This application is based upon and claims the benefit of priority from Japanese patent application No. 2016-249360, filed on Dec. 22, 2016, the disclosure of which is incorporated herein in its entirety by reference.
The present invention relates to a trench gate IGBT.
Japanese Unexamined Patent Application Publication No. 2013-140885 discloses a trench gate IGBT (Insulated Gate Bipolar Transistor). An IGBT illustrated in
There is a demand for further improving the performance of such a trench gate IGBT.
Other problems to be solved by and novel features of the present invention will become apparent from the following description and the accompanying drawings.
According to one embodiment, a trench gate IGBT includes two floating layers, two emitter trenches disposed between the two floating layers so as to be in contact with the floating layers, and at least two gate trenches disposed between the two emitter trenches.
According to the one embodiment, it is possible to provide a high-performance trench gate IGBT.
The above and other aspects, advantages and features will be more apparent from the following description of certain embodiments taken in conjunction with the accompanying drawings, in which:
The following description and drawings are omitted and simplified as appropriate for clarification of the explanation. The same elements are denoted by the same reference numerals throughout the drawings, and repeated explanations are omitted as necessary.
First, a trench gate IGBT (Insulated Gate Bipolar Transistor) disclosed in Japanese Unexamined Patent Application Publication No. 2013-140885 will be described. The trench gate IGBT (hereinafter also referred to simply as IGBT) disclosed in Japanese Unexamined Patent Application Publication No. 2013-140885 includes a P-type floating region (also referred to as a floating P-type layer; hereinafter referred to as an FLP layer). A collector-emitter voltage Vce (sat) can be reduced by enhancing a carrier storage effect.
Further, an IGBT shown in
In the trench gate IGBT disclosed in Japanese Unexamined Patent Application Publication No. 2013-140885, the collector-emitter voltage Vce (sat) can be reduced and the switch characteristics can be improved. Note that the FLP layer is deeper than the trenches. This is intended to relax the electric field at a bottom end of each trench, to thereby improve a robustness BVces. Since the FLP layer is shallow, if the width of the FLP layer is wide, the robustness BVces decreases. To be more specific, it is important to reduce the feedback capacitance Cres with respect to an input capacitance Cies.
In the trench gate IGBT shown in
The trench gate IGBT according to this embodiment has been devised to accomplish both an improvement in characteristics and an improvement in noise resistance and ESD tolerance. The trench gate IGBT according to this embodiment is especially effective for a small current application. As for the basic configuration of the trench gate IGBT according to this embodiment and a manufacturing method thereof, see the contents disclosed in Japanese Unexamined Patent Application Publication No. 2013-140885, as necessary.
First Embodiment
A trench gate IGBT according to a first embodiment will be described with reference to
The IGBT 1 includes a semiconductor substrate 11, floating P-type layers (hereinafter referred to as FLP layers) 12, emitter trenches 13, gate trenches 14, channel layers 15, an insulating film 17, an emitter electrode 18, source diffusion layers 19, contacts 21, a gate electrode 31, a P-type well 32, and contacts 36.
The semiconductor substrate 11 is, for example, a silicon single crystal wafer and is used as an N-type substrate in which an impurity such as phosphorus (P) is introduced. On the semiconductor substrate 11, the FLP layers 12, the emitter trenches 13, the gate trenches 14, and the channel layers 15 are formed. Above the semiconductor substrate 11, the insulating film 17 and the emitter electrode 18 are formed. Although not shown, the back surface of the semiconductor substrate 11 serves as a p-type collector.
Each FLP layer 12 is a P-type well in which an impurity such as boron is introduced. The potential of the FLP layer 12 is floating. As shown in
As shown in
In the XY plan view shown in
Further, as shown in
Each polysilicon electrode 35 is connected to the emitter trenches 13 so as to obtain an emitter potential. Each polysilicon electrode 35 is formed of, for example, a polysilicon film. The contact 36 is formed on the polysilicon electrode 35. Each contact 36 is in contact with the corresponding polysilicon electrode 35. Accordingly, each contact 36 is connected to the emitter trenches 13 through the corresponding polysilicon electrode 35. The emitter trenches 13 are each connected to the emitter potential through the corresponding contact 36.
