Power semiconductor device

Active solid-state devices (e.g. – transistors – solid-state diode – Regenerative type switching device – Combined with field effect transistor

Reexamination Certificate

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C257S137000, C257S154000, C257S165000

Reexamination Certificate

active

06809349

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a power semiconductor device, and particularly to an insulated gate semiconductor device favorably used as a power switching element.
2. Description of the Related Art
In recent years, power supply devices used in the power electronics field are strongly required to be more compact with higher performance. In accordance with this demand, power semiconductor devices have been improved to operate with lower loss and fewer noises, as well as higher breakdown voltage and larger electric current. Under the circumstances, an IEGT (Injection Enhanced Gate Transistor) obtained by improving an IGBT (Insulated Gate Bipolar Transistor) is attracting attention as a device, which can reduce the turn-off loss, as well as reducing the on-state voltage (for example, Jpn. Pat. Appln. KOKAI Publication No. 5-24356; Jpn. J. Appl. Phys. Vol. 36 (1997) pp. 3433-3437, ISSCC 2000 Digest Paper TA7.2; and M. Kitagawa et al., “A 4500V Injection Enhanced Insulated Gate Bipolar Transistor (IEGT) in a Mode Similar to a Thyristor”, IEDM '93, pp. 679-682, 1993).
FIG. 25
is a sectional view showing a conventional IEGT having a trench structure. As shown in
FIG. 25
, on one side of an n-base layer
101
, an n-buffer layer
102
is disposed, and a p-collector layer
103
is further disposed thereon. On the other side of the n-base layer
101
, a plurality of trenches
104
are formed at intervals in the n-base layer
101
, such that main cells MR and dummy cells DR are alternately partitioned.
In each of the main cells MR, a p-base layer
107
is disposed on the n-base layer
101
. N-emitter layers
108
are formed in the surface of the p-base layer
107
. In each of the dummy cells DR, a p-buffer layer
109
is disposed on the n-base layer
101
. Dividing a common p-layer by the trenches
104
forms the p-base layers
107
and p-buffer layers
109
.
A collector electrode
111
is disposed on the p-collector layer
103
. An emitter electrode
112
is disposed on the p-base layer
107
and n-emitter layers
108
. A gate electrode
106
is buried in each of the trenches
104
, while it is wrapped in a gate insulating film
105
. As a consequence, an n-channel MOSFET is formed in the main cell MR, such that it selectively connects the n-emitter layer
108
to the n-base layer
101
, using the p-base layer
107
as a channel region, to inject electrons.
In the sectional view shown in
FIG. 25
, the surface of the p-buffer layer
109
in each of the dummy cells DR is covered with an insulating film
110
. However, in order to fix the potential of the p-buffer layer
109
, a part of the emitter electrode
112
is also disposed on the p-buffer layer
109
at a position not shown in FIG.
25
. The density of the part of the emitter electrode
112
disposed on the p-buffer layer
109
is small, so that the resistance between the p-buffer layer
109
and emitter electrode
112
is equivalently large.
In this IEGT, each of the main cells MR forms a narrow current passage connecting the n-base layer
101
to the emitter electrode.
112
. In the on-state of the IEGT, this arrangement provides an increase in resistance against the flow of holes from the n-base layer
101
into the emitter electrode
112
through the p-base layer
107
in the main cell MR, thereby restricting the holes being exhausted into the emitter electrode
112
. As a consequence, the injection efficiency of electrons from the n-emitter layers
108
into the n-base layer
101
improves, thereby promoting conductivity modulation of the n-base layer
101
, resulting in a low on-state voltage.
A CSTBT (Carrier Stored Trench-Gate Bipolar Transistor) has also been proposed as a power semiconductor device, which can reduce the on-resistance as in the IEGT (for example, H. Takahashi et al., “Carrier Stored Trench-Gate Bipolar Transistor (CSTBT)—A Novel Power Device for High Voltage Application” ISPSD '96, pp. 349-352, 1996).
FIG. 26
is a sectional view showing a conventional CSTBT.
As shown in
FIG. 26
, on one side of an n-base layer
131
, a p-collector layer
133
is disposed. On the other side of the n-base layer
131
, an n-barrier layer
132
having an impurity concentration higher than that of the n-base layer
131
is disposed. A p-base layer
137
is disposed on the n-barrier layer
132
. N-emitter layers
138
are formed in the surface of the p-base layer
137
. A plurality of trenches
134
are formed at intervals such that they extend from the substrate surface into the n-base layer
131
.
A collector electrode
141
is disposed on the p-collector layer
133
. An emitter electrode
142
is disposed on the p-base layer
137
and n-emitter layers
138
. A gate electrode
136
is buried in each of the trenches
134
, while it is wrapped in a gate insulating film
135
. As a consequence, an n-channel MOSFET is formed such that it selectively connects the n-emitter layer
138
to the n-base layer
131
, using the p-base layer
137
as a channel region, to inject electrons.
In this CSTBT, the n-barrier layer
132
having a high impurity concentration provides a large resistance against flow of holes. In the on-state of the CSTBT, this arrangement provides an increase in resistance against the flow of holes from the n-base layer
131
into the emitter electrode
142
through the p-base layer
137
, thereby restricting the holes being exhausted into the emitter electrode
142
. As a consequence, the injection efficiency of electrons from the n-emitter layers
138
into the n-base layer
131
improves, thereby promoting conductivity modulation of the n-base layer
131
, resulting in a low on-state voltage.
The conventional IEGT and CSTB, used as power semiconductor devices, have the advantage of providing a low on-state voltage. However, these conventional power semiconductor devices have a problem causing a large noise in switching, and especially being turned on, as described above. In addition, since the resistance against holes being exhausted is high, a problem arises in that a period of time (storage period) for a depletion layer to extend up from the start of voltage rising is prolonged when the devices are turned off. This increases the turn-off loss, as well as the turn-off time.
BRIEF SUMMARY OF THE INVENTION
According to a first aspect of the present invention, there is provided a power semiconductor device comprising:
a first base layer of a first conductivity type;
a collector layer of a second conductivity type disposed on the first base layer;
a plurality of trenches disposed in the first base layer at intervals to partition a main cell and a dummy cell, at a position remote from the collector layer;
a second base layer of the second conductivity type disposed on the first base layer in the main cell;
an emitter layer of the first conductivity type disposed on the second base layer;
a buffer layer of the second conductivity type disposed on the first base layer in the dummy cell;
a gate electrode disposed in a trench of the plurality of trenches, adjacent to the main cell, to face, through a gate insulating film, a portion of the second base layer sandwiched between the first base layer and the emitter layer;
a collector electrode disposed on the collector layer;
an emitter electrode disposed on the second base layer and the emitter layer; and
a buffer resistor inserted between the buffer layer and the emitter electrode,
wherein the main cell forms a current passage narrow enough to provide, in an on-state of the device, an increase in resistance against flow of carriers of the second conductivity type from the first base layer into the emitter electrode through the second base layer, thereby improving injection efficiency of carriers of the first conductivity type from the emitter layer into the first base layer, and
the buffer resistor has a resistance value smaller than that with which gate-emitter voltage is increased by gate negative capacity, in a period of time for an applied voltage between gate and emitter to charge capacity between

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