in the ON-state. In the OFF-state of the MOSFET, n-type drift layer
12
is depleted, causing a high breakdown voltage. Thinning highly resistive n
−
-type drift layer
12
, that is shortening the drift current path, is effective for substantially reducing the on-resistance (resistance between the drain and the source) of the MOSFET, since the drift resistance is lowered in the ON-state of the device. However, since the space between the drain and the source, into that the depletion layers expand from the pn-junctions between p-type base regions
13
and n
−
-type drift layer
12
in the OFF-state of the device, is narrowed by shortening the drift current path in n
−
-type drift layer
12
, the electric field strength in the depletion layers soon reaches the maximum (critical) value for silicon. Therefore, breakdown is caused before the voltage between the drain and the source reaches the designed breakdown voltage of the device.
A high breakdown voltage is obtained by thickening n
−
-type drift layer
12
. However, a thick n
−
-type drift layer
12
inevitably causes high on-resistance and loss increase. In short, there exists a tradeoff relation between the on-resistance (current capacity) and the breakdown voltage of the MOSFET.
The tradeoff relation exists in the other semiconductor devices, such as IGBT's, bipolar transistors and diodes. The tradeoff relation exists also in the lateral semiconductor devices, therein the flow direction of the drift current in the ON-state of the devices is different from the expansion direction of the depletion layers in the OFF-state of the devices.
European Patent 0 053 854, U.S. Pat. No. 5,216,275, U.S. Pat. No. 5,438,215, and Japanese Unexamined Laid Open Patent Application H09(1997)-266311 disclose semiconductor devices, which reduce the tradeoff relation described above by employing an alternating-conductivity-type drift layer formed of heavily doped n-type regions and p-type regions alternately laminated horizontally with each other.
FIG. 8
is a cross sectional view of the vertical MOSFET disclosed in U.S. Pat. No. 5,216,275. Referring now to
FIG. 8
, the vertical MOSFET of
FIG. 8
is different from the vertical MOSFET of
FIG. 7
in that the vertical MOSFET of
FIG. 8
includes an alternating conductivity type drift layer
22
that is not a single-layered one but formed of n-type drift regions
22
a
and p-type partition regions
22
b
alternately laminated horizontally with each other. In
FIG. 8
, p-type base regions
23
, n
+
-type source regions
24
, gate insulation film
25
, gate electrodes
26
, a source electrode
27
, and a drain electrode
28
are also shown.
Drift layer
22
is formed in the following way. A highly resistive n-type layer is formed epitaxially on n
+
-type drain layer
21
as a substrate. Trenches are dug selectively in the n-type layer down to n
+
-type drain layer
21
by etching, leaving n-type drift regions
22
a.
Then, p-type partition regions
22
b
are formed by epitaxially growing p-type layers in the trenches.
The alternating conductivity type layer provides a drift current path in the ON-state of the device and is depleted in the OFF-state of the device. Hereinafter, the semiconductor device including an alternating conductivity type drift layer will be referred to as the “super-junction semiconductor device”.
The dimensions and the impurity concentrations of the constituent elements in the super-junction semiconductor device described in U.S. Pat. No. 5,216,275 are as follows. Assuming that the breakdown voltage is V
B
, drift layer
22
is 0.024 V
B
1.2
(&mgr;m) in thickness, and n-type drift region
22
a
and p-type partition region
22
b
have the same width b and the same impurity concentration, the impurity concentrations in n-type drift region
22
a
and p-type partition region
22
b
are expressed by 7.2×10
16
V
B
−0.2
/b(cm
−3
). When V
B
=800 V and b=5 &mgr;m, drift layer
22
is 73 &mgr;m in thickness and the impurity concentration thereof is 1.9×10
16
cm
−3
. Obviously, the alternating conductivity type drift layer reduces the on-resistance, since the impurity concentration in the single-layered drift layer is around 2×10
14
cm-
3
. However, it is very difficult for the epitaxial growth technique available at present to bury semiconductor layers with a good quality in such narrow and deep trenches, that is trenches with a large aspect ratio.
As described above, the tradeoff relation between the on-resistance and the breakdown voltage poses a problem also on the lateral semiconductor devices. European Patent 0 053 854, U.S. Pat. No. 5,438,215, and Japanese Unexamined Laid Open Patent Application H09(1997)-266311 disclose also lateral super-junction semiconductor devices and the methods of manufacturing the lateral super-junction semiconductor devices. The disclosed methods employ selective etching to dig trenches and epitaxial growth to bury the trenches. It is not so difficult for the selective etching technique and the epitaxial growth technique to form the alternating-conductivity-type drift layer for the lateral super-junction semiconductor device, since the lateral alternating-conductivity-type drift layer is formed by laminating thin epitaxial layers vertically.
However, the conventional selective etching and epitaxial growth techniques are not so effective to form the vertical alternating-conductivity-type drift layer described in U.S. Pat. No. 5,216,275. Japanese Unexamined Laid Open Pa
Fujihira Tatsuhiko
Iwamoto Susumu
Onishi Yasuhiko
Sato Takahiro
Ueno Katsunori
Fuji Electric & Co., Ltd.
Rose Kiesha
Rossi & Associates
Zarabian Amir
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