As shown in
As shown in
Further, at an end in the +Y-direction of each gate trench 14, two gate trenches 14 are connected through a gate trench 14a. The gate trenches 14 are supplied with a gate potential through the gate electrode 31. The gate electrode 31 is formed of, for example, the polysilicon film with which each polysilicon electrode 35 is formed. The gate electrode 31 is formed on the P-type well 32.
Note that the gate trenches 14 each include, for example, a gate oxide film formed on an inner surface the trench, and a silicon film buried in the trench. Each emitter trench 13 can be formed by a process similar to that for forming the gate trenches 14.
Further, as shown in
The insulating film 17 is formed above the semiconductor substrate 11. The insulating film 17 is, for example, a silicon oxide film. The emitter electrode 18 is formed on the insulating film 17. The emitter electrode 18 can be formed of the polysilicon film with which each polysilicon electrode 35 is formed. The insulating film 17 includes the contacts 21. The emitter electrode 18 is buried in each contact 21. Specifically, the emitter electrode 18 is connected to the channel layers 15 through each contact 21 which is formed in the insulating film 17. Like in the XY plane vies shown in
Further, the source diffusion layers 19 of an FET (Field Effect Transistor) are formed between the two gate trenches 14. The source diffusion layers 19 are each formed on the surface of each channel layer 15 of the semiconductor substrate 11. The source diffusion layers 19 are each in contact with the gate trenches 14. Each source diffusion layer 19 is an N+-type emitter diffusion layer, and is connected to the emitter potential through each contact 21.
In this manner, two gate trenches 14 are disposed between the two emitter trenches 13. The IGBT 1 has a structure (hereinafter referred to as an EGGE structure) in which the emitter trench 13, the gate trench 14, the gate trench 14, and the emitter trench 13 are disposed in this order between two adjacent FLP layers 12 in the X-direction. In the EGGE structure, two emitter trenches 13 are disposed between two FLP layers 12, and at least two gate trenches 14 are disposed between two emitter trenches 13.
By the EGGE structure, the occupancy of the gate trenches 14 can be increased while the advantages of the EGE structure are maintained. Accordingly, the input capacitance Cies can be increased. This leads to an improvement in noise tolerance and ESD tolerance. This is more effective in the application of, for example, a low current with a small chip size. In particular, the IGBT 1 is suitable for an inverter for a small current application.
The number of the gate trenches 14 disposed between the two emitter trenches 13 is not limited to two, but instead three or more gate trenches 14 may be disposed between the two emitter trenches 13. In the EGGE structure, a plurality of gate trenches 14 are disposed, which provides controllability for a capacitance value and a current density. By the floating structure, the collector-emitter voltage Vce (sat) can be reduced. Each emitter trench 13 prevent the FLP layers 12 from coming into contact with the gate trenches 14. In other words, each emitter trench 13 is interposed between the gate trench 14 and the FLP layer 12. Accordingly, flexibility of design can be obtained while the effect of reducing the feedback capacitance Cres is maintained.
First Modified Example
A trench gate IGBT 1a according to a first modified example of the first embodiment (hereinafter simply referred to as the IGBT 1a) will be described with reference to
The IGBT 1a further includes the source diffusion layers 19 that are each disposed between the emitter trench 13 and the gate trench 14. In the IGBT 1a, the source diffusion layers 19 are provided not only in the region between the two gate trenches 14, but also in the regions between the gate trench 14 and the emitter trench 13. Specifically, the source diffusion layers 19 are formed on the surface of each of the channel layers 15a and 15. In the X-direction, the source diffusion layers 19 are disposed on both sides of one gate trench 14. With this configuration, the source density can be increased and a larger current can be caused to flow. The components other than the source diffusion layer 19 provided between the gate trench 14 and the emitter trench 13 are similar to those of the first embodiment, and thus descriptions thereof are omitted.
