Method of forming power semiconductor devices having...

Semiconductor device manufacturing: process – Making regenerative-type switching device – Having structure increasing breakdown voltage

Reexamination Certificate

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C438S454000

Reexamination Certificate

active

06190948

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to semiconductor devices and fabrication methods, and more particularly to power semiconductor devices and methods of fabricating same.
BACKGROUND OF THE INVENTION
The breakdown characteristics of parallel-plane (semi-infinite) junctions typically provide an upper bound on the breakdown characteristics of power semiconductor devices. This is because the breakdown voltages of practical power devices having finite length P-N junctions are typically limited by the occurrence of high electric fields either within interior portions of the devices or at the edges of the devices.
Although many specific edge termination techniques have been proposed in the literature to improve breakdown voltage, these techniques can generally be classified into two basic types, namely, planar terminations based upon masked diffusion processes and beveled terminations based upon the selective removal of material from the vicinity of the edge junctions. In both these techniques, floating field plates and floating field rings have been found to be useful in enhancing the breakdown voltage of power semiconductor devices. Such conventional techniques are more fully described in Section 3.6 of a textbook by B. J. Baliga entitled
Power Semiconductor Devices,
PWS Publishing Co. (1995), pp. 81-113.
Typical power semiconductor devices include the insulated gate bipolar transistor (IGBT) and static-induction transistor (SIT).
FIG. 1
illustrates a schematic cross-sectional view of a conventional insulated gate bipolar transistor containing an N+ buffer region
13
on a P+ substrate
12
having an anode electrode
11
on a face thereof. An N− drift region
14
is also provided on the buffer region
13
. Adjacent P-type base regions
15
are also provided in the drift region
14
by implanting and then diffusing P-type dopants into an upper surface of the drift region
14
using an insulated gate electrode, comprising an insulating layer
18
and gate electrode
19
, as an implant mask. N-type source regions
16
are also provided in the P-type base regions
15
. Contact to the base and source regions is provided by a cathode contact
17
on the upper surface of the drift region
14
. As will be understood by those skilled in the art, the P-type substrate
12
, the N-type buffer and drift regions
13
-
14
, and P-type base region
15
collectively form the emitter, base and collector of a vertical P-N-P bipolar transistor having a floating base. In order to turn the vertical P-N-P bipolar transistor on, the anode electrode
11
is biased positive relative to the cathode electrode
17
and a positive bias is applied to the gate electrode
19
. The application of a positive bias to the gate electrode
19
causes the formation of inversion-layer channels in the base regions
15
. These inversion-layer channels electrically connect the source regions
16
to the drift region
14
and provide the base drive current needed to initiate turn-on of the P-N-P transistor.
FIG. 2
illustrates a schematic cross-sectional view of a static induction transistor comprising a drain electrode
21
, P+ substrate region
22
, N+ buffer region
23
, N− drift region
24
, P+ gate regions 25, N+ source region
26
and source electrode
27
. The source electrode
27
may be electrically isolated from the gate regions
25
by an electrically insulating region
28
. As will be understood by those skilled in the art, forward conduction can be controlled by controlling the magnitude of the reverse bias appearing across the P-N junctions formed between the gate regions
25
and drift region
24
. When this reverse bias is substantial, the depletion regions formed in the drift region
24
merge to pinch-off the conductive channel formed in the space between the gate regions
25
and thereby prevent forward conduction. Thus, the resistance of the channel region can be modulated by the magnitude of the reverse bias appearing across the gate region/drift region junctions.
Unfortunately, both of the above described power semiconductor devices are susceptible to premature breakdown because the base regions
15
of FIG.
1
and gate regions
25
of
FIG. 2
do not form semi-infinite parallel-plane P-N junctions with the drift regions
14
and
24
, respectively. This premature breakdown is caused by electric field crowding at the curved edges of the base and gate regions. Moreover, the degree of field crowding is worse when the junction depths are small compared to the depletion layer thickness in the drift region.
As described above, in order to enhance the breakdown voltages of power semiconductor devices, several types of structures have been developed. Two well known structures can be made by a simplified fabrication method. One of these structures is a floating field ring
48
which is spaced apart from a main junction region
46
in a substrate region
44
, as illustrated by FIG.
3
. An insulating region
49
may also be provided on a face of the substrate. The other of these structures is a field plate
58
which is connected to a main junction
56
at the face of a substrate
54
and is spaced from the face by an electrically insulating region
59
, as illustrated by FIG.
4
. Referring again to
FIG. 3
, a depletion layer
45
indicated by a dotted line may be generated and extended from the main junction region
46
to an outer edge of the floating field ring
48
when the main junction region is reverse biased. This prevents electric field crowding in the region “W
S
” which designates the spacing between the main junction region
46
and the floating field ring
48
. As a result, the device of
FIG. 3
may be able to support a breakdown voltage in a range of about 60-80% of the ideal breakdown voltage of a parallel-plane junction. Referring again to
FIG. 4
, a depletion layer
55
indicated by a dotted line may be generated in the substrate
54
because of the presence of the field plate
58
. As a result, the device of
FIG. 4
may be able to support a breakdown voltage in a range of about 60% of the ideal breakdown voltage of a parallel-plane junction. To enhance the breakdown voltage of the structure of
FIG. 4
, an insulating layer
59
(e.g., SiO
2
) may be provided, as illustrated. As will be understood by those skilled in the art, if the insulating layer
59
is thick, breakdown will typically occur in region “A”, however if the insulating layer
59
is thin then breakdown will typically occur in region “B”.
Notwithstanding these above described attempts to increase the breakdown voltage ratings of power semiconductor devices to the near ideal levels associated with parallel-plane junctions, there still continues to be need for structures which can improve the breakdown voltage ratings of power devices even further.
SUMMARY OF THE INVENTION
It is therefore an object of the present invention to provide improved power semiconductor devices and methods of forming same.
It is another object of the present invention to provide power semiconductor devices having high breakdown voltages and methods of forming same.
These and other objects, features and advantages of the present invention are provided by power semiconductor devices having overlapping floating field plates for improving the breakdown characteristics of active regions therein and methods of forming same. In particular, a primary field plate and a plurality of floating field plates are formed on an electrically insulating region and are capacitively coupled together in series between an active region of a power semiconductor device and a floating field ring. Preferably, the capacitive coupling is achieved by overlapping at least portions of the floating field plates. According to one embodiment of the present invention, a power semiconductor device comprises a semiconductor substrate having a first region of first conductivity type therein extending to a face of the substrate and a second region of second conductivity type in the first region of first conductivity type and fo

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