Semiconductor device and method for manufacturing the same

Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode

Reexamination Certificate

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C257S331000, C257S347000

Reexamination Certificate

active

06198130

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a semiconductor device suitable for an IGBT (Insulated Gate Bipolar Transistor), and more particularly to an improvement to reduce an ON-state voltage.
2. Description of the Background Art
FIG. 70
is a sectional front view showing a structure of a semiconductor device according to the prior art which is a background of the present invention.
FIG. 71
is a sectional view taken along the line K—K in FIG.
70
. An device
150
according to the prior art comprises a SOI (Silicon On Insulator) wafer. The SOI wafer includes a silicon substrate
151
, a silicon oxide film (a substrate insulation film)
152
formed on the silicon substrate
151
, and an n

-type silicon layer (an active layer or a SOI layer)
153
formed on the silicon oxide film
152
.
A p-type base layer
154
and an n-type buffer layer
156
are selectively formed apart from each other over an upper principal surface of the n

-type silicon layer
153
. An n
+
-type emitter layer
155
is selectively formed on an upper principal surface of the p-type base layer
154
. A p
+
-type collector layer
157
is selectively formed on an upper principal surface of the n-type buffer layer
156
.
An emitter electrode
170
is connected across an upper principal surface of the n
+
-type emitter layer
155
and that of the p-type base layer
154
. A collector electrode
171
is connected to an upper principal surface of the p
+
-type collector layer
157
. A gate electrode
173
is provided opposite to the upper principal surface of the p-type base layer
154
with a gate insulation film (not shown) interposed therebetween. In other words, the device
150
comprises a “transverse (or lateral)” and n-channel type IGBT.
An isolation trench
161
is formed around the IGBT. An isolation electrode
163
is buried in the isolation trench
161
with an isolation insulation film
162
interposed therebetween. A circuit element which is not shown is formed in a region of the n

-type silicon layer
153
provided opposite to the IGBT with the isolation trench
161
interposed therebetween. The circuit element is an device portion for controlling the IGBT, for example. Differently from the IGBT acting as a power element, only a current having a small magnitude flows in the circuit element. The isolation trench
161
is provided in order to isolate the IGBT in which a current having a great magnitude flows from the circuit element which operates with the current having a small magnitude.
In recent years, a dielectric isolation type HVIC (High Voltage Integrated Circuit) having high-speed switching characteristics and less parasitic bipolar operation has vigorously been developed as a transverse type power device. The device
150
corresponds to an example in which a dielectric isolation is implemented by a SOI wafer and a trench isolation (the isolation trench
161
).
When using the device
150
, a positive voltage for the emitter electrode
170
is usually applied to the collector electrode
171
through a load. In this state, if a positive voltage which exceeds a predetermined threshold voltage is applied to the gate electrode
173
, a channel region Ch defined in a surface portion of the p-type base layer
154
opposite to the gate electrode
173
becomes conductive so that electrons are injected from the n
+
-type emitter layer
155
to the n

-type silicon layer
153
.
More specifically, an electronic current Jn flows from the n
+
-type emitter layer
155
to the n

-type silicon layer
153
(In the drawing, a direction of the electronic current Jn represents that of a flow of a positive electric charge). Accordingly, a hole is injected from the p
+
-type collector layer
157
to the n

-type silicon layer
153
. As a result, conductivity modulation is caused so that an electric resistance is lowered in the n

-type silicon layer
153
. Therefore, a main current (collector current) is caused to flow from the collector electrode
171
to the emitter electrode
170
. More specifically, the IGBT is brought into a conductive state (an ON state).
When a zero voltage or a negative voltage is applied to the gate electrode
173
, the channel region Ch becomes non-conductive so that the injection of the electrons from the n
+
-type emitter layer
155
to the n

-type silicon layer
153
is stopped. As a result, the conductivity modulation in the n

-type silicon layer
153
dissipates. Consequently, the flow of the main current is stopped. In other words, the IGBT is brought into a cut-off state (an OFF state). In the IGBT described above, a magnitude of the main current is controlled according to a voltage applied to the gate electrode
173
.
As an example, the IGBT provided in the device
150
according to the prior art shown in
FIGS. 70 and 71
will be described below. In the IGBT, a voltage drop is caused in the vicinity of the channel region Ch in the ON state so that a voltage drop is great between the collector electrode
171
and the emitter electrode
170
in the ON state, that is, an ON-state voltage is high. Furthermore, a hole current Jh passes through a transverse resistor (or lateral resistor) R of the p-type base layer
154
. Therefore, a latch-up tolerance is low.
Such troubles are more or less caused in a MOS transistor as well as the IGBT, and are outstanding problems to be solved in semiconductor device represented by these elements (IGBT and MOS).
SUMMARY OF THE INVENTION
A first aspect of the present invention is directed to a semiconductor device comprising a first semiconductor layer of a first conductivity type having one of principal surfaces and the other principal surface, a second semiconductor layer of a second conductivity type which is selectively formed on one of the principal surfaces of the first semiconductor layer, a third semiconductor layer of a first conductivity type selectively formed on an inside of an exposed surface of the second semiconductor layer, wherein the third semiconductor layer is shallower than the second semiconductor layer and has a higher impurity concentration than that of the first semiconductor layer, a fourth semiconductor layer which is selectively exposed to one of the principal surfaces of the first semiconductor layer apart from the second semiconductor layer, a first main electrode connected to the second and third semiconductor layers, and a second main electrode connected to the fourth semiconductor layer.
The first semiconductor layer defines a gate trench which is open to one of the principal surfaces, the gate trench being defined to extend in a direction from the third semiconductor layer toward the second main electrode, and to traverse at least from an edge of the third semiconductor layer which is closer to the second main electrode to an edge of the second semiconductor layer which is closer to the second main electrode, the semiconductor device further comprising a gate insulation film covering an internal wall of the gate trench which is defined by the first semiconductor layer, and a gate electrode buried in the gate trench with the gate insulation film interposed therebetween.
A second aspect of the present invention is directed to the semiconductor device according to the first aspect of the present invention, wherein the gate trench is divided into lines of unit gate trenches arranged at regular intervals, and a connecting portion of the first main electrode and the second and third semiconductor layers is divided into a plurality of regions interposed between the lines of the unit gate trenches.
A third aspect of the present invention is directed to the semiconductor device according to the second aspect of the present invention, wherein the fourth semiconductor layer is a semiconductor layer of a second conductivity type, and the connecting portion is provided thinly in a part of the regions.
A fourth aspect of the present invention is directed to the semiconductor devi

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