In the configuration shown in
The size of each source diffusion layer 19 may be adjusted depending on a current to be caused to flow. For example, the current can be increased by increasing the area of each source diffusion layer 19, and the current can be decreased by reducing the area of each source diffusion layer 19. A short-circuit current that flows when a load is short-circuited can be decreased by reducing the size of each source diffusion layer 19. A short-circuit tolerance can be adjusted depending on the size of each source diffusion layer 19.
Second Embodiment
A trench gate IGBT 2 according to a second embodiment (hereinafter simply referred to as the IGBT 2) will be described with reference to
The arrangement of the contacts 21 formed in the insulating film 17 in the second embodiment is different from that in the first embodiment. The basic configuration of the IGBT 2 according to the second embodiment is similar to that of the IGBT 1 according to the first embodiment, except for the arrangement of the contacts 21, and thus the description thereof is omitted.
In the second embodiment, the contacts 21 are not formed on the channel layers 15a and 15b. In other words, the channel layers 15a and 15b are each covered with the insulating film 17. Accordingly, the channel layers 15a and 15b that are each disposed between the emitter trench 13 and the gate trench 14 are floating.
The configuration in which the channel layers 15a and 15b are floating prevents stored carriers (holes) from being absorbed in the contacts. Consequently, the storage effect is enhanced and the collector-emitter voltage Vce (sat) and be reduced.
Third Embodiment
An IGBT 3 according to a third embodiment will be described with reference to
Like
The contact 21a extends from an upper part of the emitter trench 13 to an upper part of the channel layer 15a. In other words, the contact 21a straddles the boundary between the emitter trench 13 and the channel layer 15a. The contact 21b extends from an upper part of the emitter trench 13 to an upper part of the channel layer 15b. In other words, the contact 21a straddles the boundary between the emitter trench 13 and the channel layer 15a.
With this configuration, the distance of an invalid region from the emitter trench 13 to the gate trench can be reduced. Accordingly, the invalid region can be shrunk and the area thereof can be reduced.
For example, in the semiconductor devices according to the embodiments described above, the conductivity type (p-type or n-type) of the semiconductor substrate, a semiconductor layer, a diffusion layer (diffusion region), and the like may be reversed. Accordingly, when one of the conductivity types of the n-type and the p-type is defined as a first conductivity type and the other conductivity type is defined as a second conductivity type, the first conductivity type may be the p-type and the second conductivity type may be the n-type. On the contrary, the first conductivity type may be the n-type and the second conductivity type may be the p-type.
While the invention made by the present inventors has been described in detail above with reference to embodiments, the present invention is not limited to the embodiments described above and can be modified in various ways without departing from the scope of the invention.
While the invention has been described in terms of several embodiments, those skilled in the art will recognize that the invention can be practiced with various modifications within the spirit and scope of the appended claims and the invention is not limited to the examples described above.
Further, the scope of the claims is not limited by the embodiments described above.
Furthermore, it is noted that, Applicant's intent is to encompass equivalents of all claim elements, even if amended later during prosecution.
Number | Date | Country | Kind |
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2016-249360 | Dec 2016 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
9653587 | Matsuura | May 2017 | B2 |
20040084722 | Yamaguchi et al. | May 2004 | A1 |
20090283797 | Takahashi et al. | Nov 2009 | A1 |
20110233684 | Matsushita | Sep 2011 | A1 |
Number | Date | Country |
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2 942 816 | Nov 2015 | EP |
2013-140885 | Jul 2013 | JP |
Entry |
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Extended European Search Report dated Apr. 25, 2018 in European Application No. 17200776.7. |
Number | Date | Country | |
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20180182875 A1 | Jun 2018 | US |