Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
2000-08-30
2003-03-11
Fahmy, Wael (Department: 2814)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S348000, C257S349000, C257S350000, C257S506000
Reexamination Certificate
active
06531738
ABSTRACT:
BACKGROUND OF THE INVENTION
(1)Field of the Invention
The present invention relates to an SOI (Silicon On Insulator) semiconductor device, and especially relates to a technology of improving the operating voltage of the SOI semiconductor device.
(2)Related Art
In order to electrically separate the semiconductor elements in a semiconductor integrated circuit, the dielectric isolation is often used. In the dielectric isolation, insulating layers are formed at the bottom and on the side of the semiconductor layer, which is the active layer of the semiconductor device. In this specification, this structure is referred to “dielectric isolation structure”.
The SOI semiconductor device with the dielectric isolation structure solves problems facing the conventional semiconductor device using the pn junction isolation, i.e., leakage current via the pn junction and unexpected bipolar effects. The SOI semiconductor device with the dielectric isolation structure is effectively used as the high voltage semiconductor device and the semiconductor device for analog switch.
The conventional SOI semiconductor device is disclosed in Japanese Patent Nos. 2896141 and 2878689.
Each of
FIGS. 1 and 2
shows the structure of an n-type high voltage MOS (Metal Oxide Semiconductor) transistor as an example of the conventional SOI semiconductor device. An n-type high voltage MOS transistor
100
in
FIG. 1
is manufactured as follows. A silicon dioxide film
102
is formed on a main surface of a semiconductor substrate
101
, which is a supporting substrate of the SOI substrate. Then, an n
−
-type semiconductor layer
103
, which is to be the active layer of the SOI substrate, overlies the silicon dioxide film
102
. An isolation trench
104
extending to the silicon dioxide film
102
is formed on the n
−
-type semiconductor layer
103
by etching so as not to be affected by the potentials of the adjacent semiconductor elements. On the side walls of the isolation trench
104
, silicon dioxide films
105
are formed. The isolation trench
104
is filled with polysilicon
106
. As a result, the n
−
-type semiconductor layer
103
is electrically isolated from the other semiconductor island. More specifically, the n
−
-type semiconductor layer
103
is an island dielectrically isolated by the silicon dioxide films
102
and
105
.
On the surface of the island n
−
-type semiconductor layer
103
, gate oxide films
107
, gate electrodes
108
, a p-type semiconductor layer
109
, a source electrode
112
, n
+
-type semiconductor layers
110
and
111
, and drain electrodes
113
are formed to form the n-type high voltage MOS transistor
100
. The p-type semiconductor layer
109
is formed to form a channel region. The n
+
-type semiconductor layers
110
are connected to the source electrode
112
and surrounded by the p-type semiconductor layer
109
. The n
+
-type semiconductor layers
111
are connected to the drain electrodes
113
.
An n-type high voltage MOS transistor
150
in
FIG. 2
has almost the same structure as the n-type high voltage MOS transistor
100
in FIG.
1
. The n-type high voltage MOS transistor
150
is different from the n-type high voltage MOS transistor
100
in forming an n
−
-type semiconductor layer
114
between the n
−
-type semiconductor layer
103
and the silicon dioxide film
102
and forming an n
+
-type semiconductor layer
115
between the n
−
-type semiconductor layer
103
and the silicon dioxide film
105
so as to connect to the bottom of the n
+
-type semiconductor layers
111
. Here, the impurity concentration is set as relatively low in the n
−
-type semiconductor layer
114
and the n
+
-type semiconductor layer
115
. By doing so, a depletion layer is also formed around the n
−
-type semiconductor layer
114
and the n
+
-type semiconductor layer
115
in the n
−
-type semiconductor layer
103
so as to improve the operating.
Generally speaking, a voltage of 0V is applied to a semiconductor substrate
101
in the n-type high voltage MOS transistors
100
and
150
in
FIGS. 1 and 2
. When the potential of the p-type semiconductor layer
109
is almost the same as the potential of the semiconductor substrate
101
, and a large and positive voltage is applied to the n
+
-type semiconductor layers
111
, a pn junction diode consisting of the p-type semiconductor layer
109
and the n
−
-type semiconductor layer
103
is in a reverse bias state. In this case, a depletion layer extends from the interface between the p-type semiconductor layer
109
and the n
−
-type semiconductor layer
103
. Due to the large and positive voltage applied to the n
+
-type semiconductor layers
111
, the voltage of 0V applied to the semiconductor substrate
101
, and the voltage applied to the p-type semiconductor layer
109
, the depletion layer evenly extends in the n
−
-type semiconductor layer
103
to reduce the internal electric field.
As a result, avalanche breakdown hardly occurs in the n
−
-type semiconductor layer
103
. The operating voltage of the n-type high voltage MOS transistor depends on the occurrence of the avalanche breakdown in the n
−
-type semiconductor layer
103
. Accordingly, avalanche breakdown prevention can improve the operating voltage in the reverse bias state.
In the conventional SOI semiconductor device, however, especially, when the potential of the n
+
-type semiconductor layers
111
that are connected to the drain electrodes
113
is almost the same as the potential of the semiconductor substrate
101
as the supporting substrate of the SOI substrate, a depletion layer is not sufficiently formed in the n
−
-type semiconductor layer
103
. As a result, the operating voltage in the reverse bias state, which mainly depends on the avalanche breakdown, conspicuously deteriorates.
More specifically, in the reverse bias state, in which a large and negative voltage is applied to the p-type semiconductor layer
109
, a general voltage of 0V is applied to the semiconductor substrate
101
, and a voltage of 0V is applied to the n
+
-type semiconductor layers
111
, the semiconductor substrate
101
and the n
+
-type semiconductor layers
111
are at the same potential. This adversely affects the extension of the depletion layer. As a result, the depletion layer extending from the pn junction interface of the between the p-type semiconductor layer
109
and the n
−
-type semiconductor layer
103
does not sufficiently extend to reach regions of the n
−
-type semiconductor layer
103
under the n
+
-type semiconductor layers
111
. Accordingly, the electric field strength arises in the n
−
-type semiconductor layer
103
and the avalanche breakdown tends to occur to drastically deteriorate the reverse bias voltage of the n-type MOS transistor.
As has been described, the operating voltage cannot be kept relatively high in any reverse bias state according to the conventional SOI semiconductor device structure. The avalanche breakdown tends to easily occur to deteriorate the operating voltage in a specific condition.
SUMMARY OF THE INVENTION
It is accordingly the object of the present invention to provide an SOI semiconductor device with relatively high operating voltage in any reverse bias state.
The above-mentioned object may be achieved by an SOI semiconductor device including: a first semiconductor layer; a second semiconductor layer that is formed on a first part of a first main surface of the first semiconductor layer; a third semiconductor layer with a conductivity type different from a conductivity type of the second semiconductor layer, the third semiconductor layer being formed on a second part of the first main surface of the first semiconductor layer, the second part being separated from the first part; a fourth semiconductor layer with a conductivity type different from a conductivity type of the first semiconductor layer, he fourth semiconductor layer being formed on
Miura Takashi
Uemoto Yasuhiro
Yamashita Katsushige
Fahmy Wael
Ha Nathau W.
Matsushita Electric-Industrial Co., Ltd.
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